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OptimizationProbabilityStatistics·Captain: mikedeng1

Distributionally Robust Optimization: A Review: Variation²/4 ≤ Hellinger ≤ Kullback–Leibler ≤ J-Divergence, so the J, KL and Hellinger Balls of Radius ε Lie in the Variation Ball of Radius 2√εResearch Paper

Motivation

Distributionally robust optimization evaluates a decision against a set of plausible probability laws rather than against a single estimated law. A common way to specify that set is to choose a nominal law P0P_0P0​ and allow every law PPP whose discrepancy from P0P_0P0​ is below a radius ε\varepsilonε. Different discrepancies produce different ambiguity sets, so comparing them tells a modeler what one constraint guarantees about another. Rahimian and Mehrotra collect such constructions in their survey and state a chain of comparisons among variation, Hellinger, Kullback–Leibler, and J-divergences in Lemma 5.4 (arXiv:1908.05659v1, pp. 31, 34–35). The chain connects four common ways of controlling model error without requiring a finite outcome space or a common density chosen in advance.

The source is the 2019 arXiv v1 preprint of a survey. Its proof of Lemma 5.4 cites earlier work rather than giving a full derivation. The preprint also prints an additional J-to-χ2\chi^2χ2 comparison that is false; this mission isolates the part that holds for every pair of probability measures. The distinction matters when an ambiguity set is used to certify a bound under a different divergence: an inclusion based on the false link can certify laws that are outside the intended set.

Setting

Let (Ξ,F)(\Xi,\mathcal F)(Ξ,F) be a measurable space, and let M(Ξ,F)\mathfrak M(\Xi,\mathcal F)M(Ξ,F) be its probability measures. Given P1,P2∈M(Ξ,F)P_1,P_2\in\mathfrak M(\Xi,\mathcal F)P1​,P2​∈M(Ξ,F), a ϕ\phiϕ-divergence Dϕ(P1,P2)\mathfrak D^\phi(P_1,P_2)Dϕ(P1​,P2​) compares their densities using a function ϕ:[0,∞)→[0,∞]\phi:[0,\infty)\to[0,\infty]ϕ:[0,∞)→[0,∞] with ϕ(1)=0\phi(1)=0ϕ(1)=0. The paper assumes ϕ\phiϕ is convex. To account for measures that are not mutually absolutely continuous, take the common dominating measure ν=P1+P2\nu=P_1+P_2ν=P1​+P2​ and write p=dP1/dνp=dP_1/d\nup=dP1​/dν and q=dP2/dνq=dP_2/d\nuq=dP2​/dν. The integrand is qϕ(p/q)q\phi(p/q)qϕ(p/q) when q>0q>0q>0 and pϕ′(∞)p\phi'(\infty)pϕ′(∞) when q=0q=0q=0, where ϕ′(∞)=lim⁡t→∞ϕ(t)/t\phi'(\infty)=\lim_{t\to\infty}\phi(t)/tϕ′(∞)=limt→∞​ϕ(t)/t; a point with p=q=0p=q=0p=q=0 contributes zero (§5.1.2, p. 31).

Table 1 gives four generators used here:

ϕv(t)=∣t−1∣,ϕh(t)=(t−1)2,ϕkl(t)=tlog⁡t−t+1,ϕj(t)=(t−1)log⁡t.\phi_v(t)=|t-1|,\qquad \phi_h(t)=(\sqrt t-1)^2,\qquad \phi_{\mathrm{kl}}(t)=t\log t-t+1,\qquad \phi_j(t)=(t-1)\log t.ϕv​(t)=∣t−1∣,ϕh​(t)=(t​−1)2,ϕkl​(t)=tlogt−t+1,ϕj​(t)=(t−1)logt.

The first two divergences are the full L1L^1L1 variation discrepancy and the unhalved squared Hellinger discrepancy. In particular, Dϕv=2dTV\mathfrak D^{\phi_v}=2d_{\mathrm{TV}}Dϕv​=2dTV​, where dTVd_{\mathrm{TV}}dTV​ is the total variation distance defined later in the paper. The J generator has ϕj(0)=+∞\phi_j(0)=+\inftyϕj​(0)=+∞, understood as its limit at zero; ϕkl(0)=1\phi_{\mathrm{kl}}(0)=1ϕkl​(0)=1 under 0log⁡0=00\log0=00log0=0. The recession slopes of the four generators, in the displayed order, are 1,1,+∞,+∞1,1,+\infty,+\infty1,1,+∞,+∞ (Table 1, p. 31; §5.1.3, p. 35).

For a nominal probability measure P0P_0P0​ and a nonnegative radius ε\varepsilonε, equation (5.9) defines the ambiguity ball

Pϕ(P0;ε)={P∈M(Ξ,F):Dϕ(P,P0)≤ε}.\mathcal P^\phi(P_0;\varepsilon) =\{P\in\mathfrak M(\Xi,\mathcal F):\mathfrak D^\phi(P,P_0)\le\varepsilon\}.Pϕ(P0​;ε)={P∈M(Ξ,F):Dϕ(P,P0​)≤ε}.

Formalization targets

The three milestone comparisons are the valid initial part of (5.10), for every P,P0∈M(Ξ,F)P,P_0\in\mathfrak M(\Xi,\mathcal F)P,P0​∈M(Ξ,F):

14(Dϕv(P,P0))2≤Dϕh(P,P0)≤Dϕkl(P,P0)≤Dϕj(P,P0).\frac14\bigl(\mathfrak D^{\phi_v}(P,P_0)\bigr)^2 \le\mathfrak D^{\phi_h}(P,P_0) \le\mathfrak D^{\phi_{\mathrm{kl}}}(P,P_0) \le\mathfrak D^{\phi_j}(P,P_0).41​(Dϕv​(P,P0​))2≤Dϕh​(P,P0​)≤Dϕkl​(P,P0​)≤Dϕj​(P,P0​).

The middle comparison is also stated in footnote 18. The mission goal is the corrected Lemma 5.4: it joins these three comparisons to the resulting valid part of (5.11), for every nominal P0P_0P0​ and radius ε\varepsilonε:

Pϕj(P0;ε)⊆Pϕkl(P0;ε)⊆Pϕh(P0;ε)⊆Pϕv(P0;2ε).\mathcal P^{\phi_j}(P_0;\varepsilon) \subseteq\mathcal P^{\phi_{\mathrm{kl}}}(P_0;\varepsilon) \subseteq\mathcal P^{\phi_h}(P_0;\varepsilon) \subseteq\mathcal P^{\phi_v}(P_0;2\sqrt\varepsilon).Pϕj​(P0​;ε)⊆Pϕkl​(P0​;ε)⊆Pϕh​(P0​;ε)⊆Pϕv​(P0​;2ε​).

Each inclusion has the direction induced by the preceding divergence inequality: a stronger divergence constraint gives a smaller ball. The first comparison retains the paper's factor 1/41/41/4, and the final ball retains its radius 2ε2\sqrt\varepsilon2ε​ (Lemma 5.4, p. 34).

Significance

The result allows a J-divergence or KL-divergence ambiguity model to carry a simultaneous bound in Hellinger and full variation divergence. A Hellinger radius ε\varepsilonε yields the explicit variation radius 2ε2\sqrt\varepsilon2ε​; this makes the scale change visible when comparing two models built with different discrepancies. Without a general-measure statement, a finite-outcome approximation does not itself cover continuous laws or pairs with a singular component.

The paper presents the inequalities as known and cites sources for them. A finite-alphabet TV–Hellinger–KL chain and a general-measure KL–affinity bound already have machine-checked results in the platform catalog. The work here is to formalize the four generators with one shared general-measure divergence, close the remaining inequalities in that representation, and connect them to the ambiguity-ball inclusions. This also provides reusable definitions for other distributionally robust models that use the same divergence convention.

Difficulty

Writing the density ratio only with respect to P0P_0P0​ loses the part of PPP singular to P0P_0P0​. That would change both variation and Hellinger divergence and make the stated chain an unreliable comparison of the paper's objects. At the opposite boundary, PPP can vanish on a set that P0P_0P0​ charges. There the J generator must be infinite, although a direct use of a total real logarithm at zero can assign it an incorrect finite value. These two edge cases make an apparently routine pointwise comparison insufficient for the full measurable-space theorem.

Formalization scope

Lean represents PPP and P0P_0P0​ as ProbabilityMeasure Ξ on an arbitrary MeasurableSpace Ξ. It computes Radon–Nikodym densities relative to P+P0P+P_0P+P0​, evaluates the divergence with an extended nonnegative Lebesgue integral, and represents both divergence values and radii in ENNReal. The generic definition computes the recession slope as a limsup; for the four Table 1 generators this is the limit in the paper. The formal ambiguity ball contains probability measures only. A top radius is allowed by the type; the finite nonnegative radii are the paper's intended model parameters. The generic operation does not take a convexity certificate, but the four named generators are the only ones used in the theorem.

The formalization must not turn a nondominated pair into divergence zero or assign ϕj(0)=0\phi_j(0)=0ϕj​(0)=0: either choice changes the claimed chain. It must also retain the full variation divergence, without the half factor used for total variation distance. The definitions of the common-measure divergence, its four generators, and the ambiguity ball are intended for reuse. Contributions establishing properties of the recession slopes, comparison lemmas on arbitrary measurable spaces, and their ambiguity-set consequences are within scope.

The paper's final inequality in (5.10), Dϕj≤Dϕca2\mathfrak D^{\phi_j}\le\mathfrak D^{\phi_{\mathrm{ca}^2}}Dϕj​≤Dϕca2​, and the associated first inclusion in (5.11) are removed. They are false even on a two-point space: with P0=(1/2,1/2)P_0=(1/2,1/2)P0​=(1/2,1/2) and P=(0,1)P=(0,1)P=(0,1), J-divergence is +∞+\infty+∞ while the order-two χ\chiχ-divergence is 111. Thus PPP lies in the latter ball of radius 111 but outside the J ball of that radius. The source's footnote 18 separately notes an error in a cited Hellinger–KL comparison; the corrected Hellinger–KL inequality is retained (pp. 34–35).

Selected references

  • H. Rahimian and S. Mehrotra, Distributionally Robust Optimization: A Review, arXiv preprint arXiv:1908.05659v1, 2019. Preprint.
10 thms6 active usersReviewed
🏆Completed
Linear algebraQuantum Information·Captain: mikedeng1

Reversing quantum dynamics with near-optimal quantum and classical fidelity II: The Pretty Good Measurement Errs at Most the Weighted Sum of Bures–Uhlmann FidelitiesResearch Paper

Motivation

Quantum communication and computation often require a receiver to infer which preparation was sent after it has passed through a noisy quantum process. When possible preparations are mixed states, their overlap makes exact identification impossible. A measurement is then judged by its average probability of a correct label. The pretty good measurement gives a concrete measurement from the ensemble itself, without first solving the optimization over all measurements. Barnum and Knill related it to a general reversal operation for noisy dynamics and bounded its error through pairwise state fidelities in their preprint, §V–VI. The bound is useful when the overlaps are easier to estimate than the measurement's success probability.

The present mission addresses the preprint's second main result. The source is arXiv:quant-ph/0004088v2, not the later journal pagination. The preprint also strengthens its Theorem 3 relative to the published text, as its acknowledgment explains; this mission concerns Theorem 5 and the calculation around it.

Setting

An ensemble is a finite family of output density matrices ρ^j\hat\rho_jρ^​j​ with probabilities pj≥0p_j\geq0pj​≥0 satisfying ∑jpj=1\sum_jp_j=1∑j​pj​=1. A density matrix is a positive semidefinite complex matrix with trace one. For each label jjj, fix an orthonormal eigenbasis vijv_{ij}vij​ and nonnegative eigenvalues λij\lambda_{ij}λij​ such that

ρ^j=∑iλij∣vij⟩⟨vij∣,∑iλij=1.\hat\rho_j=\sum_i\lambda_{ij}|v_{ij}\rangle\langle v_{ij}|, \qquad \sum_i\lambda_{ij}=1.ρ^​j​=i∑​λij​∣vij​⟩⟨vij​∣,i∑​λij​=1.

The eigenpair index iii runs over a finite output basis OOO; zero eigenvalues are allowed. The input labels form a finite basis JJJ. A label distribution is represented by ρ=∑jpj∣j⟩⟨j∣\rho=\sum_jp_j|j\rangle\langle j|ρ=∑j​pj​∣j⟩⟨j∣.

The paper's classicizing channel AAA has Kraus operators Aij=λij∣vij⟩⟨j∣A_{ij}=\sqrt{\lambda_{ij}}|v_{ij}\rangle\langle j|Aij​=λij​​∣vij​⟩⟨j∣. Acting on an input matrix XXX, its value is A(X)=∑i,jAijXAij†A(X)=\sum_{i,j}A_{ij}X A_{ij}^{\dagger}A(X)=∑i,j​Aij​XAij†​. In particular, its output on ρ\rhoρ is ρout=∑jpjρ^j\rho_{\mathrm{out}}=\sum_jp_j\hat\rho_jρout​=∑j​pj​ρ^​j​. The paper assumes ρout\rho_{\mathrm{out}}ρout​ has full support when it writes its reversal operation. For a general Kraus family AaA_aAa​, that operation has operators

(RA,ρ)a=ρ1/2Aa†A(ρ)−1/2.(R_{A,\rho})_a=\rho^{1/2}A_a^\dagger A(\rho)^{-1/2}.(RA,ρ​)a​=ρ1/2Aa†​A(ρ)−1/2.

The inverse square root is spectral: invert nonzero eigenvalues and leave zero eigenvalues at zero. With full support, it is the usual inverse square root.

For an input label jjj, classical fidelity is the chance that the composite operation returns the same label. Averaging gives

Fcl(ρ,K)=∑jpj⟨j∣K(∣j⟩⟨j∣)∣j⟩.F_{\mathrm{cl}}(\rho,K)= \sum_jp_j\langle j|K(|j\rangle\langle j|)|j\rangle.Fcl​(ρ,K)=j∑​pj​⟨j∣K(∣j⟩⟨j∣)∣j⟩.

The Bures–Uhlmann fidelity used here is the unsquared quantity FBU(σ,τ)=tr⁡σ τ σF_{\mathrm{BU}}(\sigma,\tau)=\operatorname{tr}\sqrt{\sqrt\sigma\,\tau\,\sqrt\sigma}FBU​(σ,τ)=trσ​τσ​​. For the classicizing channel, the reversal operation realizes the pretty good measurement, as shown by equation (36) and the discussion after equation (37) in the preprint, p. 10.

Formalization targets

Recovery error

The goal, in the reading established by the paper's proof, is

Fcl(ρ,RA,ρA)≥1−∑i,j∈Ji≠jpipj FBU(ρ^i,ρ^j).F_{\mathrm{cl}}(\rho,R_{A,\rho}A) \geq 1-\sum_{\substack{i,j\in J\\i\ne j}} \sqrt{p_ip_j}\,F_{\mathrm{BU}}(\hat\rho_i,\hat\rho_j).Fcl​(ρ,RA,ρ​A)≥1−i,j∈Ji=j​∑​pi​pj​​FBU​(ρ^​i​,ρ^​j​).

The sum is over ordered pairs; each unordered pair of distinct labels is counted twice. The coefficient is exactly one. The goal applies to every finite ensemble with the spectral data above and a full-support output. It does not fix the number of labels or the dimension of the output.

The milestones are the reversal formula (36), the classical-fidelity identities in (38), the unit squared Frobenius norm (40), the diagonal-block expression (41), the off-diagonal trace-norm identity following (42), and the two-block estimate of Lemma 6. They record the paper's mathematical statements and keep the attack path tied to the authors' displayed results.

Significance

The result bounds a measurement's probability of error using only pairwise similarities of the possible output states and their prior probabilities. For nearly distinguishable states, the weighted fidelity sum is small, so this particular measurement succeeds with high probability. The theorem therefore gives a usable guarantee for a specified recovery procedure, rather than only asserting that some procedure exists. In the preprint, §VII, Barnum and Knill describe quantum-information applications of such recovery bounds.

The mathematical result is already proved in the paper, subject to the correction explained below. The formalization work is to make the mixed-state channel, its recovery, the finite-dimensional spectral conventions, and the block-matrix norm estimate precise in Lean. The published Prove2Me definitions for Kraus updates and trace norm supply reusable starting points. A complete proof of this mission would add a checked mixed-state pretty-good-measurement bound; the local statements here compile as open theorems, and no proof is claimed.

Difficulty

The obvious pairwise-overlap estimate does not by itself express the error of the recovery channel. The recovery's classical fidelity is initially a channel evaluation on basis states, while the bound uses trace norms of blocks of a Gram matrix. The key obstacle is controlling the off-diagonal Frobenius mass of the positive square root of that Gram matrix by the trace norms of the corresponding blocks of the Gram matrix itself. Lemma 6 states the needed two-block comparison, including rectangular blocks. The matrix dimension and block labels must remain consistent when it is applied across a larger array.

Formalization scope

All systems and index sets are finite, with matrices over C\mathbb CC and real probabilities. A general completely positive map is represented by an unbundled finite family of Kraus matrices. The classicizing family has rectangular matrices from the input-label space to the output space; the reversal has matrices in the opposite direction. Composite Kraus families are indexed by pairs. The classical fidelity is defined from the channel action in equation (10); the goal does not define it using the desired overlap bound. The reversal is defined by equation (12) for a general family, so its specialized formula remains a theorem.

The spectral hypotheses include nonnegative probabilities and eigenvalues, unit sums, and orthonormal eigenvectors. Full support of ρout\rho_{\mathrm{out}}ρout​ is an explicit hypothesis wherever the reversal appears, following page 7. Empty input or output types cannot satisfy the normalized data together with these hypotheses. The Bures–Uhlmann expression is the unsquared trace of a positive square root; using the squared fidelity would change the constant and is outside this mission. Lemma 6 is independent of the ensemble and can be reused for finite block-matrix estimates. Contributions to the spectral identities, the array equalities, and the block-norm argument are welcome.

Equation (39) prints the square of the optimal success probability on its left. The first line of (38) compares that quantity with the recovery fidelity in the opposite direction to Corollary 4. The proof on pages 12–13 concludes the displayed bound for Fcl(ρ,RA,ρA)F_{\mathrm{cl}}(\rho,R_{A,\rho}A)Fcl​(ρ,RA,ρ​A). This mission states that proved conclusion and records the printed discrepancy in its item and audit notes.

Selected references

  • Howard Barnum and Emanuel Knill, Reversing quantum dynamics with near-optimal quantum and classical fidelity, arXiv:quant-ph/0004088v2, 2000/2026 version. arXiv
  • Howard Barnum and Emanuel Knill, Reversing quantum dynamics with near-optimal quantum and classical fidelity, Journal of Mathematical Physics 43 (2002), 2097–2106. DOI
11 thms5 active usersReviewed
🏆Completed
CombinatoricsTheoretical Computer Science·Captain: mikedeng1

Fuzzy Extractors: How to Generate Strong Keys from Biometrics and Other Noisy Data 4: A Secure Sketch Correcting t Errors Has Residual Min-Entropy at Most L(M, t, m)Research Paper

Motivation

Biometric readings, typed passphrases and physical measurements are secrets that are never reproduced exactly: a second reading w′w'w′ of the same fingerprint differs from the enrolled reading www in a few positions. Dodis, Ostrovsky, Reyzin and Smith (arXiv:cs/0602007, SIAM J. Comput. 38(1), 2008) introduced the secure sketch, public helper data that lets anyone holding a nearby w′w'w′ recover www while leaking as little as possible about www, and the fuzzy extractor, which in addition turns www into a nearly uniform key. Their constructions for the Hamming, set-difference and edit metrics are the standard reference for this primitive in cryptography.

A construction is judged by its entropy loss: how much min-entropy of the secret the published sketch destroys. To call a construction optimal one needs a lower bound on that loss which holds for every sketch, whatever its algorithm. Appendix C of the paper supplies such a bound from coding theory. It shows that, for uniformly distributed inputs, the code-offset sketch for the Hamming metric and the set-difference sketches lose no more entropy than any sketch must. This mission formalizes that bound, Lemma C.1.

Setting

A metric space is a finite set M\mathcal MM with an integer-valued distance dis\mathrm{dis}dis; the paper also requires dis(x,y)=0\mathrm{dis}(x,y)=0dis(x,y)=0 exactly when x=yx=yx=y, symmetry, and the triangle inequality (§2.1, p. 7). Random variables are identified with their laws; logarithms are base 2.

The min-entropy of a random variable AAA is H∞(A)=−log⁡max⁡aPr⁡[A=a]\mathbf H_\infty(A) = -\log \max_a \Pr[A=a]H∞​(A)=−logmaxa​Pr[A=a]. For a pair (A,B)(A,B)(A,B) the average min-entropy is

H~∞(A∣B)=−log⁡Eb←B[max⁡aPr⁡[A=a∣B=b]],\tilde{\mathbf H}_\infty(A\mid B) = -\log \mathbb E_{b\leftarrow B}\Big[\max_a \Pr[A=a\mid B=b]\Big],H~∞​(A∣B)=−logEb←B​[amax​Pr[A=a∣B=b]],

the negative logarithm of the probability that an adversary who sees BBB guesses AAA.

An (M,m,m~,t)(\mathcal M,m,\tilde m,t)(M,m,m~,t)-secure sketch (Definition 3, p. 11) is a pair of randomized procedures: SS\mathsf{SS}SS maps w∈Mw\in\mathcal Mw∈M to a string sss, and Rec\mathsf{Rec}Rec maps (w′,s)(w',s)(w′,s) back to M\mathcal MM. Correctness: if dis(w,w′)≤t\mathrm{dis}(w,w')\le tdis(w,w′)≤t then Rec(w′,SS(w))=w\mathsf{Rec}(w',\mathsf{SS}(w))=wRec(w′,SS(w))=w. Security: for every distribution WWW on M\mathcal MM with H∞(W)≥m\mathbf H_\infty(W)\ge mH∞​(W)≥m, one has H~∞(W∣SS(W))≥m~\tilde{\mathbf H}_\infty(W\mid \mathsf{SS}(W))\ge\tilde mH~∞​(W∣SS(W))≥m~.

An (M,K,t)(\mathcal M,K,t)(M,K,t)-code (§2.2, p. 8) is a set C⊆MC\subseteq\mathcal MC⊆M of KKK points such that every ball {c:dis(w,c)≤t}\{c : \mathrm{dis}(w,c)\le t\}{c:dis(w,c)≤t} around a point w∈Mw\in\mathcal Mw∈M contains at most one codeword. For S⊆MS\subseteq\mathcal MS⊆M, K(M,t,S)K(\mathcal M,t,S)K(M,t,S) is the largest KKK for which an (M,K,t)(\mathcal M,K,t)(M,K,t)-code lies inside SSS, and K(M,t)=K(M,t,M)K(\mathcal M,t)=K(\mathcal M,t,\mathcal M)K(M,t)=K(M,t,M). Finally (Appendix C, p. 40)

L(M,t,m)=log⁡(min⁡∣S∣=2mK(M,t,S)),L(\mathcal M,t,m) = \log\Big(\min_{|S|=2^m} K(\mathcal M,t,S)\Big),L(M,t,m)=log(∣S∣=2mmin​K(M,t,S)),

the worst case, over all sets SSS of 2m2^m2m points, of the largest ttt-error-correcting code inside SSS.

In the Lean development these are minEntropy, avgMinEntropy, IsSecureSketch, IsCode, K dis t S and L dis t N hN, in the namespace FuzzyExtractors.LowerBound.

Formalization targets

Goal: Lemma C.1

If (SS,Rec)(\mathsf{SS},\mathsf{Rec})(SS,Rec) is an (M,m,m′,t)(\mathcal M,m,m',t)(M,m,m′,t)-secure sketch and 2m=N2^m=N2m=N is a natural number with N≤∣M∣N\le|\mathcal M|N≤∣M∣, then

m′≤L(M,t,m).m' \le L(\mathcal M,t,m).m′≤L(M,t,m).

The bound fixes no particular metric and no particular sketch; it is stated for every finite integer-valued metric and every sketch, with an arbitrary type of sketch values.

Milestones

The proof in Appendix C has three steps, each a milestone. For WWW uniform on a set SSS of 2m2^m2m points:

  1. some sketch value vvv has Pr⁡[SS(W)=v]>0\Pr[\mathsf{SS}(W)=v]>0Pr[SS(W)=v]>0 and H∞(W∣SS(W)=v)≥m′\mathbf H_\infty(W\mid\mathsf{SS}(W)=v)\ge m'H∞​(W∣SS(W)=v)≥m′;
  2. the set TTT of points of SSS that can produce vvv has ∣T∣≥2m′|T|\ge 2^{m'}∣T∣≥2m′;
  3. under the correctness property alone, TTT is an (M,∣T∣,t)(\mathcal M,|T|,t)(M,∣T∣,t)-code.

A fourth milestone is the lemma's second sentence: when m=log⁡∣M∣m=\log|\mathcal M|m=log∣M∣,

m′≤log⁡K(M,t).m' \le \log K(\mathcal M,t).m′≤logK(M,t).

Significance

The result. Lemma C.1 converts any secure sketch into a code: the residual entropy m′m'm′ of the sketch can be no larger than the logarithm of the best ttt-error-correcting code inside a worst-case set of 2m2^m2m points. For uniform inputs it says m′≤log⁡K(M,t)m'\le\log K(\mathcal M,t)m′≤logK(M,t), so the entropy loss is at least log⁡∣M∣−log⁡K(M,t)\log|\mathcal M|-\log K(\mathcal M,t)log∣M∣−logK(M,t). The code-offset construction built from an optimal code attains that loss, which is how the paper certifies its Hamming and set-difference constructions as optimal for uniform passwords. The companion Lemma C.2 gives the analogous bound for fuzzy extractors, up to a −log⁡(1−ε)-\log(1-\varepsilon)−log(1−ε) term. Lower bounds of this shape are what separate an efficient construction from a provably best one.

Formalizing it. The lemma has a complete, short proof in the paper; it has no machine-checked proof that we know of. The mission produces a checked version of the bound for arbitrary finite integer metrics and arbitrary randomized sketches, together with reusable definitions of min-entropy and average min-entropy on probability mass functions, of secure sketches, and of ttt-error-correcting codes in a general finite metric space.

Difficulty

The combinatorial core, that the preimage set of one sketch value is a code, is immediate from correctness. The work lies in the probabilistic bookkeeping. One must pass from an average bound on guessing probability to a single good sketch value, which requires handling sketch values of probability zero and an infinite (possibly uncountable) space of sketch outputs. One must then pass from "Pr⁡[W=w∣v]≤2−m′\Pr[W=w\mid v]\le 2^{-m'}Pr[W=w∣v]≤2−m′ for all www" to "at least 2m′2^{m'}2m′ points carry positive probability", and compute the min-entropy of a uniform distribution exactly. Finally the bound must be transferred to the minimum over all sets of size 2m2^m2m, a finite but large family. A first idea, to reason only about deterministic sketches, does not suffice: Definition 3 allows randomized SS\mathsf{SS}SS and Rec\mathsf{Rec}Rec, and the statement quantifies over them.

Formalization scope

Laws are Mathlib PMFs; randomized procedures are maps into PMF. The sketch value type V is arbitrary, standing in for {0,1}∗\{0,1\}^*{0,1}∗. Average min-entropy is written in the equivalent joint form −log⁡∑bmax⁡aPr⁡[A=a∧B=b]-\log\sum_b\max_a\Pr[A=a\wedge B=b]−log∑b​maxa​Pr[A=a∧B=b], which avoids conditioning on null events. "Min-entropy mmm" is read as H∞(W)≥m\mathbf H_\infty(W)\ge mH∞​(W)≥m, and m,m′m, m'm,m′ are real numbers. Rec\mathsf{Rec}Rec is randomized and correctness asks that it return www with probability one for every possible sketch value of www.

The explicit choices:

  • L(M,t,m)L(\mathcal M,t,m)L(M,t,m) is defined only when 2m2^m2m is a natural number N≤∣M∣N\le|\mathcal M|N≤∣M∣ (otherwise the minimum ranges over no sets); the goal takes such an NNN with (N:R)=2m(N:\mathbb R)=2^m(N:R)=2m. The printed K(n,t,S)K(n,t,S)K(n,t,S) inside the minimum is read as K(M,t,S)K(\mathcal M,t,S)K(M,t,S), and the printed L(M,t,n)L(\mathcal M,t,n)L(M,t,n) as L(M,t,log⁡∣M∣)L(\mathcal M,t,\log|\mathcal M|)L(M,t,log∣M∣).
  • The code-bound statements explicitly assume all metric axioms from §2.1: zero distance exactly for equal points, symmetry, and the triangle inequality. Symmetry is used because the ball condition of a code measures dis(w′,c)\mathrm{dis}(w',c)dis(w′,c), while correctness is stated for dis(c,w′)\mathrm{dis}(c,w')dis(c,w′). The second-sentence milestone also assumes M\mathcal MM nonempty, which the paper leaves implicit.
  • The hypothesis is the worst-case secure sketch of Definition 3, not the average-case one of Definition 4, which would weaken the lemma.
  • Definition 3's efficiency requirement is dropped; no complexity theory is formalized, and no placeholder predicate replaces it.

Two trivializing formalizations are ruled out: K(M,t,S)K(\mathcal M,t,S)K(M,t,S) is the largest size of a code in SSS, not a count of codes; and a code is defined by the ball condition, not by "distinct codewords are at distance greater than ttt", which is weaker in the absence of the triangle inequality.

Needed infrastructure: the min-entropy of a uniform PMF on a finset, the averaging argument over a tsum of ENNReal values, and monotonicity of Finset.inf'. The min-entropy and code definitions are reusable by every other mission of this paper. Contributions are welcome on any milestone, in any order.

Selected references

  • Y. Dodis, R. Ostrovsky, L. Reyzin, A. Smith, Fuzzy Extractors: How to Generate Strong Keys from Biometrics and Other Noisy Data, SIAM J. Comput. 38(1):97–139, 2008. arXiv:cs/0602007v4. https://arxiv.org/abs/cs/0602007 — DOI https://doi.org/10.1137/060651380
  • A. Juels, M. Wattenberg, A Fuzzy Commitment Scheme, ACM CCS 1999. https://doi.org/10.1145/319709.319714
  • R. Renner, S. Wolf, Simple and Tight Bounds for Information Reconciliation and Privacy Amplification, ASIACRYPT 2005. https://doi.org/10.1007/11593447_11
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Information-Theoretic Analysis of Generalization Capability of Learning Algorithms I: The Expected Generalization Error Is at Most √(2σ²I(S;W)/n) (Theorem 1)Research Paper

Motivation

A learning algorithm trained on a finite sample generalizes when its empirical risk on that sample is close to its risk on fresh data. Classical guarantees come from uniform convergence over the hypothesis class (VC dimension, Rademacher complexity) or from algorithmic stability, such as uniform stability (Bousquet and Elisseeff, 2002) and on-average stability (Shalev-Shwartz et al., 2010). Both families look at the class or at the algorithm's worst-case sensitivity, not at how much the trained hypothesis actually depends on the data it was trained on.

Russo and Zou (arXiv:1511.05219, 2016) bounded the bias of adaptive data analysis by mutual information, and Xu and Raginsky (arXiv:1705.07809, NIPS 2017) turned this into a generalization bound for learning algorithms: the expected generalization error is at most 2σ2I(S;W)/n\sqrt{2\sigma^2 I(S;W)/n}2σ2I(S;W)/n​, where I(S;W)I(S;W)I(S;W) is the mutual information between the training sample and the output hypothesis. This bound started the line of information-theoretic generalization bounds, later refined to individual-sample mutual information (Bu, Zou and Veeravalli, 2020), conditional mutual information (Steinke and Zakynthinou, 2020) and chaining variants (Asadi, Abbe and Verdú, 2018).

Timeline:

  • 2016, Russo and Zou: bias of adaptive analysis bounded by I(ΛW(S);W)I(\Lambda_{\mathsf W}(S);W)I(ΛW​(S);W), the information carried by the vector of empirical risks, for a finite hypothesis space.
  • 2017, Xu and Raginsky: the bound with the input–output mutual information I(S;W)I(S;W)I(S;W), for arbitrary hypothesis spaces (Theorem 1); high-probability versions and an analysis of the Gibbs algorithm.
  • 2018–2020: chaining, individual-sample and conditional mutual information refinements.

Setting

There is an instance space Z\mathsf ZZ, a hypothesis space W\mathsf WW and a nonnegative loss ℓ:W×Z→R+\ell:\mathsf W\times\mathsf Z\to\mathbb R_+ℓ:W×Z→R+​, written ℓ : W → Z → ℝ in Lean. Data are drawn from an unknown probability measure μ\muμ on Z\mathsf ZZ; a dataset of size nnn is an i.i.d. sample S=(Z1,…,Zn)∼μ⊗nS=(Z_1,\dots,Z_n)\sim\mu^{\otimes n}S=(Z1​,…,Zn​)∼μ⊗n (sampleLaw μ n).

A learning algorithm is a Markov kernel PW∣SP_{W|S}PW∣S​ (κ : Kernel (Fin n → Z) W): given the dataset, it outputs a random hypothesis WWW. The pair (S,W)(S,W)(S,W) has joint law PS,W=μ⊗n⊗PW∣SP_{S,W}=\mu^{\otimes n}\otimes P_{W|S}PS,W​=μ⊗n⊗PW∣S​ (sampleLaw μ n ⊗ₘ κ), with marginals PS=μ⊗nP_S=\mu^{\otimes n}PS​=μ⊗n and PWP_WPW​.

The population risk and the empirical risk of a hypothesis www are

Lμ(w)=∫Zℓ(w,z) μ(dz),LS(w)=1n∑i=1nℓ(w,Zi)L_\mu(w)=\int_{\mathsf Z}\ell(w,z)\,\mu(dz),\qquad L_S(w)=\frac1n\sum_{i=1}^n \ell(w,Z_i)Lμ​(w)=∫Z​ℓ(w,z)μ(dz),LS​(w)=n1​i=1∑n​ℓ(w,Zi​)

(risk ℓ μ w, empRisk ℓ s w). The expected generalization error is

gen(μ,PW∣S)=E[Lμ(W)−LS(W)],\mathrm{gen}(\mu,P_{W|S})=\mathbb E\big[L_\mu(W)-L_S(W)\big],gen(μ,PW∣S​)=E[Lμ​(W)−LS​(W)],

the expectation taken under PS,WP_{S,W}PS,W​ (genError ℓ μ κ).

The mutual information of a pair (X,Y)(X,Y)(X,Y) with joint law PX,YP_{X,Y}PX,Y​ is the relative entropy I(X;Y)=D(PX,Y ∥ PX⊗PY)∈[0,∞]I(X;Y)=D(P_{X,Y}\,\|\,P_X\otimes P_Y)\in[0,\infty]I(X;Y)=D(PX,Y​∥PX​⊗PY​)∈[0,∞] (mutualInfo). A real random variable UUU is σ\sigmaσ-subgaussian if log⁡E[eλ(U−EU)]≤λ2σ2/2\log\mathbb E[e^{\lambda(U-\mathbb EU)}]\le\lambda^2\sigma^2/2logE[eλ(U−EU)]≤λ2σ2/2 for all λ∈R\lambda\in\mathbb Rλ∈R.

Formalization targets

Goal: Theorem 1 (p. 4)

If ℓ(w,Z)\ell(w,Z)ℓ(w,Z) is σ\sigmaσ-subgaussian under μ\muμ for every w∈Ww\in\mathsf Ww∈W, then

∣gen(μ,PW∣S)∣≤2σ2n I(S;W).\big|\mathrm{gen}(\mu,P_{W|S})\big|\le\sqrt{\frac{2\sigma^2}{n}\,I(S;W)} .​gen(μ,PW∣S​)​≤n2σ2​I(S;W)​.

The statement fixes no structure on W\mathsf WW (it may be uncountable) and no bound on the loss beyond subgaussianity.

Milestones

  1. (A.1), Donsker–Varadhan (p. 11), the inequality ∫F dπ−D(π∥ρ)≤log⁡∫eF dρ\int F\,d\pi-D(\pi\|\rho)\le\log\int e^F\,d\rho∫Fdπ−D(π∥ρ)≤log∫eFdρ. Already proved on the platform and referenced.
  2. Lemma 1 (p. 3), the decoupling estimate: if f(Xˉ,Yˉ)f(\bar X,\bar Y)f(Xˉ,Yˉ) is σ\sigmaσ-subgaussian under PX⊗PYP_X\otimes P_YPX​⊗PY​, then
∣Ef(X,Y)−Ef(Xˉ,Yˉ)∣≤2σ2I(X;Y).\big|\mathbb E f(X,Y)-\mathbb E f(\bar X,\bar Y)\big|\le\sqrt{2\sigma^2 I(X;Y)} .​Ef(X,Y)−Ef(Xˉ,Yˉ)​≤2σ2I(X;Y)​.
  1. Subgaussianity of the empirical risk (§3.2, p. 4): for every www, LS(w)−Lμ(w)L_S(w)-L_\mu(w)LS​(w)−Lμ​(w) is σ/n\sigma/\sqrt nσ/n​-subgaussian under μ⊗n\mu^{\otimes n}μ⊗n.
  2. The mixture step (§3.2, p. 4, corrected): under PS⊗PWP_S\otimes P_WPS​⊗PW​, f(Sˉ,Wˉ)=LSˉ(Wˉ)−Lμ(Wˉ)f(\bar S,\bar W)=L_{\bar S}(\bar W)-L_\mu(\bar W)f(Sˉ,Wˉ)=LSˉ​(Wˉ)−Lμ​(Wˉ) is σ/n\sigma/\sqrt nσ/n​-subgaussian with mean 000.

Significance

The result. Theorem 1 makes generalization a property of the dependence between data and output rather than of the size of the hypothesis class. It applies to randomized algorithms on uncountable or infinite-dimensional hypothesis spaces, where uniform convergence gives nothing, and to unbounded subgaussian losses. Any mechanism that limits I(S;W)I(S;W)I(S;W), such as noise injection, differential privacy, compression or relative-entropy regularization, inherits a generalization guarantee. A loss with values in [a,b][a,b][a,b] is (b−a)/2(b-a)/2(b−a)/2-subgaussian for every μ\muμ, so the theorem covers all bounded losses. The bound is also the template for the later refinements listed above, which share Lemma 1's decoupling argument.

Formalizing it. The result is proved on paper; no machine-checked proof is known. A formalization supplies a reusable statement of mutual information as a relative entropy of a joint law on general measurable spaces, a decoupling lemma for subgaussian functions, and the mixture argument for subgaussian families, all of which recur in the later literature. It also settles a point the paper leaves loose: the printed proof applies Lemma 1 to the uncentred empirical risk, which is not subgaussian in general; the milestones state the corrected step.

Difficulty

The two halves of the proof are short on paper, but each step that "follows" uses a fact the page does not state. The decoupling estimate needs Ef(X,Y)\mathbb E f(X,Y)Ef(X,Y) to be finite, which holds only because finite relative entropy and exponential integrability under the product together force integrability under the joint law. The mixture step needs the moment-generating-function bound of each section w↦f(⋅,w)w\mapsto f(\cdot,w)w↦f(⋅,w) to integrate over PWP_WPW​, which requires joint measurability and the centring of every section at its own mean: the uncentred empirical risk LSˉ(Wˉ)L_{\bar S}(\bar W)LSˉ​(Wˉ) mixes laws with different means and is not subgaussian.

A natural first attempt applies Lemma 1 directly to f(s,w)=Ls(w)f(s,w)=L_s(w)f(s,w)=Ls​(w) as printed; it fails on the example ℓ(w,z)=w\ell(w,z)=wℓ(w,z)=w with WWW uniform on {0,1}\{0,1\}{0,1} and independent of SSS.

Formalization scope

  • Objects. The sample law, LμL_\muLμ​ and LSL_SLS​ are reused from the published LearnStability.Characterization.Setting. This mission defines mutualInfo P := klDiv P (P.fst.prod P.snd) (values in [0,∞][0,\infty][0,∞]) and genError, the integral of the pointwise difference Lμ(w)−Ls(w)L_\mu(w)-L_s(w)Lμ​(w)−Ls​(w) under sampleLaw μ n ⊗ₘ κ. Samples are Fin n → Z; the algorithm is a Markov kernel.
  • Subgaussianity is Mathlib's HasSubgaussianMGF of the centred variable, whose parameter is the variance proxy: σ2\sigma^2σ2 for the loss, σ2/n\sigma^2/nσ2/n for the empirical risk.
  • Added hypotheses, all implicit on the page: n≥1n\ge1n≥1 (the bound divides by nnn); joint measurability of ℓ\ellℓ (so that Lμ(W)L_\mu(W)Lμ​(W) and LS(W)L_S(W)LS​(W) are random variables); and I≠∞I\ne\inftyI=∞ in Lemma 1 and Theorem 1, because Lean's conversion of ∞\infty∞ to a real number gives 000, which would turn the page's vacuous bound into a false claim. The page's nonnegativity of ℓ\ellℓ is kept. No integrability hypothesis on fff or on the losses is assumed beyond subgaussianity.
  • Correction of the print. The page says that f(Sˉ,Wˉ)=LSˉ(Wˉ)f(\bar S,\bar W)=L_{\bar S}(\bar W)f(Sˉ,Wˉ)=LSˉ​(Wˉ) is σ/n\sigma/\sqrt nσ/n​-subgaussian; milestone 4 states it for the centred LSˉ(Wˉ)−Lμ(Wˉ)L_{\bar S}(\bar W)-L_\mu(\bar W)LSˉ​(Wˉ)−Lμ​(Wˉ), together with its mean being 000. Equation (9) is not posed separately.
  • Ruled out. The goal is stated for genError and the mutual information of the algorithm's own joint law; a version through Lemma 1's abstract pair (Xˉ,Yˉ)(\bar X,\bar Y)(Xˉ,Yˉ), through I(ΛW(S);W)I(\Lambda_{\mathsf W}(S);W)I(ΛW​(S);W) (Theorem 2, out of scope), or with III truncated to a real number would not be this theorem.
  • Infrastructure. Integrability transfer from PX⊗PYP_X\otimes P_YPX​⊗PY​ to PX,YP_{X,Y}PX,Y​ under finite relative entropy; sums of independent subgaussian variables on Measure.pi (Mathlib has HasSubgaussianMGF.sum_of_iIndepFun); mixtures of mean-zero subgaussian families under a product measure. These are reusable beyond this mission, and contributions of each are welcome.

Selected references

  • A. Xu, M. Raginsky, Information-theoretic analysis of generalization capability of learning algorithms, NIPS 2017; arXiv:1705.07809v2. https://arxiv.org/abs/1705.07809
  • D. Russo, J. Zou, Controlling bias in adaptive data analysis using information theory, AISTATS 2016. https://arxiv.org/abs/1511.05219
  • S. Shalev-Shwartz, O. Shamir, N. Srebro, K. Sridharan, Learnability, stability and uniform convergence, JMLR 11, 2010. https://jmlr.org/papers/v11/shalev-shwartz10a.html
  • O. Bousquet, A. Elisseeff, Stability and generalization, JMLR 2, 2002. https://www.jmlr.org/papers/v2/bousquet02a.html
  • S. Boucheron, G. Lugosi, P. Massart, Concentration Inequalities, Oxford University Press, 2013 (Donsker–Varadhan, Cor. 4.15). https://doi.org/10.1093/acprof:oso/9780199535255.001.0001
  • A. Asadi, E. Abbe, S. Verdú, Chaining mutual information and tightening generalization bounds, NeurIPS 2018. https://arxiv.org/abs/1806.03803
  • Y. Bu, S. Zou, V. Veeravalli, Tightening mutual information based bounds on generalization error, IEEE JSAIT 2020. https://arxiv.org/abs/1901.04609
  • T. Steinke, L. Zakynthinou, Reasoning about generalization via conditional mutual information, COLT 2020. https://arxiv.org/abs/2001.09122
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Probability·Captain: wurtle

Sharp binary-information contraction on the discrete cubeResearch Paper

Motivation

Draw nnn independent fair bits XXX, compute a one-bit summary f(X)f(X)f(X), and send the bits through independent binary symmetric channels with crossover probability ε\varepsilonε, producing YYY. Which summary tells the receiver the most about YYY? Kumar and Courtade conjectured that a single coordinate, f(X)=X1f(X)=X_1f(X)=X1​, is optimal: I(f(X);Y)≤1−h2(ε)I(f(X);Y)\le 1-h_2(\varepsilon)I(f(X);Y)≤1−h2​(ε) bits for every Boolean fff, in every dimension and at every noise level (ISIT 2013; IEEE Trans. Inf. Theory 2014). The Courtade–Kumar (most informative Boolean function) conjecture is a basic question about how noise destroys information on the discrete cube, connecting information theory with Boolean Fourier analysis and hypercontractivity.

This mission asks for a formal proof of a sharp contraction theorem for arbitrary randomized binary summaries, whose Boolean case is the Courtade–Kumar conjecture, as stated in an OpenAI preprint dated September 24, 2026 (source). The preprint has not been peer reviewed and its claims have not been independently verified; on the platform the Lean goal is open.

Background

  • 1970–1976 — Hypercontractivity on the cube (Bonami, Ann. Inst. Fourier 1970; Gross, Amer. J. Math. 1975; Beckner, Annals 1975); Mrs. Gerber's lemma (Wyner–Ziv, IEEE TIT 1973).
  • 2013–2014 — Kumar and Courtade pose the conjecture and prove a coordinatewise sum bound.
  • 2016 — High-noise results: Ordentlich, Shayevitz and Weinstein for balanced functions (ISIT 2016); Samorodnitsky for all Boolean functions in a dimension-independent high-noise range (IEEE TIT 2016).
  • 2018 — Pichler, Piantanida and Matz prove coordinate optimality when the observation is also reduced to one bit (Ann. Appl. Probab. 2018).
  • 2020–2023 — Barnes–Özgür's symmetrized reformulation (ISIT 2020); Li–Médard on fixed-mean optimizers (IEEE TIT 2021); Yu's Φ\PhiΦ-stability (PTRF 2023).
  • 2025–2026 — Chen, Gohari and Nair's differential (entropy-production) approach; independent preprints announcing proofs by Chen, Gohari, Javanmard, Lin, Mirrokni, Nair and Woodruff (arXiv:2609.24931), Ky and Tran (arXiv:2609.24184), Mahdavifar and Beirami (arXiv:2609.26444), and a bias-retaining finite-noise bound by Kramer and Saglam.
  • September 2026 — The OpenAI preprint (Theorems 1.1 and 1.3, Corollary 1.2, pp. 1–4).

Setting

Let Ωn={−1,1}n\Omega_n=\{-1,1\}^nΩn​={−1,1}n with uniform measure; information is in nats unless stated. For r∈[−1,1]r\in[-1,1]r∈[−1,1] put

L=log⁡2,H(r)=−1+r2log⁡1+r2−1−r2log⁡1−r2,ψ(r)=L−H(r),L=\log2,\quad H(r)=-\tfrac{1+r}2\log\tfrac{1+r}2-\tfrac{1-r}2\log\tfrac{1-r}2,\quad \psi(r)=L-H(r),L=log2,H(r)=−21+r​log21+r​−21−r​log21−r​,ψ(r)=L−H(r),

with 0log⁡0=00\log0=00log0=0; ψ−1\psi^{-1}ψ−1 is the increasing branch [0,L]→[0,1][0,L]\to[0,1][0,L]→[0,1]. A soft channel is u:Ωn→[−1,1]u:\Omega_n\to[-1,1]u:Ωn​→[−1,1], the conditional mean of an auxiliary sign UUU given XXX; its information is I(u)=H(Eu)−EH(u)=I(U;X)I(u)=H(\mathbb Eu)-\mathbb EH(u)=I(U;X)I(u)=H(Eu)−EH(u)=I(U;X). For ρ∈[−1,1]\rho\in[-1,1]ρ∈[−1,1] let Yi=XiZiY_i=X_iZ_iYi​=Xi​Zi​ with independent signs EZi=ρ\mathbb EZ_i=\rhoEZi​=ρ, and let Tρu(y)=E[u(X)∣Y=y]T_\rho u(y)=\mathbb E[u(X)\mid Y=y]Tρ​u(y)=E[u(X)∣Y=y], so I(Tρu)=I(U;Y)I(T_\rho u)=I(U;Y)I(Tρ​u)=I(U;Y). For an interior field g:Ωn→(−1,1)g:\Omega_n\to(-1,1)g:Ωn​→(−1,1) with m=Egm=\mathbb Egm=Eg, the production is D(g)=E[atanh⁡(g) Ng]D(g)=\mathbb E[\operatorname{atanh}(g)\,Ng]D(g)=E[atanh(g)Ng] with Ng=12∑i(g−g∘flipi)Ng=\frac12\sum_i(g-g\circ\mathrm{flip}_i)Ng=21​∑i​(g−g∘flipi​); the rate FFF is defined by F(ψ(r))=ratanh⁡rF(\psi(r))=r\operatorname{atanh}rF(ψ(r))=ratanhr; S(I)=F(I)−2IS(I)=F(I)-2IS(I)=F(I)−2I (zero for I<0I<0I<0); Bm(I)=2I+(1−m2)S(L−H(m)−I1−m2)B_m(I)=2I+(1-m^2)S\bigl(L-\frac{H(m)-I}{1-m^2}\bigr)Bm​(I)=2I+(1−m2)S(L−1−m2H(m)−I​).

Formalization targets

Milestone: Courtade–Kumar inequality in bits (Corollary 1.2, p. 2)

For n≥1n\ge1n≥1, 0≤ε≤120\le\varepsilon\le\frac120≤ε≤21​ and every Boolean fff on {0,1}n\{0,1\}^n{0,1}n,

I2(f(X);Y)≤1−h2(ε),I_2(f(X);Y)\le 1-h_2(\varepsilon),I2​(f(X);Y)≤1−h2​(ε),

with equality for every coordinate x↦xix\mapsto x_ix↦xi​ and its complement.

Goal: the soft contraction package (Theorem 1.1, p. 1; Corollary 1.2, p. 2; Theorem 1.3, p. 4)

The goal OAI.SoftChannel204.fullMain is the conjunction of:

  1. Theorem 1.1. For all nnn, u:Ωn→[−1,1]u:\Omega_n\to[-1,1]u:Ωn​→[−1,1], ρ∈[−1,1]\rho\in[-1,1]ρ∈[−1,1]:
I(Tρu)≤ψ(∣ρ∣ ψ−1(I(u))),I(T_\rho u)\le\psi\bigl(|\rho|\,\psi^{-1}(I(u))\bigr),I(Tρ​u)≤ψ(∣ρ∣ψ−1(I(u))),

with equality for every soft coordinate u(x)=axiu(x)=a x_iu(x)=axi​, ∣a∣≤1|a|\le1∣a∣≤1; and I(U;Y)=I(Tρu)I(U;Y)=I(T_\rho u)I(U;Y)=I(Tρ​u) for the joint law of (U,Y)(U,Y)(U,Y). 2. Corollary 1.2. For Boolean fff with m=Efm=\mathbb Efm=Ef and rm=ψ−1(H(m))r_m=\psi^{-1}(H(m))rm​=ψ−1(H(m)): I(f(X);Y)≤ψ(∣ρ∣rm)≤ψ(∣ρ∣)I(f(X);Y)\le\psi(|\rho|r_m)\le\psi(|\rho|)I(f(X);Y)≤ψ(∣ρ∣rm​)≤ψ(∣ρ∣), strictly below ψ(∣ρ∣)\psi(|\rho|)ψ(∣ρ∣) when 0<∣m∣<10<|m|<10<∣m∣<1 and 0<∣ρ∣0<|\rho|0<∣ρ∣; coordinates and their negations attain ψ(∣ρ∣)\psi(|\rho|)ψ(∣ρ∣); and the bits conversion ψ(1−2ε)/L=1−h2(ε)\psi(1-2\varepsilon)/L=1-h_2(\varepsilon)ψ(1−2ε)/L=1−h2​(ε). 3. Theorem 1.3. For every interior ggg: D(g)≥max⁡{Bm(I(g)),F(I(g))}≥F(I(g))D(g)\ge\max\{B_m(I(g)),F(I(g))\}\ge F(I(g))D(g)≥max{Bm​(I(g)),F(I(g))}≥F(I(g)).

Significance

The result itself. It settles the Courtade–Kumar conjecture and strengthens it in two directions: to randomized summaries at fixed initial information, and to a bias-dependent bound that is strictly better for nonconstant biased outputs. Theorem 1.3 is a mean-dependent entropy-production inequality, stronger than the scalar rate needed for Theorem 1.1. Several independent proofs of the Boolean conjecture were announced in the same period; the preprint compares its production profile with that of Chen et al. in Section 8.

Formalizing it. All objects are finite sums over {−1,1}n\{-1,1\}^n{−1,1}n, so the statements are elementary to state in Lean. The proof requires an explicit three-point optimizer for a joining problem, convexity facts about FFF and SSS (Lemmas 2.2–2.4, pp. 5–6), dimension induction and integration along the noise semigroup. A formal proof would give a checked solution of a conjecture with several competing announced proofs, some computer-assisted.

Difficulty

The local-to-global method of Chen, Gohari and Nair needs a local inequality to pass from the two halves of the cube to the whole. The natural information-only profile Φm(I)=F(I)\Phi_m(I)=F(I)Φm​(I)=F(I) fails the corresponding local comparison for some coupled pair laws, so the induction must carry the mean mmm as well. The preprint uses the maximum of two profiles, BmB_mBm​ and FFF; it must solve the minimization of the joining cost exactly (Section 3), pay the interior pair with a variance-refined one-bit inequality (Lemma 4.1, p. 12), and control the common-output corners by a thinning argument (Theorem 6.1, p. 17). The linear bound D(g)≥2I(g)D(g)\ge2I(g)D(g)≥2I(g) from the log-Sobolev inequality does not suffice; the nonlinear surplus above 2I2I2I is where the difficulty lies.

Formalization scope

  • Cube n = Fin n → Bool, averages are finite sums divided by 2n2^n2n, logs are natural; sign maps Bool to ±1\pm1±1.
  • psiInv is Function.invFunOn psi (Icc 0 1); since ψ\psiψ is strictly increasing on [0,1][0,1][0,1] and I(u)∈[0,L]I(u)\in[0,L]I(u)∈[0,L], this is the paper's branch.
  • noise ρ u y = ∑ x, kernel ρ y x * u x with kernel the product of (1±ρ)/2(1\pm\rho)/2(1±ρ)/2, which is TρT_\rhoTρ​. Mutual information is the finite sum over the joint table, with terms omitted where the joint probability is 000.
  • F is stated as psiInv s * artanh (psiInv s) and is only used on [0,L)[0,L)[0,L); for interior ggg, ∣m∣<1|m|<1∣m∣<1 and 0≤I(g)<H(m)≤L0\le I(g)<H(m)\le L0≤I(g)<H(m)≤L, so reserve and hybrid are evaluated in their source domain.
  • All results hold for every n≥0n\ge0n≥0; the attainment statements quantify over i : Fin n. The milestone (separate definition file) uses the crossover form with bits.

Selected references

  • OpenAI, Sharp binary-information contraction on the discrete cube, OpenAI Math Release preprint, September 24, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Sharp-binary-information-contraction-on-the-discrete-cube-September-24-2026/main.pdf
  • T. A. Courtade, G. R. Kumar, Which Boolean functions maximize mutual information on noisy inputs?, IEEE Trans. Inf. Theory 60 (2014). https://doi.org/10.1109/TIT.2014.2326877
  • G. R. Kumar, T. A. Courtade, Which Boolean functions are most informative?, ISIT 2013. https://doi.org/10.1109/ISIT.2013.6620221
  • A. Samorodnitsky, On the entropy of a noisy function, IEEE Trans. Inf. Theory (2016). https://doi.org/10.1109/TIT.2016.2584625
  • O. Ordentlich, O. Shayevitz, O. Weinstein, An improved upper bound for the most informative Boolean function conjecture, ISIT 2016. https://doi.org/10.1109/ISIT.2016.7541349
  • G. Pichler, P. Piantanida, G. Matz, Dictator functions maximize mutual information, Ann. Appl. Probab. (2018). https://doi.org/10.1214/18-AAP1384
  • L. Yu, On the Φ\PhiΦ-stability and related conjectures, Probab. Theory Relat. Fields (2023). https://doi.org/10.1007/s00440-023-01209-5
  • A. Gohari, C. Nair, Outer bounds for multiuser settings: the auxiliary receiver approach, IEEE Trans. Inf. Theory (2022). https://doi.org/10.1109/TIT.2021.3128136
  • Z. Chen, A. Gohari, A. Javanmard, et al., A proof of the most informative Boolean function conjecture, arXiv:2609.24931 (2026). https://arxiv.org/abs/2609.24931
  • V. K. Ky, T. Tran, Dictators are most informative, arXiv:2609.24184 (2026). https://arxiv.org/abs/2609.24184
  • H. Mahdavifar, A. Beirami, The most informative bit and beyond, arXiv:2609.26444 (2026). https://arxiv.org/abs/2609.26444
  • S. G. Bobkov, P. Tetali, Modified logarithmic Sobolev inequalities in discrete settings, J. Theoret. Probab. (2006). https://doi.org/10.1007/s10959-006-0016-3
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AlgebraCombinatoricsTheoretical Computer Science·Captain: mikedeng1

Fuzzy Extractors: How to Generate Strong Keys from Biometrics and Other Noisy Data 2: The Improved Juels–Sudan Sketch Is an Average-Case Secure Sketch for s-Element Sets with Entropy Loss t log nResearch Paper

Motivation

Many security-relevant inputs are noisy and do not repeat exactly: fingerprint minutiae, iris codes, lists of personal preferences, the set of features extracted from a document. A cryptographic key derived from such an input must be reproducible from a later, slightly different reading, without storing the input itself. Dodis, Ostrovsky, Reyzin and Smith (SIAM J. Comput. 38(1), 2008; arXiv:cs/0602007) introduced secure sketches for this purpose: public helper data that lets the holder of a nearby reading recover the original exactly, while revealing as little as possible about it.

When the input is a set of features, the natural distance is the size of the symmetric difference. Juels and Sudan proposed the fuzzy vault for this setting (Des. Codes Cryptogr. 38, 2006). Section 6.2 of Dodis et al. gives a simpler, deterministic variant, the improved Juels–Sudan sketch (Construction 5), whose storage and entropy loss are both tlog⁡nt\log ntlogn for sss-element subsets of an nnn-element universe, independent of sss. The paper's Theorem 6.1 is the analysis of that construction. This mission formalizes it.

Setting

Laws and average min-entropy. A random variable is identified with its law. For a pair (A,B)(A,B)(A,B),

H~∞(A∣B)=−log⁡2∑bmax⁡aPr⁡[A=a∧B=b],\tilde H_\infty(A\mid B) = -\log_2 \sum_b \max_a \Pr[A=a \wedge B=b],H~∞​(A∣B)=−log2​b∑​amax​Pr[A=a∧B=b],

which equals −log⁡2Eb←B[max⁡aPr⁡[A=a∣B=b]]-\log_2 \mathbb E_{b\leftarrow B}\big[\max_a\Pr[A=a\mid B=b]\big]−log2​Eb←B​[maxa​Pr[A=a∣B=b]], the average min-entropy of §2.4: the negative logarithm of the best probability of guessing AAA after seeing BBB.

Secure sketches. Let M\mathcal MM be a set with an integer-valued distance dis\mathrm{dis}dis. A pair of procedures (SS,Rec)(\mathsf{SS},\mathsf{Rec})(SS,Rec) is an average-case (M,m,m~,t)(\mathcal M,m,\tilde m,t)(M,m,m~,t)-secure sketch (Definitions 3 and 4) if

  1. (correctness) dis(w,w′)≤t\mathrm{dis}(w,w')\le tdis(w,w′)≤t implies Rec(w′,SS(w))=w\mathsf{Rec}(w',\mathsf{SS}(w))=wRec(w′,SS(w))=w;
  2. (security) for all random variables WWW over M\mathcal MM and III with H~∞(W∣I)≥m\tilde H_\infty(W\mid I)\ge mH~∞​(W∣I)≥m, one has H~∞(W∣(SS(W),I))≥m~\tilde H_\infty(W\mid (\mathsf{SS}(W),I))\ge\tilde mH~∞​(W∣(SS(W),I))≥m~.

The difference m−m~m-\tilde mm−m~ is the entropy loss.

The metric. For a finite universe U\mathcal UU with n=∣U∣n=|\mathcal U|n=∣U∣, SDifs(U)\mathrm{SDif}_s(\mathcal U)SDifs​(U) is the set of sss-element subsets of U\mathcal UU with dis(w,w′)=∣w△w′∣\mathrm{dis}(w,w')=|w\triangle w'|dis(w,w′)=∣w△w′∣.

Construction 5. Identify U\mathcal UU with a finite field F\mathcal FF of nnn elements and let t≤st\le st≤s.

  • SS(w)\mathsf{SS}(w)SS(w): form p′(z)=∏x∈w(z−x)p'(z)=\prod_{x\in w}(z-x)p′(z)=∏x∈w​(z−x), monic of degree sss, and output its coefficients as−1,…,as−ta_{s-1},\dots,a_{s-t}as−1​,…,as−t​ of degree s−1s-1s−1 down to s−ts-ts−t.
  • Rec(w′,(as−1,…,as−t))\mathsf{Rec}(w',(a_{s-1},\dots,a_{s-t}))Rec(w′,(as−1​,…,as−t​)): form phigh(z)=zs+∑i=s−ts−1aizip_{\mathrm{high}}(z)=z^s+\sum_{i=s-t}^{s-1}a_iz^iphigh​(z)=zs+∑i=s−ts−1​ai​zi; find a polynomial plowp_{\mathrm{low}}plow​ of degree at most s−t−1s-t-1s−t−1 that agrees with phighp_{\mathrm{high}}phigh​ on at least s−t/2s-t/2s−t/2 points of w′w'w′ (Reed–Solomon decoding); output the roots of phigh−plowp_{\mathrm{high}}-p_{\mathrm{low}}phigh​−plow​.

The Lean development names these charPoly, sketchCoeffs, sketch, pHigh, Step3Cond and recover, and the metric SDifS with distance sdifDist, in the namespace FuzzyExtractors.ImprovedJS.

Formalization targets

Goal: Theorem 6.1

For every finite field F\mathcal FF with nnn elements, all t≤st\le st≤s and every real mmm,

(SS,Rec) is an average-case (SDifs(F), m, m−tlog⁡2n, t)-secure sketch.(\mathsf{SS},\mathsf{Rec})\ \text{is an average-case}\ \big(\mathrm{SDif}_s(\mathcal F),\,m,\,m-t\log_2 n,\,t\big)\text{-secure sketch}.(SS,Rec) is an average-case (SDifs​(F),m,m−tlog2​n,t)-secure sketch.

The goal is uniform in mmm: the entropy loss tlog⁡nt\log ntlogn does not depend on the input distribution.

Milestones (the correctness half)

The paper's argument on p. 21 splits into four steps, each a milestone:

  1. p′=phigh+qp'=p_{\mathrm{high}}+qp′=phigh​+q with deg⁡q≤s−t−1\deg q\le s-t-1degq≤s−t−1, and phigh=−qp_{\mathrm{high}}=-qphigh​=−q on www;
  2. ∣w△w′∣≤t|w\triangle w'|\le t∣w△w′∣≤t implies ∣w∩w′∣≥s−t/2|w\cap w'|\ge s-t/2∣w∩w′∣≥s−t/2, so −q-q−q is a valid plowp_{\mathrm{low}}plow​;
  3. any two valid plowp_{\mathrm{low}}plow​ coincide;
  4. Rec(w′,SS(w))=w\mathsf{Rec}(w',\mathsf{SS}(w))=wRec(w′,SS(w))=w whenever ∣w△w′∣≤t|w\triangle w'|\le t∣w△w′∣≤t.

A fifth, off the goal's path, records Step 2's remark that the sketch consists of the first ttt elementary symmetric polynomials of www, up to sign.

The security half is the entropy bound: since SS\mathsf{SS}SS takes at most ntn^tnt values, H~∞(W∣(SS(W),I))≥H~∞(W∣I)−tlog⁡n\tilde H_\infty(W\mid(\mathsf{SS}(W),I))\ge\tilde H_\infty(W\mid I)-t\log nH~∞​(W∣(SS(W),I))≥H~∞​(W∣I)−tlogn (the paper cites its Lemma 3.1, which is posed in the first mission of this series and is not restated here).

Significance

The result. Theorem 6.1 gives a secure sketch for set difference whose sketch length and entropy loss are tlog⁡nt\log ntlogn, which the paper shows is essentially optimal when n≫sn\gg sn≫s (§6.2, via Lemma C.1 and a constant-weight code bound). It improves the original fuzzy vault, whose entropy loss the paper analyses in Appendix D and finds good only when the stored data is very large. Through the paper's generic composition with randomness extractors (Lemma 4.1), it yields fuzzy extractors for set-valued inputs in large universes, the regime of biometric feature sets.

Formalizing it. The theorem is proved in the paper; no machine-checked version exists on Prove2Me or, to our knowledge, elsewhere. A formal proof combines three pieces of reusable infrastructure: a probabilistic layer (average min-entropy of laws on arbitrary types, and the chain-rule-type bound for a function with few values), the combinatorics of symmetric differences of equal-size sets, and the algebra of Reed–Solomon unique decoding (a low-degree polynomial is determined by its values on enough points). Each of these is useful beyond this mission.

Difficulty

No step is deep; the difficulty is in the bookkeeping. The correctness argument relies on exact degree accounting: phighp_{\mathrm{high}}phigh​ must agree with p′p'p′ in every coefficient of degree at least s−ts-ts−t, so that the remainder has degree at most s−t−1s-t-1s−t−1, and the uniqueness count ("two candidates agree on at least s−ts-ts−t points") requires the threshold to be at least s−t/2s-t/2s−t/2; the paper's sentence says "more than", which does not support the argument as written. The roots of phigh−plowp_{\mathrm{high}}-p_{\mathrm{low}}phigh​−plow​ must be shown to form exactly the set www, with no multiplicities lost. The security half needs the average min-entropy of a joint law with a deterministic, ntn^tnt-valued component bounded uniformly over all auxiliary variables, including those with infinite or uncountable range, where sums are infinite sums of extended nonnegative reals.

Formalization scope

Conventions committed to in Lean:

  • Laws are PMFs; the procedures are kernels M → PMF S, here deterministic (PMF.pure). Average min-entropy is the joint form above, logarithms base 2, and the auxiliary III ranges over an arbitrary ι : Type (a superset of the paper's {0,1}∗\{0,1\}^*{0,1}∗), never restricted to finite types.
  • The universe is the field F\mathcal FF itself, [Field 𝔽] [Fintype 𝔽], with nnn = Fintype.card 𝔽; the paper's "nnn is a prime power" is then automatic.
  • The paper leaves t≤st\le st≤s implicit; every statement assumes it. No parity condition on ttt is imposed: "at least s−t/2s-t/2s−t/2" is written 2⋅#≥2s−t2\cdot\#\ge 2s-t2⋅#≥2s−t in N\mathbb NN, which covers odd ttt.
  • "Degree at most s−t−1s-t-1s−t−1" is degree < s - t, so plow=0p_{\mathrm{low}}=0plow​=0 when t=st=st=s.
  • The sketch is a vector in Ft\mathcal F^tFt indexed from 000: entry iii is the coefficient of degree s−1−is-1-is−1−i. The storage bound tlog⁡nt\log ntlogn holds by this type and is not restated.
  • Rec\mathsf{Rec}Rec takes an arbitrary valid plowp_{\mathrm{low}}plow​ (by choice) instead of running a decoding algorithm. The paper's "fail" output is encoded as returning w′w'w′, which only occurs when correctness makes no claim.
  • Running time is out of scope. Theorem 6.1's clause that SS\mathsf{SS}SS and Rec\mathsf{Rec}Rec run in time polynomial in sss, ttt and log⁡n\log nlogn is dropped, and no surrogate predicate replaces it.

A formalization that checks only correctness, drops or trivializes the entropy clause, or lets Rec\mathsf{Rec}Rec see www itself, would not be Theorem 6.1. The goal states both clauses through the definition of an average-case secure sketch, with Rec\mathsf{Rec}Rec given only w′w'w′ and the sketch.

Contributions welcome: proofs of the milestones, a general lemma bounding average min-entropy loss by the logarithm of the number of sketch values (the paper's Lemma 2.2(b) and Lemma 3.1), and Reed–Solomon uniqueness lemmas stated for reuse.

Selected references

  • Y. Dodis, R. Ostrovsky, L. Reyzin, A. Smith, Fuzzy Extractors: How to Generate Strong Keys from Biometrics and Other Noisy Data, SIAM J. Comput. 38(1):97–139, 2008. https://doi.org/10.1137/060651380 ; arXiv:cs/0602007v4, https://arxiv.org/abs/cs/0602007
  • A. Juels, M. Sudan, A Fuzzy Vault Scheme, Designs, Codes and Cryptography 38(2):237–257, 2006. https://doi.org/10.1007/s10623-005-6343-z
  • E. Agrell, A. Vardy, K. Zeger, Upper Bounds for Constant-Weight Codes, IEEE Trans. Inform. Theory 46(7):2373–2395, 2000. https://doi.org/10.1109/18.887851
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ProbabilityTheoretical Computer Science·Captain: mikedeng1

Fuzzy Extractors: How to Generate Strong Keys from Biometrics and Other Noisy Data 1: Every [n, k, 2t+1] Code Gives an Average-Case Hamming Fuzzy Extractor with ℓ = m + kf − nf − 2 log(1/ε) + 2Research Paper

Motivation

Cryptographic keys must be uniformly random and reproducible exactly. Many secrets people actually possess are neither: a biometric reading (an iris code, a fingerprint template), a long passphrase recalled with typos, or the correlated bits two parties obtain from a quantum channel are noisy, so two readings of the same secret differ in a few positions, and they are not uniform. Fuzzy extractors, introduced by Dodis, Ostrovsky, Reyzin and Smith (arXiv:cs/0602007; SIAM J. Comput. 38(1), 2008), turn such a secret into a nearly uniform key that can be regenerated from any sufficiently close reading, using public helper data that does not compromise the key.

The construction for the Hamming metric is the one most used in practice and in later work on biometric key derivation and physically unclonable functions. Its history is short. Juels and Wattenberg's fuzzy commitment (CCS 1999) shifted an error-correcting code onto the secret but was analysed only for uniform inputs. The syndrome of a linear code had been used for information reconciliation in quantum key agreement (Bennett, Bessette, Brassard, Salvail and Smolin, J. Cryptology 1992). Dodis et al. defined secure sketches and fuzzy extractors for arbitrary entropy distributions, introduced average min-entropy to handle side information, and proved the bound formalized here. This mission is the first of four drawn from that paper.

Setting

All logarithms are base 2. A random variable is identified with its law. For a random variable AAA, the min-entropy is H∞(A)=−log⁡max⁡aPr⁡[A=a]\mathbf H_\infty(A) = -\log \max_a \Pr[A=a]H∞​(A)=−logmaxa​Pr[A=a]. For a pair (A,B)(A,B)(A,B), the average min-entropy of AAA given BBB is

H~∞(A∣B)=−log⁡Eb←B[max⁡aPr⁡[A=a∣B=b]],\tilde{\mathbf H}_\infty(A\mid B) = -\log \mathbb E_{b\leftarrow B}\big[\max_a \Pr[A=a\mid B=b]\big],H~∞​(A∣B)=−logEb←B​[amax​Pr[A=a∣B=b]],

the adversary's chance of guessing AAA after seeing BBB, on a log scale. The statistical distance is SD(A,B)=12∑v∣Pr⁡(A=v)−Pr⁡(B=v)∣\mathbf{SD}(A,B)=\tfrac12\sum_v|\Pr(A=v)-\Pr(B=v)|SD(A,B)=21​∑v​∣Pr(A=v)−Pr(B=v)∣, and UℓU_\ellUℓ​ is uniform on {0,1}ℓ\{0,1\}^\ell{0,1}ℓ.

The space is M=Fn\mathcal M=\mathcal F^nM=Fn, where F\mathcal FF is a finite additive group with FFF elements, f=log⁡Ff=\log Ff=logF, and dis(w,w′)\mathrm{dis}(w,w')dis(w,w′) is the Hamming distance, the number of positions where www and w′w'w′ differ. A code C⊆FnC\subseteq\mathcal F^nC⊆Fn with KKK codewords is an [n,k,2t+1]F[n,k,2t+1]_{\mathcal F}[n,k,2t+1]F​ code if distinct codewords are at distance at least 2t+12t+12t+1; its dimension is k=log⁡FKk=\log_F Kk=logF​K, so kf=log⁡Kkf=\log Kkf=logK.

A secure sketch (SS,Rec)(\mathsf{SS},\mathsf{Rec})(SS,Rec) is a pair of randomized procedures with Rec(w′,SS(w))=w\mathsf{Rec}(w',\mathsf{SS}(w))=wRec(w′,SS(w))=w whenever dis(w,w′)≤t\mathrm{dis}(w,w')\le tdis(w,w′)≤t. It is an average-case (M,m,m~,t)(\mathcal M,m,\tilde m,t)(M,m,m~,t)-secure sketch if H~∞(W∣(SS(W),I))≥m~\tilde{\mathbf H}_\infty(W\mid(\mathsf{SS}(W),I))\ge\tilde mH~∞​(W∣(SS(W),I))≥m~ for every pair (W,I)(W,I)(W,I) with H~∞(W∣I)≥m\tilde{\mathbf H}_\infty(W\mid I)\ge mH~∞​(W∣I)≥m. A fuzzy extractor (Gen,Rep)(\mathsf{Gen},\mathsf{Rep})(Gen,Rep) has Gen(w)=(R,P)\mathsf{Gen}(w)=(R,P)Gen(w)=(R,P) with R∈{0,1}ℓR\in\{0,1\}^\ellR∈{0,1}ℓ, and Rep(w′,P)=R\mathsf{Rep}(w',P)=RRep(w′,P)=R whenever dis(w,w′)≤t\mathrm{dis}(w,w')\le tdis(w,w′)≤t. It is an average-case (M,m,ℓ,t,ε)(\mathcal M,m,\ell,t,\varepsilon)(M,m,ℓ,t,ε)-fuzzy extractor if

SD((R,P,I),(Uℓ,P,I))≤εwheneverH~∞(W∣I)≥m.\mathbf{SD}\big((R,P,I),(U_\ell,P,I)\big)\le\varepsilon \quad\text{whenever}\quad \tilde{\mathbf H}_\infty(W\mid I)\ge m .SD((R,P,I),(Uℓ​,P,I))≤εwheneverH~∞​(W∣I)≥m.

A family {Hx}x∈X\{H_x\}_{x\in X}{Hx​}x∈X​ of functions into {0,1}ℓ\{0,1\}^\ell{0,1}ℓ is universal if Pr⁡x[Hx(a)=Hx(b)]=2−ℓ\Pr_{x}[H_x(a)=H_x(b)]=2^{-\ell}Prx​[Hx​(a)=Hx​(b)]=2−ℓ for all a≠ba\ne ba=b.

Formalization targets

Goal: Theorem 5.2 (p. 17)

For every [n,k,2t+1]F[n,k,2t+1]_{\mathcal F}[n,k,2t+1]F​ code, every mmm, every ε>0\varepsilon>0ε>0 and every natural number

ℓ  ≤  m+kf−nf−2log⁡(1/ε)+2,\ell\;\le\;m+kf-nf-2\log(1/\varepsilon)+2,ℓ≤m+kf−nf−2log(1/ε)+2,

there is an average-case (Fn,m,ℓ,t,ε)(\mathcal F^n,m,\ell,t,\varepsilon)(Fn,m,ℓ,t,ε)-fuzzy extractor.

The sketch branch

  • Lemma 2.2(b): publishing a value with at most 2λ2^\lambda2λ possibilities lowers average min-entropy by at most λ\lambdaλ.
  • Lemma 3.1: a correct sketch with at most 2λ2^\lambda2λ outputs is an average-case secure sketch with entropy loss λ\lambdaλ.
  • Lemma 4.5: the sketch for transitive metric spaces (Construction 1) loses at most log⁡∣Π∣−log⁡Γ−log⁡K\log|\Pi|-\log\Gamma-\log Klog∣Π∣−logΓ−logK.
  • §5, p. 17: at most one word within distance ttt of w′w'w′ has a given syndrome.
  • Theorem 5.1: the code-offset sketch is an average-case (Fn,m,m−(n−k)f,t)(\mathcal F^n,m,m-(n-k)f,t)(Fn,m,m−(n−k)f,t)-secure sketch; for a linear code, the syndrome sketch is deterministic, n−kn-kn−k symbols long, with the same loss.

The extractor branch

  • Lemma 2.1 and Lemma 2.4: the leftover hash lemma and its average-case generalization, SD((HX(W),X,I),(Uℓ,X,I))≤122−H~∞(W∣I)2ℓ\mathbf{SD}\big((H_X(W),X,I),(U_\ell,X,I)\big)\le\frac12\sqrt{2^{-\tilde{\mathbf H}_\infty(W\mid I)}2^\ell}SD((HX​(W),X,I),(Uℓ​,X,I))≤21​2−H~∞​(W∣I)2ℓ​.
  • Lemma 4.1 (average-case form): an average-case sketch plus an average-case strong extractor gives an average-case fuzzy extractor.
  • Lemma 4.3 (average-case form): with universal hashing, any ℓ≤m~−2log⁡(1/ε)+2\ell\le\tilde m-2\log(1/\varepsilon)+2ℓ≤m~−2log(1/ε)+2 is achievable.

Significance

Theorem 5.2 says that the only costs of tolerating ttt Hamming errors are the redundancy of the code, (n−k)f(n-k)f(n−k)f bits, and the 2log⁡(1/ε)2\log(1/\varepsilon)2log(1/ε) bits that any extractor loses. Appendix C of the paper shows the redundancy term cannot be avoided for uniform inputs, so for optimal codes the construction is optimal there. The average-case form matters for composition: it remains valid when the adversary holds side information correlated with the secret, which is the situation of every protocol that uses the key afterwards or reuses the reading.

Formalizing it produces machine-checked versions of the leftover hash lemma in its average-case form, the basic calculus of average min-entropy, and the code-offset and syndrome sketches. These are the standard tools of information-theoretic cryptography, used well beyond fuzzy extraction (privacy amplification, randomness extraction, information reconciliation). All results are proved in the paper; as far as is known, none of them has a formal proof in Lean or on this platform.

Difficulty

The obvious route bounds the leakage of the sketch with min-entropy and then applies an extractor to WWW conditioned on each sketch value. That fails: conditioned on a particular sketch value, WWW may have far less min-entropy than average, so a worst-case extractor has nothing to work with on some values, and paying for those bad values costs an extra error term (Corollary 4.2). The average-case notions exist to avoid this loss, and the chain must be kept average-case at every step. In Lean the work is in the probability bookkeeping: computing laws of pairs and triples formed by independent coin flips, rearranging them, and bounding sums of maxima over possibly infinite auxiliary types, together with the leftover hash lemma itself, which Mathlib does not provide.

Formalization scope

Random variables are their laws, Mathlib PMFs; pairs are joint laws and randomized procedures are kernels whose coins are independent of everything else. Average min-entropy is written in the equivalent joint form −log⁡∑bmax⁡aPr⁡[A=a∧B=b]-\log\sum_b\max_a\Pr[A=a\wedge B=b]−log∑b​maxa​Pr[A=a∧B=b], which needs no conditioning on null events. The auxiliary variable III ranges over every type, not only finite ones. Logarithms are Real.logb 2; {0,1}ℓ\{0,1\}^\ell{0,1}ℓ is Fin ℓ → Bool; Fn\mathcal F^nFn is Fin n → F with Mathlib's hammingDist.

Explicit choices:

  • Efficiency is dropped. Every "efficient" and polynomial-time clause (Definitions 1–5, Lemma 4.5, Theorems 5.1 and 5.2) is omitted; there is no complexity substrate, and no vacuous predicate stands in for it.
  • ℓ\ellℓ is a natural number with ℓ≤m+kf−nf−2log⁡(1/ε)+2\ell\le m+kf-nf-2\log(1/\varepsilon)+2ℓ≤m+kf−nf−2log(1/ε)+2 as a real inequality; the printed ℓ\ellℓ is a real expression.
  • ε>0\varepsilon>0ε>0 is stated wherever log⁡(1/ε)\log(1/\varepsilon)log(1/ε) appears.
  • "Min-entropy mmm" means H∞(W)≥m\mathbf H_\infty(W)\ge mH∞​(W)≥m; minimum distance 2t+12t+12t+1 means at least 2t+12t+12t+1; kf=log⁡Kkf=\log Kkf=logK, so non-linear codes are covered.
  • F\mathcal FF is any finite additive commutative group (the paper's additive cyclic group is a special case); the syndrome is any linear map onto Fn−k\mathcal F^{n-k}Fn−k with kernel CCC.
  • Extractor domains are arbitrary finite sets with arbitrary finite nonempty seed sets, instead of {0,1}n\{0,1\}^n{0,1}n and {0,1}r\{0,1\}^r{0,1}r.
  • Γ\GammaΓ in Lemma 4.5 is read as "for each www and bbb there are at least Γ≥1\Gamma\ge1Γ≥1 permutations with π(w)=b\pi(w)=bπ(w)=b"; symmetry of the distance is an explicit hypothesis there.
  • Theorem 5.1 is stated for the code-offset and syndrome constructions themselves, not as a bare existence claim.

A trivializing formalization is ruled out: the security clause quantifies over every auxiliary type and every joint law meeting the entropy bound, ε\varepsilonε and ℓ\ellℓ are constrained exactly as in the paper, and the universal hash family is constructed inside the goal (a supporting item states that universal families exist), never assumed.

Contributions welcome: proofs of any milestone; general lemmas on PMF marginals, statistical distance and average min-entropy, which are reusable across all four missions of this paper and in other information-theoretic cryptography; and the leftover hash lemma as a standalone result.

Selected references

  • Y. Dodis, R. Ostrovsky, L. Reyzin, A. Smith, Fuzzy Extractors: How to Generate Strong Keys from Biometrics and Other Noisy Data, SIAM J. Comput. 38(1):97–139, 2008. arXiv:cs/0602007v4. https://arxiv.org/abs/cs/0602007 , https://doi.org/10.1137/060651380
  • A. Juels, M. Wattenberg, A Fuzzy Commitment Scheme, ACM CCS 1999. https://doi.org/10.1145/319709.319714
  • J. L. Carter, M. N. Wegman, Universal Classes of Hash Functions, J. Comput. System Sci. 18(2):143–154, 1979. https://doi.org/10.1016/0022-0000(79)90044-8
  • J. Håstad, R. Impagliazzo, L. Levin, M. Luby, A Pseudorandom Generator from any One-way Function, SIAM J. Comput. 28(4):1364–1396, 1999. https://doi.org/10.1137/S0097539793244708
  • C. H. Bennett, F. Bessette, G. Brassard, L. Salvail, J. Smolin, Experimental Quantum Cryptography, J. Cryptology 5(1):3–28, 1992. https://doi.org/10.1007/BF00191318
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OptimizationProbabilityStatistics·Captain: mikedeng1

I-Divergence Geometry of Probability Distributions and Minimization Problems 1: Cyclic I-Projections onto Linear Sets of a Finite Space Converge to the I-Projection onto Their IntersectionResearch Paper

Motivation

Fitting a probability distribution to prescribed margins or moments is a basic task in statistics and information theory. Starting from a reference distribution, one can enforce one constraint at a time by choosing the closest distribution in I-divergence, then cycle through the constraints. In a contingency table this procedure is iterative proportional fitting. A single projection onto the intersection is the desired answer, but each step of the iteration sees only one constraint set. Csiszár's 1975 paper proves that cyclic I-projections converge to the joint I-projection when the underlying set is finite and the constraint sets are linear. This mission formalizes that result together with the geometric statements needed to identify its limit.

Setting

Let (X,X)(X,\mathcal X)(X,X) be a measurable space. A probability distribution (PD) is a probability measure on it. For PDs PPP and QQQ, the I-divergence I(P∥Q)I(P\|Q)I(P∥Q) is the Kullback–Leibler divergence: integrate the logarithm of the density of PPP relative to QQQ against PPP, with value +∞+\infty+∞ when PPP is not absolutely continuous with respect to QQQ or the integral diverges. It takes values in [0,+∞][0,+\infty][0,+∞] and vanishes exactly when P=QP=QP=Q. The logarithmic conventions are log⁡0=−∞\log0=-\inftylog0=−∞ and 0⋅(±∞)=00\cdot(\pm\infty)=00⋅(±∞)=0 (Csiszár 1975, (1.1)–(1.3)).

Given a PD RRR and a set E\mathcal EE of PDs that contains at least one PPP with finite I(P∥R)I(P\|R)I(P∥R), an I-projection QQQ of RRR onto E\mathcal EE minimizes I(P∥R)I(P\|R)I(P∥R) over P∈EP\in\mathcal EP∈E and itself has finite divergence. The variation distance is the L1L^1L1 distance between the densities of two PDs relative to a common dominating measure. A set of PDs is linear here when every real affine combination of two members that is still a PD also belongs to the set. This includes distributions satisfying fixed linear moment constraints (Csiszár 1975, pp. 147 and 150–151).

For the goal, XXX is finite. Choose k≥1k\ge1k≥1 linear sets E1,…,Ek\mathcal E_1,\ldots,\mathcal E_kE1​,…,Ek​, and write E=⋂i=1kEi\mathcal E=\bigcap_{i=1}^k\mathcal E_iE=⋂i=1k​Ei​. Beginning with Q0=RQ_0=RQ0​=R, let QnQ_nQn​ be the I-projection of Qn−1Q_{n-1}Qn−1​ onto Ei\mathcal E_iEi​ when n=mk+in=mk+in=mk+i and 1≤i≤k1\le i\le k1≤i≤k. The common feasible set is assumed nonempty and contains a PD absolutely continuous with respect to RRR. These assumptions ensure that the intended finite-divergence projection problem is present (Csiszár 1975, Theorem 3.2).

Formalization targets

The goal is the convergence statement of Theorem 3.2:

∀x∈X,Qn({x})⟶Q({x}),Q=proj⁡EI(R).\forall x\in X,\qquad Q_n(\{x\})\longrightarrow Q(\{x\}), \quad Q=\operatorname{proj}^{I}_{\mathcal E}(R).∀x∈X,Qn​({x})⟶Q({x}),Q=projEI​(R).

The goal also asserts existence of the cyclic sequence. On finite XXX, convergence of every point mass is equivalent to convergence in variation distance. The target fixes no rate. Its milestones include existence on variation-closed convex sets (Theorem 2.1), the identity (2.6) and the tangent-hyperplane Lemma 2.1, the Pythagorean characterization and transitivity of I-projections (Theorems 2.2–2.3), the density form under general linear constraints (Theorem 3.1) and the finite-moment exponential-density characterization (Corollary 3.1(A)), and the finite-space identity used in Theorem 3.2's proof. The two displayed identities in that proof are also targets:

I(Q∥R)=I(Q∥Qn)+∑i=1nI(Qi∥Qi−1),I(P∥Qn)=I(P∥Q)+I(Q∥Qn)(P∈E).I(Q\|R)=I(Q\|Q_n)+\sum_{i=1}^{n}I(Q_i\|Q_{i-1}),\qquad I(P\|Q_n)=I(P\|Q)+I(Q\|Q_n)\quad(P\in\mathcal E).I(Q∥R)=I(Q∥Qn​)+i=1∑n​I(Qi​∥Qi−1​),I(P∥Qn​)=I(P∥Q)+I(Q∥Qn​)(P∈E).

They specify the divergence relationships that the eventual convergence theorem must preserve (Csiszár 1975, (3.14)–(3.15)).

Significance

The theorem justifies enforcing finitely many linear distribution constraints one at a time while still obtaining the same I-projection as a simultaneous minimization. It gives a precise limit for the iterative proportional fitting procedure discussed by Csiszár, including cases in which the initial distribution has zero probabilities; strict positivity of RRR is not required (Csiszár 1975, p. 155). The accompanying identities make the relation between a partial iterate and the final solution explicit. The result was proved in 1975. The work here is to provide machine-checked proofs of that known result and its supporting geometry, while keeping the source's extended-value and boundary conventions visible.

Difficulty

Successive projections minimize divergence over different sets. Minimization for one set by itself does not identify the minimizer over their intersection, and ordinary metric projection facts do not directly apply because I-divergence is asymmetric and can be infinite. The paper's statements need to handle zero densities and feasible distributions at infinite divergence without turning extended-real expressions into default values. On the finite space, convergence of a subsequence is available, but the formal claim must still identify every possible limit as the joint I-projection. These are the mathematical and representation difficulties faced by a complete proof (Csiszár 1975, §§2–3).

Formalization scope

Lean uses Measure X and Mathlib's InformationTheory.klDiv : ℝ≥0∞ for I(P∥Q)I(P\|Q)I(P∥Q). A projection is a finite-divergence minimizer over the stated feasible set; no real-valued infimum or implicit arbitrary witness replaces it. Variation distance uses the densities relative to P+QP+QP+Q, which dominates both PDs and gives the value of (1.6). Variation closure is expressed by sequential convergence in this distance. The integral ∫log⁡qR dP\int\log q_R\,dP∫logqR​dP is represented in extended reals using positive and negative logarithmic parts and ENNReal.log; the theorem hypotheses keep the indeterminate +∞−(+∞)+\infty-(+\infty)+∞−(+∞) case out. Density equations are RRR-almost everywhere, and a claim that QQQ has an RRR-density explicitly includes Q≪RQ\ll RQ≪R.

For moment constraints, every integral is accompanied by integrability. Real affine combinations are tested through their values on measurable sets; the candidate combination must be a PD. The goal assumes a finite carrier with measurable singleton sets and k≥1k\ge1k≥1. Lean indexes the sets by Fin k from zero, so Qs (n+1) is projected onto the set at n % k; this is the paper's rule (3.13) shifted by one. The goal asserts existence of a recursive sequence before speaking about every such sequence, and the required feasible witness has P≪RP\ll RP≪R. These choices rule out an empty cyclic schedule, junk integrals, and a vacuous convergence assertion. Reusable contributions include the variation-distance and I-projection interfaces, their Pythagorean geometry, and the finite-moment density characterization; the mission's main closure remains Theorem 3.2.

Selected references

  • I. Csiszár, I-Divergence Geometry of Probability Distributions and Minimization Problems, The Annals of Probability 3(1), 146–158 (1975). DOI: 10.1214/aop/1176996454.
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Operations ResearchOptimizationProbability·Captain: mikedeng1

Worst-Case Value-At-Risk and Robust Portfolio Optimization: A Conic Programming Approach 2: Closed Form of the Entropy-Constrained Worst-Case VaRResearch Paper

Motivation

Value-at-Risk (VaR) is the loss level that a portfolio exceeds with probability at most ε\varepsilonε. It is the standard risk measure of banking regulation, and its classical computation assumes Gaussian returns: for a Gaussian return vector with mean x^\hat xx^ and covariance Γ\GammaΓ it equals −Φ−1(ε)w⊤Γw−x^⊤w-\Phi^{-1}(\varepsilon)\sqrt{w^\top\Gamma w} - \hat x^\top w−Φ−1(ε)w⊤Γw​−x^⊤w, where Φ\PhiΦ is the standard normal distribution function. Real returns are not exactly Gaussian, and a VaR computed from a misspecified distribution can badly understate risk.

El Ghaoui, Oks and Oustry (Oper. Res. 51(4), 2003) replace the single distribution by a class P\mathcal PP of distributions and define the worst-case VaR as the smallest loss level whose probability is at most ε\varepsilonε under every distribution of the class. Their first class, distributions with a given mean and covariance, leads to the Chebyshev-type bound of their Theorem 1, whose worst case is attained by discrete distributions. §4.2 of the paper asks instead for distributions that stay close to a Gaussian, measured by relative entropy (Kullback–Leibler divergence). Such balls are the basic uncertainty sets of distributionally robust optimization and of robust control in economics (Hansen and Sargent's multiplier and constraint preferences), and they give a smooth worst case. Theorem 9 computes the resulting worst-case VaR in closed form.

Setting

Returns are random vectors x∈Rnx \in \mathbb R^nx∈Rn and a portfolio is a vector w∈Rnw \in \mathbb R^nw∈Rn with w≠0w \neq 0w=0; its return is r(w,x)=w⊤xr(w,x) = w^\top xr(w,x)=w⊤x. For a level γ∈R\gamma \in \mathbb Rγ∈R the loss set is Sγ={x:γ≤−x⊤w}\mathcal S_\gamma = \{x : \gamma \le -x^\top w\}Sγ​={x:γ≤−x⊤w} (Eq. 13 of the paper).

Given a class P\mathcal PP of probability distributions on Rn\mathbb R^nRn and ε∈(0,1)\varepsilon \in (0,1)ε∈(0,1), the worst-case Value-at-Risk (Eq. 4) is

VP(w)=min⁡{γ∈R:sup⁡P∈PP(Sγ)≤ε}.V_{\mathcal P}(w) = \min\Big\{\gamma \in \mathbb R : \sup_{P \in \mathcal P} P(\mathcal S_\gamma) \le \varepsilon\Big\}.VP​(w)=min{γ∈R:P∈Psup​P(Sγ​)≤ε}.

Fix a mean x^∈Rn\hat x \in \mathbb R^nx^∈Rn and a positive definite covariance Γ≻0\Gamma \succ 0Γ≻0, and let P0=N(x^,Γ)P_0 = \mathcal N(\hat x, \Gamma)P0​=N(x^,Γ) be the reference Gaussian. For d≥0d \ge 0d≥0 the relative-entropy class (Eq. 43) is

Pd={P probability on Rn:KL(P,P0)=∫log⁡dPdP0 dP≤d},\mathcal P_d = \Big\{P \text{ probability on } \mathbb R^n : \mathrm{KL}(P, P_0) = \int \log\frac{dP}{dP_0}\,dP \le d\Big\},Pd​={P probability on Rn:KL(P,P0​)=∫logdP0​dP​dP≤d},

with KL(P,P0)=+∞\mathrm{KL}(P,P_0) = +\inftyKL(P,P0​)=+∞ unless PPP is absolutely continuous with respect to P0P_0P0​.

The risk factor (Eq. 45) is

f(ε,d)=sup⁡λ>0eε/λ−d−1e1/λ−1,κ(ε,d)=−Φ−1(f(ε,d)),f(\varepsilon,d) = \sup_{\lambda>0}\frac{e^{\varepsilon/\lambda - d} - 1}{e^{1/\lambda} - 1}, \qquad \kappa(\varepsilon,d) = -\Phi^{-1}\big(f(\varepsilon,d)\big),f(ε,d)=λ>0sup​e1/λ−1eε/λ−d−1​,κ(ε,d)=−Φ−1(f(ε,d)),

and the Gaussian tail of the loss set is ϕ(γ)=P0(Sγ)=1−Φ((γ+w⊤x^)/w⊤Γw)\phi(\gamma) = P_0(\mathcal S_\gamma) = 1 - \Phi\big((\gamma + w^\top\hat x)/\sqrt{w^\top\Gamma w}\big)ϕ(γ)=P0​(Sγ​)=1−Φ((γ+w⊤x^)/w⊤Γw​).

Formalization targets

Goal: Theorem 9 (p. 553)

For Γ≻0\Gamma \succ 0Γ≻0, w≠0w \neq 0w=0, d≥0d \ge 0d≥0 and 0<ε<10 < \varepsilon < 10<ε<1, the minimum in (4) over Pd\mathcal P_dPd​ exists and

VPd(w)=κ(ε,d)w⊤Γw−x^⊤w.(44)V_{\mathcal P_d}(w) = \kappa(\varepsilon,d)\sqrt{w^\top\Gamma w} - \hat x^\top w. \tag{44}VPd​​(w)=κ(ε,d)w⊤Γw​−x^⊤w.(44)

Milestones

The milestones follow the proof of Theorem 9 on pp. 553–554, in attack order.

  1. Eq. (45). The two expressions of fff agree: sup⁡λ>0eε/λ−d−1e1/λ−1=sup⁡v>0e−d(v+1)ε−1v\sup_{\lambda>0}\frac{e^{\varepsilon/\lambda-d}-1}{e^{1/\lambda}-1} = \sup_{v>0}\frac{e^{-d}(v+1)^\varepsilon - 1}{v}supλ>0​e1/λ−1eε/λ−d−1​=supv>0​ve−d(v+1)ε−1​.
  2. Gaussian tail. P0(Sγ)=1−Φ((γ+w⊤x^)/w⊤Γw)P_0(\mathcal S_\gamma) = 1 - \Phi\big((\gamma + w^\top\hat x)/\sqrt{w^\top\Gamma w}\big)P0​(Sγ​)=1−Φ((γ+w⊤x^)/w⊤Γw​).
  3. Eq. (47). For λ>0\lambda > 0λ>0, the Lagrangian L(Q)=Q(Sγ)+λ0(1−Q(Rn))+λ(d−KL-integral)L(Q) = Q(\mathcal S_\gamma) + \lambda_0(1 - Q(\mathbb R^n)) + \lambda(d - \mathrm{KL}\text{-integral})L(Q)=Q(Sγ​)+λ0​(1−Q(Rn))+λ(d−KL-integral) is maximised over finite measures Q≪P0Q \ll P_0Q≪P0​ by the exponentially tilted density dQ⋆/dP0=exp⁡((χS−λ0)/λ−1)dQ^\star/dP_0 = \exp((\chi_{\mathcal S} - \lambda_0)/\lambda - 1)dQ⋆/dP0​=exp((χS​−λ0​)/λ−1), with value
θ(λ0,λ)=λ0+λd+λe−λ0/λ−1((e1/λ−1)ϕ(γ)+1).\theta(\lambda_0,\lambda) = \lambda_0 + \lambda d + \lambda e^{-\lambda_0/\lambda - 1}\big((e^{1/\lambda}-1)\phi(\gamma) + 1\big).θ(λ0​,λ)=λ0​+λd+λe−λ0​/λ−1((e1/λ−1)ϕ(γ)+1).
  1. Eq. (48). min⁡λ0∈Rθ(λ0,λ)=λd+λlog⁡((e1/λ−1)ϕ(γ)+1)\min_{\lambda_0\in\mathbb R}\theta(\lambda_0,\lambda) = \lambda d + \lambda\log\big((e^{1/\lambda}-1)\phi(\gamma)+1\big)minλ0​∈R​θ(λ0​,λ)=λd+λlog((e1/λ−1)ϕ(γ)+1).
  2. Duality. sup⁡P∈PdP(Sγ)=inf⁡λ>0(λd+λlog⁡((e1/λ−1)ϕ(γ)+1))\sup_{P\in\mathcal P_d} P(\mathcal S_\gamma) = \inf_{\lambda>0}\big(\lambda d + \lambda\log((e^{1/\lambda}-1)\phi(\gamma)+1)\big)supP∈Pd​​P(Sγ​)=infλ>0​(λd+λlog((e1/λ−1)ϕ(γ)+1)).
  3. Inversion. For d>0d > 0d>0: some λ>0\lambda > 0λ>0 makes the dual value at most ε\varepsilonε if and only if γ≥κ(ε,d)w⊤Γw−w⊤x^\gamma \ge \kappa(\varepsilon,d)\sqrt{w^\top\Gamma w} - w^\top\hat xγ≥κ(ε,d)w⊤Γw​−w⊤x^.
  4. Remark after Theorem 9. f(ε,0)=εf(\varepsilon, 0) = \varepsilonf(ε,0)=ε, so κ(ε,0)=−Φ−1(ε)\kappa(\varepsilon,0) = -\Phi^{-1}(\varepsilon)κ(ε,0)=−Φ−1(ε). The risk factor κ(ε,d)\kappa(\varepsilon, d)κ(ε,d) is strictly increasing in d≥0d \ge 0d≥0.

Significance

Theorem 9 says that an entropy ball around a Gaussian leaves the form of the Gaussian VaR unchanged: only the risk factor moves, from −Φ−1(ε)-\Phi^{-1}(\varepsilon)−Φ−1(ε) to κ(ε,d)\kappa(\varepsilon,d)κ(ε,d), a scalar computed by a one-dimensional maximisation. The worst-case VaR therefore stays a convex function of www whenever κ≥0\kappa \ge 0κ≥0, and minimising it over a polytope of portfolios is a second-order cone program (problem (3) of the paper). The number f(ε,d)f(\varepsilon,d)f(ε,d) is the largest ppp with KL(Bernoulli(ε) ∥ Bernoulli(p))≤d\mathrm{KL}(\mathrm{Bernoulli}(\varepsilon)\,\|\,\mathrm{Bernoulli}(p)) \le dKL(Bernoulli(ε)∥Bernoulli(p))≤d, which ties the result to the binary-divergence bounds used throughout information theory.

The theorem was proved in 2003. The worst-case-probability step (milestone 5) is an instance of the Donsker–Varadhan / Gibbs variational duality for relative-entropy balls, which the paper imports from the literature (Smith 1995). No machine-checked proof of Theorem 9 or of this duality on Rn\mathbb R^nRn is known. A formalization would give a verified closed form for a relative-entropy distributionally robust chance constraint, and the duality and tilting lemmas would serve any mission on KL-ball robust optimization.

Difficulty

The obvious argument is Lagrangian duality for the infinite-dimensional problem sup⁡{P(Sγ):KL(P,P0)≤d}\sup\{P(\mathcal S_\gamma) : \mathrm{KL}(P,P_0) \le d\}sup{P(Sγ​):KL(P,P0​)≤d}. Weak duality and the pointwise maximisation that produces the tilted density are elementary. The difficulty is the step the paper cites rather than proves: that the duality gap is zero, and that the supremum over distributions equals the infimum of the dual over λ>0\lambda > 0λ>0. The feasible set is a set of measures, the objective is an indicator, and the constraint is a divergence that is +∞+\infty+∞ off a set of absolutely continuous measures, so a finite-dimensional Slater argument does not apply as stated.

The second difficulty is at the boundary of the parameters. At d=0d = 0d=0 the supremum defining f(ε,0)f(\varepsilon,0)f(ε,0) is approached only as λ→∞\lambda \to \inftyλ→∞, so the final inversion step behaves differently from d>0d > 0d>0. At ε=1\varepsilon = 1ε=1 the theorem is false, since every level γ\gammaγ is feasible and (4) has no minimum.

Formalization scope

Returns live in EuclideanSpace ℝ (Fin n). P0P_0P0​ is Mathlib's multivariateGaussian xhat Γ with Γ.PosDef, and KL\mathrm{KL}KL is InformationTheory.klDiv, which is ∞\infty∞ unless P≪P0P \ll P_0P≪P0​ with integrable log-likelihood ratio and equals ∫log⁡dPdP0 dP\int\log\frac{dP}{dP_0}\,dP∫logdP0​dP​dP otherwise for probability measures. The class Pd\mathcal P_dPd​ requires IsProbabilityMeasure P. Φ\PhiΦ is cdf (gaussianReal 0 1), and Φ−1(p)\Phi^{-1}(p)Φ−1(p) is defined as inf⁡{t:p≤Φ(t)}\inf\{t : p \le \Phi(t)\}inf{t:p≤Φ(t)}, which inverts Φ\PhiΦ on (0,1)(0,1)(0,1). The quadratic form w⊤Γww^\top\Gamma ww⊤Γw is a double sum, and ∥Γ1/2w∥2\|\Gamma^{1/2}w\|_2∥Γ1/2w∥2​ is written w⊤Γw\sqrt{w^\top\Gamma w}w⊤Γw​.

Conventions the Lean statements commit to:

  • "min" in (4) is IsLeast of the feasible set {γ:P(Sγ)≤ε ∀P∈Pd}\{\gamma : P(\mathcal S_\gamma) \le \varepsilon \ \forall P \in \mathcal P_d\}{γ:P(Sγ​)≤ε ∀P∈Pd​}. "sup⁡PP(Sγ)≤ε\sup_{P}P(\mathcal S_\gamma) \le \varepsilonsupP​P(Sγ​)≤ε" is written "for every PPP", with probabilities compared in [0,∞][0,\infty][0,∞].
  • The paper prints ε∈(0,1]\varepsilon \in (0,1]ε∈(0,1]. The mission assumes 0<ε<10 < \varepsilon < 10<ε<1, because the goal is false at ε=1\varepsilon = 1ε=1.
  • w≠0w \neq 0w=0 is the paper's assumption that the admissible set of portfolios excludes 000.
  • f(ε,d)f(\varepsilon,d)f(ε,d) is a Lean sSup of a set that is nonempty and bounded above by 111 for ε≤1\varepsilon \le 1ε≤1, d≥0d \ge 0d≥0.
  • The duality of milestone 5 is stated as the existence of one real number that is both the least upper bound of the worst-case probabilities and the greatest lower bound of the dual values, not as an equality of Lean's sSup and sInf.
  • Eq. (48) is stated as an attained minimum (IsLeast), which the calculus gives.
  • Milestone 3 works with finite measures Q≪P0Q \ll P_0Q≪P0​ with integrable log-likelihood ratio in place of the paper's densities ppp. It uses the complement of Sγ\mathcal S_\gammaSγ​ where the paper writes {γ≥−x⊤w}\{\gamma \ge -x^\top w\}{γ≥−x⊤w}, which differs by a P0P_0P0​-null hyperplane.
  • Milestone 6 assumes d>0d > 0d>0; the goal keeps d≥0d \ge 0d≥0.

Restricting Pd\mathcal P_dPd​ to {P0}\{P_0\}{P0​}, dropping IsProbabilityMeasure, or taking an arbitrary reference measure would trivialize or change the theorem. The class is the full KL ball around the nondegenerate Gaussian.

Infrastructure a complete development needs: the pushforward of a multivariate Gaussian under a linear functional (a one-dimensional Gaussian), the Gibbs variational principle for relative entropy, the strong duality for KL balls, and properties of Φ\PhiΦ and its quantile (continuity, strict monotonicity, symmetry Φ(−t)=1−Φ(t)\Phi(-t) = 1 - \Phi(t)Φ(−t)=1−Φ(t)). The Gaussian-quantile and KL-ball duality lemmas are reusable beyond this mission. Contributions of any of these as separate lemmas are welcome.

Selected references

  • L. El Ghaoui, M. Oks, F. Oustry, Worst-Case Value-at-Risk and Robust Portfolio Optimization: A Conic Programming Approach, Operations Research 51(4):543–556, 2003. https://doi.org/10.1287/opre.51.4.543.16101
  • J. E. Smith, Generalized Chebychev Inequalities: Theory and Applications in Decision Analysis, Operations Research 43(5):807–825, 1995. https://doi.org/10.1287/opre.43.5.807
  • M. D. Donsker, S. R. S. Varadhan, Asymptotic evaluation of certain Markov process expectations for large time, I, Communications on Pure and Applied Mathematics 28(1):1–47, 1975. https://doi.org/10.1002/cpa.3160280102
  • L. P. Hansen, T. J. Sargent, Robust Control and Model Uncertainty, American Economic Review 91(2):60–66, 2001. https://doi.org/10.1257/aer.91.2.60
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Captain: Elsie66

Shannon's Source Coding TheoremResearch Paper

Motivation

How short can a code for a data source be, if the code must still be uniquely decodable — if every string of concatenated codewords can be unambiguously split back into the original symbols? Shannon's 1948 source coding theorem answers this exactly: the entropy of the source is a hard lower bound on the average codeword length of any uniquely decodable code, and it is also achievable up to a one-symbol slack. Entropy is not just a measure of "average surprise" — it is the literal, tight answer to a combinatorial question about how densely symbols can be packed into strings without losing decodability. This is the theorem that gives Shannon's entropy its operational meaning, and it underlies every practical lossless compression scheme (Huffman coding, arithmetic coding, Lempel–Ziv) as the benchmark they approach.

Timeline.

  • 1948 — Claude Shannon, "A Mathematical Theory of Communication" (Bell System Technical Journal), introduces entropy and proves the source coding theorem.
  • 1949 — Leon Kraft's MIT master's thesis proves the combinatorial inequality (for prefix codes) that makes the theorem's achievability half constructive.
  • 1956 — Brockway McMillan extends Kraft's inequality's necessity direction from prefix codes to the strictly larger class of uniquely decodable codes, giving the theorem its full generality.

Setting

A source has a finite alphabet of symbols ι\iotaι, with at least two symbols, and probability distribution p:ι→Rp:\iota\to\mathbb Rp:ι→R (pi>0p_i>0pi​>0, ∑ipi=1\sum_i p_i=1∑i​pi​=1). A code assigns to each symbol iii a codeword c(i)c(i)c(i), a finite string over a DDD-ary code alphabet α\alphaα (D=∣α∣≥2D=|\alpha|\ge 2D=∣α∣≥2); the code is uniquely decodable if every finite sequence of codewords is determined by its concatenation. The entropy of ppp in base DDD is

HD(p)=−∑ipilog⁡Dpi.H_D(p) = -\sum_i p_i \log_D p_i.HD​(p)=−i∑​pi​logD​pi​.

The expected codeword length of ccc under ppp is L(c)=∑ipi ∣c(i)∣L(c) = \sum_i p_i \, |c(i)|L(c)=∑i​pi​∣c(i)∣.

Formalization targets

Goal — Shannon's source coding theorem

∀ injective, uniquely decodable c,HD(p)≤L(c),∃ such c,L(c)<HD(p)+1.\forall \text{ injective, uniquely decodable } c,\quad H_D(p) \le L(c), \qquad \exists \text{ such } c,\quad L(c) < H_D(p) + 1.∀ injective, uniquely decodable c,HD​(p)≤L(c),∃ such c,L(c)<HD​(p)+1.

(For a source with ∣ι∣≥2|\iota| \ge 2∣ι∣≥2 symbols — see Formalization scope for why the single-symbol case must be excluded.)

Significance

The result itself. This theorem is the reason entropy is called entropy in an information-theoretic sense at all: it converts a quantity defined by an abstract formula (−∑pilog⁡pi-\sum p_i\log p_i−∑pi​logpi​) into the exact answer to an operational question (minimum achievable expected code length), with a slack no worse than one symbol. It is the founding theorem of lossless source coding and the benchmark every practical compressor is measured against.

Formalizing it. Mathlib recently gained genuine information-theoretic coding content: InformationTheory.UniquelyDecodable and the necessity direction of the Kraft–McMillan inequality (McMillan's 1956 result: a uniquely decodable code's lengths satisfy ∑wD−∣w∣≤1\sum_w D^{-|w|}\le 1∑w​D−∣w∣≤1) are already proved, via a counting argument on concatenations of rrr codewords. This mission builds directly on that foundation rather than duplicating it. What Mathlib does not have — and what this mission's milestones supply — is Kraft's original 1949 sufficiency direction (existence of a uniquely decodable code realizing any length assignment satisfying the Kraft sum bound), any notion of Shannon entropy for a general finite distribution, and the source coding theorem itself.

Difficulty

The lower bound (HD(p)≤L(c)H_D(p)\le L(c)HD​(p)≤L(c)) is the easier half: it follows from the Kraft–McMillan inequality (already in Mathlib) via Gibbs'/Jensen's inequality applied to the two probability-like sequences pip_ipi​ and D−ℓi/KD^{-\ell_i}/KD−ℓi​/K (where K=∑jD−ℓj≤1K=\sum_j D^{-\ell_j}\le1K=∑j​D−ℓj​≤1 is the Kraft sum) — a short, self-contained convexity argument.

The achievability half is the genuine construction. Given the ideal (generally non-integer) lengths −log⁡Dpi-\log_D p_i−logD​pi​, one rounds up to ℓi=⌈−log⁡Dpi⌉\ell_i=\lceil -\log_D p_i\rceilℓi​=⌈−logD​pi​⌉ (Shannon–Fano–Elias lengths); a one-line estimate shows D−ℓi≤piD^{-\ell_i}\le p_iD−ℓi​≤pi​, so the Kraft sum of the rounded lengths is still ≤∑ipi=1\le\sum_i p_i=1≤∑i​pi​=1, and the bound ℓi<−log⁡Dpi+1\ell_i<-\log_D p_i+1ℓi​<−logD​pi​+1 gives L(c)<HD(p)+1L(c)<H_D(p)+1L(c)<HD​(p)+1 immediately once a code with exactly these lengths is shown to exist. Producing that code is Kraft's sufficiency direction, and it needs an explicit construction: order the lengths, and assign to symbol iii the first ℓi\ell_iℓi​ digits of the DDD-ary expansion of the cumulative sum ∑j<iD−ℓj\sum_{j<i} D^{-\ell_j}∑j<i​D−ℓj​. Verifying this assignment is injective, has the prescribed lengths, and is uniquely decodable (indeed prefix-free) is a careful but standard combinatorial argument — the main open piece of this mission.

Formalization scope

The source alphabet ι\iotaι must have at least two symbols (∣ι∣≥2|\iota|\ge 2∣ι∣≥2), not merely be nonempty. A single-symbol source forces p≡1p\equiv 1p≡1 and entropy HD(p)=0H_D(p)=0HD​(p)=0, so the achievability conjunct would demand a codeword of length 000 — but a uniquely decodable code can never contain the empty codeword (InformationTheory.UniquelyDecodable.epsilon_not_mem, provable from the definition: the empty string decodes ambiguously as zero or two copies of itself), so no admissible code exists and the theorem would be false, not merely hard, at ∣ι∣=1|\iota|=1∣ι∣=1. The same defect breaks Kraft's sufficiency direction (Milestone 2) whenever any prescribed length is 000, independent of ∣ι∣|\iota|∣ι∣; that milestone accordingly requires every length strictly positive. With ∣ι∣≥2|\iota|\ge2∣ι∣≥2 and full support, every pi<1p_i<1pi​<1 strictly, so the Shannon–Fano lengths ⌈−log⁡Dpi⌉\lceil-\log_D p_i\rceil⌈−logD​pi​⌉ are automatically all ≥1\ge1≥1, and the achievability construction only ever needs Milestone 2 at positive lengths. The code alphabet α\alphaα is likewise an arbitrary finite type (matching Mathlib's own Fintype/Nonempty conventions for the Kraft–McMillan file), with ∣α∣≥2|\alpha|\ge2∣α∣≥2 required to keep Real.logb non-degenerate. The source distribution is required strictly positive (pi>0p_i>0pi​>0) — the standard simplifying assumption (zero-probability symbols can always be dropped without loss). Unique decodability is stated exactly as Mathlib's InformationTheory.UniquelyDecodable, not re-derived from a "prefix code" definition, so the mission's results transport directly onto Mathlib's existing Kraft–McMillan file. A trivializing route to rule out: proving only the lower bound (citing Mathlib's inequality) while leaving the existential achievability half unaddressed would not be Shannon's theorem — the sandwich HD(p)≤L∗<HD(p)+1H_D(p)\le L^*<H_D(p)+1HD​(p)≤L∗<HD​(p)+1 is the theorem's actual content, and the lower bound alone (already essentially free from Mathlib) is not a novel contribution on its own.

Reusable output: the Kraft sufficiency construction (Milestone 2) is directly reusable for any future formalization of Huffman coding optimality, arithmetic coding, or the general "Kraft-inequality-achieving code exists" fact used throughout coding theory. Contributions are welcome starting from Milestone 2 (the open construction) or Milestone 3 (the Gibbs'-inequality lower bound, which only needs Milestone 1, already available via Mathlib).

Selected references

  • C. E. Shannon, "A Mathematical Theory of Communication," The Bell System Technical Journal 27 (1948), 379–423, 623–656.
  • T. M. Cover and J. A. Thomas, Elements of Information Theory, 2nd ed., Wiley, 2006, Chapter 5 ("Data Compression"), §5.2 ("Kraft Inequality") and §5.4 ("Bounds on the Optimal Code Length," Theorem 5.4.1).
  • L. G. Kraft, A Device for Quantizing, Grouping, and Coding Amplitude-Modulated Pulses, M.S. thesis, MIT, 1949.
  • B. McMillan, "Two Inequalities Implied by Unique Decipherability," IRE Transactions on Information Theory 2:4 (1956), 115–116.
  • Mathlib, Mathlib.InformationTheory.Coding.UniquelyDecodable and Mathlib.InformationTheory.Coding.KraftMcMillan (2026).
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EconomicsOperations Research·Captain: mikedeng1

Human and Machine: The Impact of Machine Input on Decision-Making Under Cognitive Limitations II: Machine Input Never Lowers the Decision-Maker's Accuracy or Expected ValueResearch Paper

Motivation

Machine-learning systems are increasingly placed beside human experts — physicians reading scans, loan officers screening applications, judges assessing risk — rather than replacing them. The machine processes the structured data it can see; the human also has access to information the algorithm cannot observe, but her attention is limited. Whether such a partnership improves the decision is a question about how the human reallocates scarce cognitive effort once part of the information is handed to her for free.

Boyacı, Canyakmaz and de Véricourt (ESMT Working Paper 20-02, 2020; published in Management Science, 2024) model the human as a rationally inattentive decision-maker in the sense of Sims (2003): she chooses how much information to process, and pays a cost proportional to the mutual information between the state and her decision. In the binary-choice setting, Matějka and McKay (2015) showed that such problems reduce to choosing conditional choice probabilities, with logit-form solutions. The paper uses this reduction to compare a decision-maker who decides alone with one who first sees a machine's assessment. This mission formalizes its first comparison, Proposition 1: the machine never lowers the decision-maker's accuracy or her expected value.

Setting

A decision-maker (DM) must announce whether the state of the world ω∈{g,b}\omega\in\{g,b\}ω∈{g,b} is good (a=ya=ya=y) or bad (a=na=na=n). A correct choice pays 111, an incorrect one 000. Her prior that the state is good is μ∈[0,1]\mu\in[0,1]μ∈[0,1], and λ≥0\lambda\ge0λ≥0 is the information cost.

A strategy is a pair (pg,pb)∈[0,1]2(p_g,p_b)\in[0,1]^2(pg​,pb​)∈[0,1]2 of conditional probabilities of choosing yyy in state ggg and in state bbb. It induces the choice probability p=μpg+(1−μ)pbp=\mu p_g+(1-\mu)p_bp=μpg​+(1−μ)pb​, the accuracy A=μpg+(1−μ)(1−pb)A=\mu p_g+(1-\mu)(1-p_b)A=μpg​+(1−μ)(1−pb​), the cognitive cost

C=λ[H(p)−(1−μ)H(pb)−μH(pg)],H(x)=−xlog⁡x−(1−x)log⁡(1−x),C=\lambda\big[H(p)-(1-\mu)H(p_b)-\mu H(p_g)\big],\qquad H(x)=-x\log x-(1-x)\log(1-x),C=λ[H(p)−(1−μ)H(pb​)−μH(pg​)],H(x)=−xlogx−(1−x)log(1−x),

(the mutual information between state and action, in nats) and the expected value V=A−CV=A-CV=A−C. The DM maximizes VVV. The optimal accuracy A⋆(μ)A^\star(\mu)A⋆(μ) and optimal value V⋆(μ)V^\star(\mu)V⋆(μ) are the accuracy and value at a maximizer. Two thresholds organize the solution:

μ‾=1e1/λ+1,μˉ=e1/λe1/λ+1.\underline\mu=\frac{1}{e^{1/\lambda}+1},\qquad \bar\mu=\frac{e^{1/\lambda}}{e^{1/\lambda}+1}.μ​=e1/λ+11​,μˉ​=e1/λ+1e1/λ​.

The machine. Information is aggregated into two binary variables: X1X_1X1​, which the machine and the DM can both evaluate, and X2X_2X2​, which only the DM can assess. Realizations are x1,x2∈{−,+}x_1,x_2\in\{-,+\}x1​,x2​∈{−,+} and the state is good iff x1=x2=+x_1=x_2=+x1​=x2​=+. The DM's prior on (X1,X2)(X_1,X_2)(X1​,X2​) is π\piπ, with π(x1,x2)>0\pi(x_1,x_2)>0π(x1​,x2​)>0 for all four realizations, so μ=π(+,+)\mu=\pi(+,+)μ=π(+,+). The machine reveals x1x_1x1​ at no cost; the DM updates by Bayes' rule to μx=P(ω=g∣X1=x)\mu^x=P(\omega=g\mid X_1=x)μx=P(ω=g∣X1​=x) and then solves her problem with prior μx\mu^xμx. The machine-assisted accuracy and value are the ex-ante expectations

Am⋆=∑xP(X1=x) A⋆(μx),Vm⋆=∑xP(X1=x) V⋆(μx).A^\star_m=\sum_{x}P(X_1=x)\,A^\star(\mu^x),\qquad V^\star_m=\sum_{x}P(X_1=x)\,V^\star(\mu^x).Am⋆​=x∑​P(X1​=x)A⋆(μx),Vm⋆​=x∑​P(X1​=x)V⋆(μx).

Formalization targets

Goal: Proposition 1

For every λ≥0\lambda\ge0λ≥0 and every prior π\piπ with positive entries,

Am⋆≥A⋆(μ)andVm⋆≥V⋆(μ).A^\star_m\ge A^\star(\mu)\qquad\text{and}\qquad V^\star_m\ge V^\star(\mu).Am⋆​≥A⋆(μ)andVm⋆​≥V⋆(μ).

Milestones

  1. Equation (3). μ−=0\mu^-=0μ−=0 and μ+=μ/(μ+π(+,−))>μ\mu^+=\mu/(\mu+\pi(+,-))>\muμ+=μ/(μ+π(+,−))>μ.
  2. Corollary 2, (13). For λ>0\lambda>0λ>0: A⋆(μ)=1−μA^\star(\mu)=1-\muA⋆(μ)=1−μ on [0,μ‾][0,\underline\mu][0,μ​], e1/λ/(e1/λ+1)e^{1/\lambda}/(e^{1/\lambda}+1)e1/λ/(e1/λ+1) on (μ‾,μˉ)(\underline\mu,\bar\mu)(μ​,μˉ​), and μ\muμ on [μˉ,1][\bar\mu,1][μˉ​,1].
  3. Corollary 2, (15). For λ>0\lambda>0λ>0: V⋆(μ)=1−μV^\star(\mu)=1-\muV⋆(μ)=1−μ on [0,μ‾][0,\underline\mu][0,μ​], λ[log⁡(e1/λ+1)−H(μ)]\lambda[\log(e^{1/\lambda}+1)-H(\mu)]λ[log(e1/λ+1)−H(μ)] on (μ‾,μˉ)(\underline\mu,\bar\mu)(μ​,μˉ​), and μ\muμ on [μˉ,1][\bar\mu,1][μˉ​,1].
  4. Lemma 2 (accuracy and value). Am⋆=1−μ/μ++(μ/μ+)A⋆(μ+)A^\star_m=1-\mu/\mu^++(\mu/\mu^+)A^\star(\mu^+)Am⋆​=1−μ/μ++(μ/μ+)A⋆(μ+), and the same identity for Vm⋆V^\star_mVm⋆​.
  5. Convexity of A⋆A^\starA⋆ on [0,1][0,1][0,1] (proof of Proposition 1).
  6. Slopes at the thresholds. The middle branch of (15) has derivative −1-1−1 at μ‾\underline\muμ​ and 111 at μˉ\bar\muμˉ​.
  7. Convexity of V⋆V^\starV⋆ on [0,1][0,1][0,1].

Significance

The result. Proposition 1 is the baseline against which the paper's other findings are measured: although accuracy and value always improve, the machine can lower the probability of choosing the good state, raise false positives, and increase the DM's cognitive effort (Theorems 2–4 of the paper). Without Proposition 1 those effects would not be separable from a simple loss of decision quality. The closed forms (13) and (15) also show that, where the DM processes information, her accuracy depends on λ\lambdaλ alone and not on her prior.

Formalizing it. The proposition and its milestones are proved in the paper, in Appendix A, and the closed forms rely on the logit characterization of the optimum. None of this is machine-checked. A complete development produces a verified closed-form solution of the binary rational-inattention problem with entropy cost, with accuracy and value as explicit functions of the prior, and a verified value-of-information inequality for that problem. Both are reusable by the other four missions of this series and by any binary rational-inattention model.

Difficulty

The obvious argument — more information cannot hurt — is not available off the shelf: the DM is not a Bayesian with free information but optimizes an entropy-penalized program, and the comparison is between optimal values of two such programs at different priors. A⋆A^\starA⋆ and V⋆V^\starV⋆ are values at an optimum of a non-linear program over [0,1]2[0,1]^2[0,1]2. Their closed forms require identifying exactly when the corner solutions pg=pb=0p_g=p_b=0pg​=pb​=0 and pg=pb=1p_g=p_b=1pg​=pb​=1 are optimal and handling the degenerate priors μ=0,1\mu=0,1μ=0,1, where the maximizer is not unique. Both functions are piecewise in μ\muμ, so their shape on [0,1][0,1][0,1] does not follow from the shape of each piece: the behaviour at the kinks μ‾\underline\muμ​ and μˉ\bar\muμˉ​ decides it. Accuracy is a component of the objective, not the objective itself, so statements about A⋆A^\starA⋆ do not follow from optimality alone.

Formalization scope

  • Decision problem. The paper's general information-processing problem (2) is not formalized. The DM chooses (pg,pb)∈[0,1]2(p_g,p_b)\in[0,1]^2(pg​,pb​)∈[0,1]2 directly — the paper's own §4 reduction (Matějka & McKay 2015), not a restriction. HHH is Mathlib's Real.binEntropy (natural logarithm); λ\lambdaλ is lam.
  • Starred metrics. A⋆A^\starA⋆ and V⋆V^\starV⋆ are accuracy and value at a chosen maximizer (Classical.epsilon); every maximizer yields the same values. They are defined for every real μ\muμ and used on [0,1][0,1][0,1].
  • Machine. {−,+}\{-,+\}{−,+} is Bool with true =+=+=+; the prior is π : Bool → Bool → ℝ with positive entries summing to 111. Posteriors are defined by Bayes' rule; Am⋆A^\star_mAm⋆​, Vm⋆V^\star_mVm⋆​ are expectations over x1x_1x1​.
  • Parameters. The goal keeps the printed λ≥0\lambda\ge0λ≥0 (at λ=0\lambda=0λ=0 the cost vanishes); all milestones assume the model's standing λ>0\lambda>0λ>0, needed for 1/λ1/\lambda1/λ. The paper's parameter set S={(μ,μ+)∈[0,1]2:μ<μ+}\mathcal S=\{(\mu,\mu^+)\in[0,1]^2:\mu<\mu^+\}S={(μ,μ+)∈[0,1]2:μ<μ+} is replaced by priors with positive entries, which realize exactly 0<μ<μ+<10<\mu<\mu^+<10<μ<μ+<1.
  • Ruled out. Defining A⋆A^\starA⋆, V⋆V^\starV⋆ by the closed forms (13), (15); defining Am⋆A^\star_mAm⋆​, Vm⋆V^\star_mVm⋆​ by the right-hand sides of Lemma 2; or assuming convexity as a hypothesis — each makes the corresponding statement true by definition, and none of them is used here.
  • Infrastructure. Calculus of Real.binEntropy (derivative, concavity) is in Mathlib. Needed: existence of a maximizer on the square, the first-order characterization of the interior optimum, and convexity of piecewise functions glued with matching slopes. Contributions of general lemmas on these points are welcome.

Selected references

  • T. Boyacı, Y. Canyakmaz, F. de Véricourt, Human and Machine: The Impact of Machine Input on Decision-Making Under Cognitive Limitations, ESMT Working Paper 20-02, 2020; Management Science 70(2), 2024. https://doi.org/10.1287/mnsc.2023.4744
  • F. Matějka, A. McKay, Rational Inattention to Discrete Choices: A New Foundation for the Multinomial Logit Model, American Economic Review 105(1), 2015. https://doi.org/10.1257/aer.20130047
  • C. A. Sims, Implications of Rational Inattention, Journal of Monetary Economics 50(3), 2003. https://doi.org/10.1016/S0304-3932(03)00029-1
  • T. M. Cover, J. A. Thomas, Elements of Information Theory, 2nd ed., Wiley, 2006. https://doi.org/10.1002/047174882X
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EconomicsOperations ResearchOptimization·Captain: mikedeng1

Human and Machine: The Impact of Machine Input on Decision-Making Under Cognitive Limitations I: The Rationally Inattentive Decision-Maker's Optimal Choice Probability in Closed FormResearch Paper

Motivation

A person using a machine's advice may decide more accurately, but attention is costly. Before asking what a machine changes, the baseline decision has to be understood: how often would the person choose the action associated with a good state without machine input? Boyacı, Canyakmaz, and de Véricourt study this question in a model of a decision maker who can acquire information about an unknown binary state and pays for the expected reduction in uncertainty. Their working paper derives a closed form for the decision maker's choice probability. That baseline is used later in the paper to compare decisions with and without machine input.

The information cost follows the rational inattention approach: a decision maker chooses how much information to process while considering its effect on the final action. In the discrete choice setting, Matějka and McKay (2015) characterize optimal conditional choice probabilities. The paper adopts their equivalent choice probability representation in §4. This mission isolates the first consequence of that representation, Theorem 1, before the paper introduces the machine.

Setting

The unknown state is good, ggg, with prior probability μ\muμ, and bad, bbb, with probability 1−μ1-\mu1−μ. The decision maker selects either yyy (declare good) or nnn (declare bad). A correct action earns one unit, and an incorrect action earns zero. Write pgp_gpg​ for the probability of choosing yyy when the state is ggg, and pbp_bpb​ for the probability of choosing yyy when the state is bbb. A strategy is any pair (pg,pb)∈[0,1]2(p_g,p_b)\in[0,1]^2(pg​,pb​)∈[0,1]2; the pair may lie on the no-information diagonal or on the boundary of the square.

The unconditional choice probability is p=μpg+(1−μ)pbp=\mu p_g+(1-\mu)p_bp=μpg​+(1−μ)pb​. The accuracy is A=μpg+(1−μ)(1−pb)A=\mu p_g+(1-\mu)(1-p_b)A=μpg​+(1−μ)(1−pb​). Binary entropy, measured with the natural logarithm, is H(t)=−tlog⁡t−(1−t)log⁡(1−t)H(t)=-t\log t-(1-t)\log(1-t)H(t)=−tlogt−(1−t)log(1−t), with H(0)=H(1)=0H(0)=H(1)=0H(0)=H(1)=0. Given an information-cost parameter λ>0\lambda>0λ>0, the cognitive cost in the paper's choice probability representation is

C=λ[H(p)−(1−μ)H(pb)−μH(pg)].C=\lambda\bigl[H(p)-(1-\mu)H(p_b)-\mu H(p_g)\bigr].C=λ[H(p)−(1−μ)H(pb​)−μH(pg​)].

The decision maker maximizes net value V=A−CV=A-CV=A−C over the whole square. An optimal pair is one whose value is at least that of every feasible pair. The source originally introduces a general distribution of information signals and a Bayes consistency condition in problem (2). Section 4 and footnote 8 adopt the equivalent conditional choice probability representation used here. The equivalence itself is an input from Matějka and McKay (2015), rather than a claim of this mission.

Formalization targets

Optimal choice probability

For 0<μ<10<\mu<10<μ<1 and λ>0\lambda>0λ>0, define the thresholds

μ‾(λ)=1e1/λ+1,μ‾(λ)=e1/λe1/λ+1.\underline\mu(\lambda)=\frac{1}{e^{1/\lambda}+1},\qquad \overline\mu(\lambda)=\frac{e^{1/\lambda}}{e^{1/\lambda}+1}.μ​(λ)=e1/λ+11​,μ​(λ)=e1/λ+1e1/λ​.

The goal is the paper's Theorem 1: every optimal pair has the same unconditional choice probability,

p⋆(μ)={0,μ≤μ‾,μ1−e−1/λ−1−μe1/λ−1,μ‾<μ<μ‾,1,μ≥μ‾.p^\star(\mu)= \begin{cases} 0,&\mu\le\underline\mu,\\ \displaystyle\frac{\mu}{1-e^{-1/\lambda}}-\frac{1-\mu}{e^{1/\lambda}-1},&\underline\mu<\mu<\overline\mu,\\ 1,&\mu\ge\overline\mu. \end{cases}p⋆(μ)=⎩⎨⎧​0,1−e−1/λμ​−e1/λ−11−μ​,1,​μ≤μ​,μ​<μ<μ​,μ≥μ​.​

The same theorem states μ‾<1/2<μ‾\underline\mu<1/2<\overline\muμ​<1/2<μ​, that p⋆p^\starp⋆ is non-decreasing in the prior, and that the lower threshold increases while the upper threshold decreases as λ\lambdaλ increases. This mission includes all these clauses in its single goal. The intermediate milestones formalize the paper's conditional choice equations, the algebraic interior candidate, its threshold crossings, and its slope and threshold derivatives.

Significance

The formula partitions prior beliefs into three regimes. With a sufficiently low prior, the decision maker always chooses nnn; with a sufficiently high prior, the decision maker always chooses yyy. Between the thresholds, the probability of choosing yyy changes continuously with the prior. The threshold movements describe how a higher information cost changes the region in which information processing affects the choice. In the paper, these probabilities feed into accuracy, error rate, effort, and machine input comparisons.

The paper proves the result mathematically. The statements here are open Lean targets, so compilation of their declarations does not amount to machine-checked proofs. A complete development would verify the optimality characterization and the closed form, then provide reusable binary entropy and constrained optimization lemmas. It would also expose a precise baseline that subsequent missions can import after publication.

Difficulty

Equations (4)–(6) alone do not select the optimum: both p=0p=0p=0 and p=1p=1p=1 satisfy them for every prior. The printed uniqueness phrase in Lemma 1 therefore cannot be carried into a theorem about all solutions of those equations. The formal target says instead that every maximizing strategy satisfies the conditional choice equations, and Theorem 1 identifies the probability selected by maximization. The endpoint strategies, where entropy is evaluated at zero or one, must remain in the feasible set. One must also distinguish the algebraic interior root from the optimizer when that root leaves [0,1][0,1][0,1].

Formalization scope

Lean represents probabilities and costs as real numbers. The strategy space is the full closed square [0,1]2[0,1]^2[0,1]2, and IsOptimal compares net value against every point in that square. The prior in the goal and Lemma 1 lies strictly between zero and one, as in the paper's §4 setting; λ\lambdaλ is strictly positive. Boolean state and action types are unnecessary in this first mission because the paper's §4 representation is already the pair of conditional probabilities. The general-signal distribution of problem (2) is not encoded here.

The entropy function is Mathlib's Real.binEntropy, with natural logarithms and the endpoint values used by the paper. The threshold definitions reproduce Theorem 1 exactly. pBar is the interior algebraic expression from Appendix A, and pClosed is only the right-hand side of equation (11). Neither defines the optimizer. In particular, defining the starred optimal probability by the closed form would remove the theorem's main claim. The goal quantifies over every optimal pair and asserts that its computed choice probability equals that expression.

Contributions to the proof will need results about binary entropy at the boundary, derivatives of the objective in the interior, existence and characterization of maximizers on a compact square, and elementary inequalities for the exponential thresholds. The entropy and compact optimization infrastructure can support later formalizations beyond this paper. The four listed milestones follow the authors' Appendix A argument; alternative proofs of the same faithful statements are welcome.

Selected references

  • Tamer Boyacı, Caner Canyakmaz, and Francis de Véricourt, Human and Machine: The Impact of Machine Input on Decision-Making Under Cognitive Limitations, ESMT Working Paper 20-02, November 30, 2020, §§3–4 and Appendix A. Working paper record.
  • Filip Matějka and Alisdair McKay, Rational Inattention to Discrete Choices: A New Foundation for the Multinomial Logit Model, American Economic Review 105(1), 2015, pp. 272–298. DOI.
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Combinatorics·Captain: chaikon

Essential Coding Theory I: Generalized Hamming BoundTextbook

Motivation

An error-correcting code stores or transmits messages as words over a finite alphabet, adding redundancy so that the original word can be recovered after some symbols are corrupted. The basic question of coding theory is the trade-off between the amount of redundancy and the number of errors that can be corrected. The Hamming bound (also called the sphere-packing bound) is the first and most widely taught upper limit on this trade-off. It is due to R. W. Hamming (1950), who introduced the Hamming distance and the Hamming codes in the same paper (Hamming 1950).

This mission formalizes the bound as it is stated in Theorem 1.7.2 of the textbook Essential Coding Theory by V. Guruswami, A. Rudra and M. Sudan (web draft, §1.7, p. 21). It is the first mission of a series following that book. The result is used throughout the book to define perfect codes (Definition 1.7.3) and as the baseline against which later bounds (Singleton, Plotkin, Elias–Bassalygo, the linear-programming bound) are compared.

Setting

Let α\alphaα be a finite alphabet with q=∣α∣q = |\alpha|q=∣α∣ symbols, and let n≥0n \ge 0n≥0. A word of length nnn is a function {0,…,n−1}→α\{0, \dots, n-1\} \to \alpha{0,…,n−1}→α, and αn\alpha^nαn is the set of all qnq^nqn words. A code of block length nnn is a subset C⊆αnC \subseteq \alpha^nC⊆αn; its elements are codewords.

The Hamming distance Δ(u,v)\Delta(u, v)Δ(u,v) between two words is the number of coordinates in which they differ. The dimension of CCC is the real number k=log⁡q∣C∣k = \log_q |C|k=logq​∣C∣ (Definition 1.2.3 of the book). The book calls CCC an (n,k,d)q(n, k, d)_q(n,k,d)q​ code when its minimum distance min⁡c1≠c2∈CΔ(c1,c2)\min_{c_1 \ne c_2 \in C} \Delta(c_1, c_2)minc1​=c2​∈C​Δ(c1​,c2​) equals ddd (Definitions 1.4.1 and 1.7.1).

The Hamming ball of radius eee around a word xxx is B(x,e)={y∈αn:Δ(x,y)≤e}B(x, e) = \{ y \in \alpha^n : \Delta(x, y) \le e \}B(x,e)={y∈αn:Δ(x,y)≤e} (Definition 1.6.1).

Formalization targets

Milestone: volume of a Hamming ball

For every word x∈αnx \in \alpha^nx∈αn and every radius e≥0e \ge 0e≥0,

∣B(x,e)∣=∑i=0e(ni)(q−1)i.|B(x, e)| = \sum_{i=0}^{e} \binom{n}{i} (q-1)^i.∣B(x,e)∣=i=0∑e​(in​)(q−1)i.

This is equation (1.18) in the book.

Goal: the generalized Hamming bound

If any two distinct codewords of C⊆αnC \subseteq \alpha^nC⊆αn are at Hamming distance at least ddd, then

log⁡q∣C∣  ≤  n−log⁡q(∑i=0⌊(d−1)/2⌋(ni)(q−1)i).\log_q |C| \;\le\; n - \log_q \Bigl( \sum_{i=0}^{\lfloor (d-1)/2 \rfloor} \binom{n}{i} (q-1)^i \Bigr).logq​∣C∣≤n−logq​(i=0∑⌊(d−1)/2⌋​(in​)(q−1)i).

The hypothesis is "minimum distance at least ddd" rather than "exactly ddd". Every (n,k,d)q(n, k, d)_q(n,k,d)q​ code satisfies it, so the goal contains the book's Theorem 1.7.2 as stated.

Significance

The result itself. The bound says that a code correcting ⌊(d−1)/2⌋\lfloor (d-1)/2 \rfloor⌊(d−1)/2⌋ errors can have at most qn/Volq(⌊(d−1)/2⌋,n)q^n / \mathrm{Vol}_q(\lfloor (d-1)/2 \rfloor, n)qn/Volq​(⌊(d−1)/2⌋,n) codewords, so its rate is at most 1−log⁡qVolq/n1 - \log_q \mathrm{Vol}_q / n1−logq​Volq​/n. Codes meeting it with equality are the perfect codes: the Hamming codes, the binary repetition codes of odd length, and the two Golay codes. The bound's asymptotic form, R≤1−Hq(δ/2)R \le 1 - H_q(\delta/2)R≤1−Hq​(δ/2), is one of the standard upper bounds on the rate–distance trade-off and is the reference point for the stronger bounds later in the book.

Formalizing it. The theorem has been proved since 1950 and appears in every coding theory text. Mathlib has the Hamming distance (hammingDist) but no notion of a code's distance, no Hamming-ball cardinality formula, and no sphere-packing bound. This mission supplies those, with the dimension stated through the real logarithm exactly as in the book, so later missions in the series can cite it.

Difficulty

The mathematics is elementary. The work lies in the counting step: showing that exactly (ni)(q−1)i\binom{n}{i}(q-1)^i(in​)(q−1)i words lie at distance exactly iii from a fixed word. This identity has no ready-made counterpart in Mathlib, and the alphabet carries no algebraic structure, so translating every ball to a ball around a fixed word is not available. The final step, taking log⁡q\log_qlogq​ of both sides, must also handle the conventions of the real logarithm on degenerate inputs.

Formalization scope

  • The alphabet is an arbitrary type α with [Fintype α] [DecidableEq α], and qqq is Fintype.card α. Words are functions Fin n → α, and Δ\DeltaΔ is Mathlib's hammingDist.
  • A code is a Finset (Fin n → α). The distance hypothesis quantifies over pairs of distinct codewords.
  • The dimension is Real.logb q |C|, a real number. The ball volume is the natural-number sum ∑i=0⌊(d−1)/2⌋(ni)(q−1)i\sum_{i=0}^{\lfloor (d-1)/2 \rfloor} \binom{n}{i}(q-1)^i∑i=0⌊(d−1)/2⌋​(in​)(q−1)i, cast to R\mathbb{R}R, where ⌊(d−1)/2⌋\lfloor (d-1)/2 \rfloor⌊(d−1)/2⌋ is computed in N\mathbb{N}N as (d - 1) / 2.
  • No hypotheses q≥2q \ge 2q≥2 or C≠∅C \ne \emptysetC=∅ are imposed. The book assumes them tacitly. Under Lean's conventions log⁡qx=0\log_q x = 0logq​x=0 when q≤1q \le 1q≤1 or x=0x = 0x=0, and the statement remains true in those cases. It is therefore at least as strong as the book's version, and these degenerate cases are not a trivialization: for q≥2q \ge 2q≥2 and C≠∅C \ne \emptysetC=∅ the goal is equivalent to the sphere-packing inequality ∣C∣⋅Vol≤qn|C| \cdot \mathrm{Vol} \le q^n∣C∣⋅Vol≤qn.
  • No custom definitions are needed. The ball-volume formula is reusable for any later bound that counts Hamming balls (Gilbert–Varshamov, Elias–Bassalygo). Contributions of alternative counting proofs are welcome.

Selected references

  • V. Guruswami, A. Rudra and M. Sudan, Essential Coding Theory, draft textbook, §1.6–1.7, Theorem 1.7.2, p. 21. https://cse.buffalo.edu/faculty/atri/courses/coding-theory/book/web-coding-book.pdf
  • R. W. Hamming, Error detecting and error correcting codes, Bell System Technical Journal 29(2), 147–160, 1950. https://doi.org/10.1002/j.1538-7305.1950.tb00463.x
  • The Mathlib Community, hammingDist, Mathlib.InformationTheory.Hamming. https://leanprover-community.github.io/mathlib4_docs/Mathlib/InformationTheory/Hamming.html
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Machine LearningStatistics·Captain: mikedeng1

The Statistical Complexity of Interactive Decision Making I: Subadditivity of Squared Hellinger Distance for Sequential Laws, D²_H(P,Q) ≤ 10² log(n)·E_P[Σᵢ D²_H(P⁽ⁱ⁾, Q⁽ⁱ⁾)] for n ≥ 2Research Paper

Motivation

Lower bounds for interactive decision making (bandits, reinforcement learning, and the general decision making with structured observations framework of Foster, Kakade, Qian and Rakhlin, arXiv:2112.13487) compare what a learner observes under two different environments. A learner's whole interaction history is generated one step at a time: each observation is drawn from a conditional law that depends on everything seen before. Statistical estimation guarantees, by contrast, are stated one step at a time, as bounds on the divergence between the conditional laws at each round. Passing from the per-step guarantees to a statement about the laws of entire histories requires a chain rule for the divergence in use.

For the Kullback–Leibler divergence the chain rule is an identity. The paper's guarantees, however, are stated in the squared Hellinger distance, which is bounded, symmetric, and the natural loss for density estimation with the logarithmic loss. Hellinger distance has no exact chain rule. Lemma A.13 of the paper (App. A.2, p. 73) supplies an approximate one, losing a factor logarithmic in the number of steps, and the paper uses it in the proof of its main regret lower bound (Theorem 3.2, via App. C.1.3).

Setting

Fix n∈Nn \in \mathbb Nn∈N and finite sets X1,…,Xn\mathcal X_1, \dots, \mathcal X_nX1​,…,Xn​. A sequence is x=(x1,…,xn)x = (x_1, \dots, x_n)x=(x1​,…,xn​) with xi∈Xix_i \in \mathcal X_ixi​∈Xi​, and x1:i−1=(x1,…,xi−1)x_{1:i-1} = (x_1, \dots, x_{i-1})x1:i−1​=(x1​,…,xi−1​) denotes its prefix; X(i−1)=∏t=1i−1Xt\mathcal X^{(i-1)} = \prod_{t=1}^{i-1} \mathcal X_tX(i−1)=∏t=1i−1​Xt​.

For probability distributions p,qp, qp,q on a finite set, the squared Hellinger distance, the Hellinger distance and the Kullback–Leibler divergence are

DH2(p,q)=∑a(p(a)−q(a))2,DH=DH2,DKL(p ∥ q)=∑ap(a)log⁡p(a)q(a),D^2_{\mathrm H}(p, q) = \sum_a \big(\sqrt{p(a)} - \sqrt{q(a)}\big)^2, \qquad D_{\mathrm H} = \sqrt{D^2_{\mathrm H}}, \qquad D_{\mathrm{KL}}(p\,\|\,q) = \sum_a p(a) \log\frac{p(a)}{q(a)},DH2​(p,q)=a∑​(p(a)​−q(a)​)2,DH​=DH2​​,DKL​(p∥q)=a∑​p(a)logq(a)p(a)​,

the last one set to +∞+\infty+∞ when ppp charges a point that qqq does not. Note that the paper's DH2D^2_{\mathrm H}DH2​ carries no factor 12\tfrac1221​, so 0≤DH2≤20 \le D^2_{\mathrm H} \le 20≤DH2​≤2.

A family of sequential kernels P=(P(i))i=1nP = (P^{(i)})_{i=1}^nP=(P(i))i=1n​ assigns to each iii and each prefix x1:i−1x_{1:i-1}x1:i−1​ a probability distribution P(i)(⋅∣x1:i−1)P^{(i)}(\cdot \mid x_{1:i-1})P(i)(⋅∣x1:i−1​) on Xi\mathcal X_iXi​. Its sequential law is the law of X1,…,XnX_1, \dots, X_nX1​,…,Xn​ under Xi∼P(i)(⋅∣X1:i−1)X_i \sim P^{(i)}(\cdot \mid X_{1:i-1})Xi​∼P(i)(⋅∣X1:i−1​):

P(x)=∏i=1nP(i)(xi∣x1:i−1).\mathbb P(x) = \prod_{i=1}^n P^{(i)}(x_i \mid x_{1:i-1}).P(x)=i=1∏n​P(i)(xi​∣x1:i−1​).

For a second family QQQ with law Q\mathbb QQ, the quantity controlled by per-step estimation is

EP[∑i=1nDH2(P(i)(⋅∣X1:i−1),Q(i)(⋅∣X1:i−1))].\mathbb E_{\mathbb P}\Big[\sum_{i=1}^n D^2_{\mathrm H}\big(P^{(i)}(\cdot \mid X_{1:i-1}), Q^{(i)}(\cdot \mid X_{1:i-1})\big)\Big].EP​[i=1∑n​DH2​(P(i)(⋅∣X1:i−1​),Q(i)(⋅∣X1:i−1​))].

In Lean these are IsSeqKernel, seqLaw and condHellingerSum, with hellingerSq and klDivDiscrete the published discrete divergences.

Formalization targets

Goal: Lemma A.13, (97), for n≥2n \ge 2n≥2

DH2(P,Q)≤102log⁡(n)⋅EP[∑i=1nDH2(P(i)(⋅∣X1:i−1),Q(i)(⋅∣X1:i−1))].D^2_{\mathrm H}(\mathbb P, \mathbb Q) \le 10^2 \log(n) \cdot \mathbb E_{\mathbb P}\Big[\sum_{i=1}^n D^2_{\mathrm H}\big(P^{(i)}(\cdot \mid X_{1:i-1}), Q^{(i)}(\cdot \mid X_{1:i-1})\big)\Big].DH2​(P,Q)≤102log(n)⋅EP​[i=1∑n​DH2​(P(i)(⋅∣X1:i−1​),Q(i)(⋅∣X1:i−1​))].

The constant 10210^2102 is the paper's; the shape that matters downstream is the logarithmic dependence on nnn with no assumption on the kernels beyond their being probability kernels.

Companion: Lemma A.13, (98)

If V≥eV \ge eV≥e and P(i)(A∣x1:i−1)≤V Q(i)(A∣x1:i−1)P^{(i)}(A \mid x_{1:i-1}) \le V\, Q^{(i)}(A \mid x_{1:i-1})P(i)(A∣x1:i−1​)≤VQ(i)(A∣x1:i−1​) for every iii, prefix and event AAA, then DH2(P,Q)≤3log⁡(V)⋅EP[∑iDH2(P(i),Q(i))]D^2_{\mathrm H}(\mathbb P, \mathbb Q) \le 3\log(V) \cdot \mathbb E_{\mathbb P}[\sum_i D^2_{\mathrm H}(P^{(i)}, Q^{(i)})]DH2​(P,Q)≤3log(V)⋅EP​[∑i​DH2​(P(i),Q(i))].

Milestones

  1. Lemma A.10 (p. 72): DKL(p ∥ q)≤(2+log⁡V) DH2(p,q)D_{\mathrm{KL}}(p\,\|\,q) \le (2 + \log V)\, D^2_{\mathrm H}(p, q)DKL​(p∥q)≤(2+logV)DH2​(p,q) under a likelihood-ratio bound VVV (referenced, finite case).
  2. Lemma A.5 (p. 71): DTV2≤DH2≤DKLD^2_{\mathrm{TV}} \le D^2_{\mathrm H} \le D_{\mathrm{KL}}DTV2​≤DH2​≤DKL​ (referenced, finite case).
  3. The triangle inequality for DHD_{\mathrm H}DH​ (proof of Lemma A.13, p. 73).
  4. The chain rule DKL(Q ∥ P)=EQ[∑iDKL(Q(i) ∥ P(i))]D_{\mathrm{KL}}(\mathbb Q\,\|\,\mathbb P) = \mathbb E_{\mathbb Q}[\sum_i D_{\mathrm{KL}}(Q^{(i)}\,\|\,P^{(i)})]DKL​(Q∥P)=EQ​[∑i​DKL​(Q(i)∥P(i))] for sequential laws (p. 73).
  5. Convexity of DH2D^2_{\mathrm H}DH2​ in its second argument (p. 74).
  6. Lemma A.11 (p. 72), the multiplicative Pinsker-type inequality: ∣EPh−EQh∣≤2R(EPh+EQh)DH2(P,Q)|\mathbb E_P h - \mathbb E_Q h| \le \sqrt{2R(\mathbb E_P h + \mathbb E_Q h) D^2_{\mathrm H}(P, Q)}∣EP​h−EQ​h∣≤2R(EP​h+EQ​h)DH2​(P,Q)​ and EPh≤3EQh+4R DH2(P,Q)\mathbb E_P h \le 3\mathbb E_Q h + 4R\, D^2_{\mathrm H}(P, Q)EP​h≤3EQ​h+4RDH2​(P,Q) for 0≤h≤R0 \le h \le R0≤h≤R.

Significance

The result. Inequality (97) converts per-round Hellinger estimation error into a bound on the Hellinger distance between the laws of complete interaction histories, under no boundedness assumption on likelihood ratios. In the paper this is the step that lets the lower bound of Theorem 3.2 relate any algorithm's behaviour under a reference model to its behaviour under alternatives, and hence express the minimax regret through the decision-estimation coefficient. Without it, only the KL chain rule is available, which requires bounded likelihood ratios (the situation of (98)) or loses more than a logarithmic factor. Lemma A.11, a milestone here, is used independently in the same lower bound and in the paper's tabular reinforcement learning analysis.

Formalizing it. The lemma is proved in the paper; no machine-checked proof exists. The published layer on the platform has the discrete divergences and the comparisons of Lemmas A.5 and A.10; the sequential-law objects, the triangle inequality, the convexity of DH2D^2_{\mathrm H}DH2​, the discrete chain rule and Lemma A.11 are new. A completed development gives a reusable chain-rule toolkit for any later formalization of lower bounds over adaptive interaction histories.

Difficulty

The squared Hellinger distance does not tensorize along adaptive sequences: the natural attempt to write 1−12DH2(P,Q)1 - \tfrac12 D^2_{\mathrm H}(\mathbb P, \mathbb Q)1−21​DH2​(P,Q) as a product of conditional affinities fails because the conditional affinities are random, depending on the prefix, and their expectation does not factor. Bounding DH2D^2_{\mathrm H}DH2​ by DKLD_{\mathrm{KL}}DKL​ and applying the KL chain rule fails in the other direction: the conditional KL divergences are not controlled by the conditional Hellinger distances unless the likelihood ratios are bounded, and in (97) they are not. The difficulty is to obtain a bound that pays only log⁡n\log nlogn for an unbounded ratio, with explicit constants that survive the final numerical comparison.

Formalization scope

  • Finite alphabets. The paper works over measurable spaces. This mission formalizes the finite-alphabet case, as the published FoundationsRL divergence layer does: each Xi\mathcal X_iXi​ is a Fintype, distributions are probability vectors, expectations are finite sums. Coordinates are indexed by Fin n (0-based) and the alphabets may differ from coordinate to coordinate.
  • Kernels. A kernel family is a function P i x of the whole sequence that is a probability vector and depends only on the coordinates j < i; this is what makes seqLaw P the law the paper describes.
  • Added hypothesis n≥2n \ge 2n≥2 in (97). The paper states (97) for every nnn; at n=1n = 1n=1 the right side vanishes because log⁡1=0\log 1 = 0log1=0 while the left side is positive whenever P(1)≠Q(1)P^{(1)} \ne Q^{(1)}P(1)=Q(1), and the proof's last step 2(6log⁡(96n)+1896n)≤102log⁡n2(6\log(96n) + \tfrac{18}{96n}) \le 10^2\log n2(6log(96n)+96n18​)≤102logn holds only for n≥2n \ge 2n≥2. The goal is stated for n≥2n \ge 2n≥2, with the constant unchanged.
  • Likelihood ratios are stated multiplicatively, P(A)≤V Q(A)P(A) \le V\,Q(A)P(A)≤VQ(A), so that a zero denominator does not make a hypothesis vacuous; KL divergences are compared to Hellinger distances in [0,∞][0, \infty][0,∞].
  • Lemma A.11 holds "almost surely under PPP and QQQ", which becomes: 0≤h≤R0 \le h \le R0≤h≤R at every point charged by PPP or QQQ.
  • Ruling out trivial forms. The goal's hypotheses are satisfiable with P≠Q\mathbb P \ne \mathbb QP=Q and n≥2n \ge 2n≥2 (checked in a sanity file). A formalization in which the kernels may read coordinates beyond the prefix, in which log⁡\loglog is applied to n≤1n \le 1n≤1, or in which the ratio bound of (98) is checked through a quotient that is vacuous at zero denominators, is not the paper's statement.

Contributions welcome: proofs of any milestone and of the fact that seqLaw is a probability vector.

Selected references

  • D. J. Foster, S. M. Kakade, J. Qian, A. Rakhlin, The Statistical Complexity of Interactive Decision Making, arXiv:2112.13487v3, 2023. https://arxiv.org/abs/2112.13487
  • Y. Yang, A. Barron, An asymptotic property of model selection criteria, IEEE Transactions on Information Theory 44(1), 1998. https://doi.org/10.1109/18.650993
  • Y. Polyanskiy, Y. Wu, Lecture Notes on Information Theory, 2014. https://people.lids.mit.edu/yp/homepage/data/itlectures_v5.pdf
  • D. J. Foster, A. Rakhlin, Foundations of Reinforcement Learning and Interactive Decision Making, arXiv:2312.16730v1, 2023. https://arxiv.org/abs/2312.16730
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Machine LearningOptimal TransportOptimization·Captain: mikedeng1

Computational Optimal Transport IX: The Entropic Cost L^ε_C(a, b) Equals max ⟨f, a⟩ + ⟨g, b⟩ − ε⟨e^{f/ε}, K e^{g/ε}⟩, with Optimal Scalings (e^{f/ε}, e^{g/ε})Textbook

Motivation

Optimal transport compares two distributions by finding the least expensive way to move mass between them. For finite histograms, the resulting linear program is precise but its optimal coupling can be sparse. In applications where the coupling represents traffic, matching, or a differentiable loss, a sparse plan may be undesirable or expensive to compute repeatedly. Peyré and Cuturi describe how adding an entropy term selects a diffuse coupling and leads to matrix scaling algorithms that can be used on large finite problems (Peyré and Cuturi, 2019, Chapter 4).

The entropic dual gives a second view of the same regularized problem. Its variables are real vectors attached to the two marginal constraints. Unlike the ordinary Kantorovich dual, the objective has no explicit feasibility constraints and is smooth. This permits calculations in the log domain, which the book introduces because direct scaling with exponentials can suffer from numerical overflow or underflow when the regularization parameter is small relative to the costs (Peyré and Cuturi, 2019, §4.4). This mission targets the exact relationship between the regularized minimum, the smooth dual maximum, and the scaling factors.

Setting

Fix positive integers n,mn,mn,m. A histogram a∈Σna\in\Sigma_na∈Σn​ is a vector with nonnegative entries summing to one; b∈Σmb\in\Sigma_mb∈Σm​ is defined similarly. Strict positivity is required for the attained dual maximum and log-domain updates; the primal scaling and Kantorovich-feasibility statements also cover zero-entry histograms. A coupling P∈U(a,b)P\in U(a,b)P∈U(a,b) is an n×mn\times mn×m matrix with nonnegative entries, row sums aaa, and column sums bbb. A real matrix CCC assigns cost CijC_{ij}Cij​ to each transfer from row iii to column jjj, and ⟨C,P⟩=∑i,jCijPij\langle C,P\rangle=\sum_{i,j}C_{ij}P_{ij}⟨C,P⟩=∑i,j​Cij​Pij​ is its transport cost.

The book uses the entropy H(P)=−∑i,jPij(log⁡Pij−1)H(P)=-\sum_{i,j}P_{ij}(\log P_{ij}-1)H(P)=−∑i,j​Pij​(logPij​−1), with 0log⁡0=00\log0=00log0=0. For ε>0\varepsilon>0ε>0, the regularized cost is LCε(a,b)=min⁡P∈U(a,b){⟨C,P⟩−εH(P)}L_C^\varepsilon(a,b)=\min_{P\in U(a,b)}\{\langle C,P\rangle-\varepsilon H(P)\}LCε​(a,b)=minP∈U(a,b)​{⟨C,P⟩−εH(P)}. The Gibbs kernel has entries Kij=exp⁡(−Cij/ε)K_{ij}=\exp(-C_{ij}/\varepsilon)Kij​=exp(−Cij​/ε). Given potentials f∈Rnf\in\mathbb R^nf∈Rn and g∈Rmg\in\mathbb R^mg∈Rm, the smooth dual objective is Q(f,g)=⟨f,a⟩+⟨g,b⟩−ε∑i,jefi/εKijegj/εQ(f,g)=\langle f,a\rangle+\langle g,b\rangle-\varepsilon\sum_{i,j}e^{f_i/\varepsilon}K_{ij}e^{g_j/\varepsilon}Q(f,g)=⟨f,a⟩+⟨g,b⟩−ε∑i,j​efi​/εKij​egj​/ε. These are the finite-dimensional objects of (4.1), (4.2), and (4.30) in the source (Peyré and Cuturi, 2019, pp. 425, 428, 448).

Formalization targets

Attained entropic duality

The goal is Proposition 4.4. There are an optimal coupling PPP and potentials (f,g)(f,g)(f,g) at which the dual reaches its maximum, with the common value

LCε(a,b)=⟨C,P⟩−εH(P)=max⁡f′,g′Q(f′,g′).L_C^\varepsilon(a,b) =\langle C,P\rangle-\varepsilon H(P) =\max_{f',g'} Q(f',g').LCε​(a,b)=⟨C,P⟩−εH(P)=f′,g′max​Q(f′,g′).

For every maximizing pair (f′,g′)(f',g')(f′,g′), the same optimal coupling satisfies

Pij=efi′/εKijegj′/ε.P_{ij}=e^{f'_i/\varepsilon}K_{ij}e^{g'_j/\varepsilon}.Pij​=efi′​/εKij​egj′​/ε.

Thus the dual potentials determine the scaling vectors u=ef′/εu=e^{f'/\varepsilon}u=ef′/ε and v=eg′/εv=e^{g'/\varepsilon}v=eg′/ε in (4.12). The maximum is an attained maximum of a real function, as stated in the book, rather than an unrestricted real infimum or supremum that might take a default value on a bad input (Peyré and Cuturi, 2019, Proposition 4.4).

Supporting results

The milestones follow the source's statements. Proposition 4.3 gives existence, uniqueness, and the Gibbs scaling of the primal optimizer. Remark 4.21 gives the two partial-gradient formulas and the closed log-domain block updates. Proposition 4.5 states that an entropic dual maximizer is a feasible pair of ordinary Kantorovich potentials, so its linear objective is bounded above by the unregularized cost LC(a,b)L_C(a,b)LC​(a,b) (Peyré and Cuturi, 2019, pp. 432, 449, 452–453).

Significance

The equality establishes that the matrix scaling variables and the dual potentials describe the same optimal coupling. It lets a computation based on scaling be interpreted as maximizing a smooth objective, and it gives exact marginal-error expressions through the dual gradients. Feasible Kantorovich potentials obtained at the optimum also provide a lower bound on the ordinary transport cost. These statements explain why log-domain updates represent the same mathematical problem as entropic transport, even when direct exponentiation is numerically fragile (Peyré and Cuturi, 2019, §§4.4–4.5).

The results are established in the textbook; the open work here is their Lean formalization. A completed development would provide reusable finite coupling, entropy, Gibbs-kernel, and smooth-dual interfaces, together with the existence and differentiability results needed to connect them. It would also distinguish a primal optimum, a dual maximum, and a feasible potential without relying on informal convention. The mission does not assert that these textbook results are new, and no machine-checked proof of these exact statements is claimed here.

Difficulty

The unconstrained dual objective has a symmetry: shifting every coordinate of fff by one constant and every coordinate of ggg by its negative leaves the value unchanged. Consequently, the set of maximizers is not bounded in the ordinary product space. Positivity of the marginals matters for attaining a maximum with finite real potentials; if a marginal entry is zero, the corresponding potential can escape toward negative infinity. On the primal side, the entropy formula must be valid at zero entries even though optimality links it to strictly positive exponential scalings. The formal argument must connect these boundary conventions and the finite-dimensional optimization statements without turning the maximum into a junk real supremum (Peyré and Cuturi, 2019, Proposition 4.4 and Remark 4.21).

Formalization scope

The Lean development represents indices by Fin n and Fin m, matrices by Matrix (Fin n) (Fin m) ℝ, and histograms by Mathlib's stdSimplex. Positive dimensions and ε>0\varepsilon>0ε>0 appear throughout. Strictly positive marginal entries are required for the attained dual maximum and log-domain updates; the other statements permit zero entries. The book assumes positive weights for discrete measures in Remark 2.1; the marginal positivity is also required for the attained dual maximum and the logarithmic updates. The cost matrix itself may have arbitrary real entries. Entropy uses Real.negMulLog, which implements 0log⁡0=00\log0=00log0=0 on the nonnegative couplings where it is applied.

The primal optimum is a predicate on a coupling and its objective, rather than a chosen matrix. The unregularized LCL_CLC​ is a real infimum used only when simplex marginals make its feasible set nonempty and bounded. The dual objective is a finite sum. Its gradients are stated as one-variable derivatives in each coordinate, and each block update is characterized as the unique maximizer with the other block fixed. The complete development needs Mathlib's finite sums, real exponential and logarithm, calculus, finite-dimensional topology, and optimization facts. Contributions that establish these shared interfaces or the four milestone statements are in scope.

Propositions 4.7 and 4.8 are excluded from this proposal because their printed bounds compare a dual linear objective with LCεL_C^\varepsilonLCε​ where the accompanying arguments instead support a comparison with the unregularized LCL_CLC​; (4.47) also has a sign discrepancy. The milestone list therefore avoids encoding a false inequality (Peyré and Cuturi, 2019, pp. 453–454).

Selected references

  • Gabriel Peyré and Marco Cuturi, Computational Optimal Transport, Foundations and Trends in Machine Learning 11(5–6), 2019, pp. 355–607. DOI: 10.1561/2200000073.
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Computational Optimal Transport VII: The Entropic Optimal Coupling P_ε Tends to the Maximum-Entropy Optimal Plan as ε → 0 and to a ⊗ b as ε → ∞Textbook

Motivation

The discrete optimal transport problem of Kantorovich asks for the cheapest way to move a probability histogram a\mathbf aa onto a histogram b\mathbf bb when moving a unit of mass from iii to jjj costs Ci,j\mathbf C_{i,j}Ci,j​. Its optimal couplings are vertices of a polytope and are typically sparse: they rely on a few routes. Two communities have reasons to blur them. In transportation planning, observed traffic is more diffuse than linear-programming predictions, which led to the "gravity" model of Wilson (1969) and Erlander (1980), as recounted in Peyré and Cuturi, §4.1. In machine learning and statistics, adding an entropy term to the objective turns the linear program into a strictly convex problem that Sinkhorn's matrix-scaling algorithm solves at scale (Cuturi, 2013).

Every use of the entropic problem raises the same question: what does the regularized solution approximate? Chapter 4 of Peyré and Cuturi's Computational Optimal Transport answers it in Proposition 4.1 for the two extreme regimes of the regularization strength ε\varepsilonε.

Timeline. Cominetti and San Martín (1994) studied the convergence of entropic penalties for linear programs, including first-order expansions near ε=0\varepsilon = 0ε=0 and ε=+∞\varepsilon = +\inftyε=+∞. Peyré and Cuturi (2019) record the transport case as Proposition 4.1, with a short compactness proof.

Setting

Fix sizes n,m≥1n, m \ge 1n,m≥1. A histogram is a vector of the probability simplex Σn={a∈R+n:∑iai=1}\Sigma_n = \{\mathbf a \in \mathbb R^n_+ : \sum_i \mathbf a_i = 1\}Σn​={a∈R+n​:∑i​ai​=1}. Given a∈Σn\mathbf a \in \Sigma_na∈Σn​, b∈Σm\mathbf b \in \Sigma_mb∈Σm​, the set of couplings is

U(a,b)={P∈R+n×m:P1m=a, P⊤1n=b},\mathbf U(\mathbf a,\mathbf b) = \{\mathbf P \in \mathbb R_+^{n\times m} : \mathbf P\mathbb 1_m = \mathbf a,\ \mathbf P^\top\mathbb 1_n = \mathbf b\},U(a,b)={P∈R+n×m​:P1m​=a, P⊤1n​=b},

nonnegative matrices with row sums a\mathbf aa and column sums b\mathbf bb. For a cost matrix C∈Rn×m\mathbf C \in \mathbb R^{n\times m}C∈Rn×m write ⟨C,P⟩=∑i,jCi,jPi,j\langle \mathbf C, \mathbf P\rangle = \sum_{i,j}\mathbf C_{i,j}\mathbf P_{i,j}⟨C,P⟩=∑i,j​Ci,j​Pi,j​. The Kantorovich problem is LC(a,b)=min⁡P∈U(a,b)⟨C,P⟩\mathrm L_{\mathbf C}(\mathbf a,\mathbf b) = \min_{\mathbf P \in \mathbf U(\mathbf a,\mathbf b)}\langle \mathbf C,\mathbf P\rangleLC​(a,b)=minP∈U(a,b)​⟨C,P⟩.

The discrete entropy of a coupling is

H(P)=−∑i,jPi,j(log⁡Pi,j−1),\mathbf H(\mathbf P) = -\sum_{i,j}\mathbf P_{i,j}(\log \mathbf P_{i,j} - 1),H(P)=−i,j∑​Pi,j​(logPi,j​−1),

with 0log⁡0=00\log 0 = 00log0=0. For ε>0\varepsilon > 0ε>0 the entropic problem is

LCε(a,b)=min⁡P∈U(a,b)⟨P,C⟩−εH(P),\mathrm L^\varepsilon_{\mathbf C}(\mathbf a,\mathbf b) = \min_{\mathbf P\in\mathbf U(\mathbf a,\mathbf b)}\langle \mathbf P,\mathbf C\rangle - \varepsilon\mathbf H(\mathbf P),LCε​(a,b)=P∈U(a,b)min​⟨P,C⟩−εH(P),

whose unique minimizer is Pε\mathbf P_\varepsilonPε​. The maximum-entropy optimal coupling P0⋆\mathbf P^\star_0P0⋆​ is the optimal coupling of the Kantorovich problem with the largest entropy. The Gibbs kernel is Ki,j=e−Ci,j/ε\mathbf K_{i,j} = e^{-\mathbf C_{i,j}/\varepsilon}Ki,j​=e−Ci,j​/ε and the Kullback–Leibler divergence between matrices is KL(P∣K)=∑i,jPi,jlog⁡(Pi,j/Ki,j)−Pi,j+Ki,j\mathrm{KL}(\mathbf P|\mathbf K) = \sum_{i,j}\mathbf P_{i,j}\log(\mathbf P_{i,j}/\mathbf K_{i,j}) - \mathbf P_{i,j} + \mathbf K_{i,j}KL(P∣K)=∑i,j​Pi,j​log(Pi,j​/Ki,j​)−Pi,j​+Ki,j​.

In Lean these are couplings, frob and IsOptimalCoupling in CompOT.Assignment, and entropy, entObjective, IsEntropicOptimal, IsMaxEntropyOptimal, gibbs and klMat in CompOT.EntropicLimit.

Formalization targets

Goal: Proposition 4.1

For a∈Σn\mathbf a\in\Sigma_na∈Σn​, b∈Σm\mathbf b \in \Sigma_mb∈Σm​ and any cost matrix C\mathbf CC,

Pε→ε→0+P0⋆,LCε(a,b)→ε→0+LC(a,b),Pε→ε→+∞a⊗b=(aibj)i,j.\mathbf P_\varepsilon \xrightarrow{\varepsilon\to 0^+} \mathbf P^\star_0,\qquad \mathrm L^\varepsilon_{\mathbf C}(\mathbf a,\mathbf b)\xrightarrow{\varepsilon\to 0^+}\mathrm L_{\mathbf C}(\mathbf a,\mathbf b),\qquad \mathbf P_\varepsilon\xrightarrow{\varepsilon\to+\infty}\mathbf a\otimes\mathbf b = (\mathbf a_i\mathbf b_j)_{i,j}.Pε​ε→0+​P0⋆​,LCε​(a,b)ε→0+​LC​(a,b),Pε​ε→+∞​a⊗b=(ai​bj​)i,j​.

Milestones

  1. For ε>0\varepsilon > 0ε>0, problem (4.2) has a unique optimal solution (§4.1, p. 425).
  2. The maximum-entropy optimal coupling (4.3) exists and is unique (proof of Proposition 4.1, p. 426).
  3. The sandwich (4.5): for an optimal P\mathbf PP and ε>0\varepsilon>0ε>0, 0≤⟨C,Pε⟩−⟨C,P⟩≤ε(H(Pε)−H(P))0 \le \langle\mathbf C,\mathbf P_\varepsilon\rangle - \langle \mathbf C,\mathbf P\rangle \le \varepsilon(\mathbf H(\mathbf P_\varepsilon) - \mathbf H(\mathbf P))0≤⟨C,Pε​⟩−⟨C,P⟩≤ε(H(Pε​)−H(P)).
  4. a⊗b\mathbf a \otimes \mathbf ba⊗b is the unique maximizer of H\mathbf HH on U(a,b)\mathbf U(\mathbf a,\mathbf b)U(a,b) (p. 426).
  5. (4.7): Pε\mathbf P_\varepsilonPε​ is the KL projection of the Gibbs kernel onto U(a,b)\mathbf U(\mathbf a,\mathbf b)U(a,b) (p. 428).

Significance

The result. Proposition 4.1 justifies the entropic regularization as an approximation scheme: for small ε\varepsilonε the regularized plan converges to an exact optimal plan, and specifically to a canonical one, the most diffuse among all optimal couplings, so the limit does not depend on any tie-breaking. The value LCε\mathrm L^\varepsilon_{\mathbf C}LCε​ converges to the transport cost, which is what makes Sinkhorn-based estimates of transport distances meaningful. For large ε\varepsilonε the plan becomes the independent coupling a⊗b\mathbf a\otimes\mathbf ba⊗b, which explains the interpolation between optimal transport and maximum mean discrepancy studied later in the book. The KL projection identity (4.7) is the starting point of Sinkhorn's algorithm, so this mission also supplies the bridge to the next missions of the series.

Formalizing it. The proposition is a known result with a complete proof in the source; the work is formalizing it in Lean 4 with Mathlib. To our knowledge none of these statements, nor the discrete entropic transport problem itself, has a machine-checked proof in Mathlib or on the platform. A formal proof also pins down the convention for zero entries, on which the statement silently depends.

Difficulty

The obvious argument passes to the limit in the optimality of Pε\mathbf P_\varepsilonPε​, but this only shows that limit points are optimal for the Kantorovich problem; it does not identify which optimal coupling is the limit when the optimal set is a face of the polytope rather than a vertex. Identifying it requires a second-order argument at the level of the entropy, and the convergence of the whole family (not just a subsequence) rests on the uniqueness of the maximum-entropy optimal coupling, which in turn needs strict concavity of H\mathbf HH on a set that may contain matrices with zero entries, where the logarithm is singular. Existence and uniqueness of Pε\mathbf P_\varepsilonPε​ face the same boundary issue: the minimizer may a priori sit on the boundary of the polytope.

Formalization scope

Indices are 0-based (Fin n, Fin m); histograms are functions Fin n → ℝ in Mathlib's stdSimplex; matrices are Matrix (Fin n) (Fin m) ℝ with the product topology, so convergence is entrywise. Entropy uses 0log⁡0=00\log 0 = 00log0=0 (Real.negMulLog); the book's remark that H=−∞\mathbf H = -\inftyH=−∞ at a zero entry is not used, since it would contradict the continuity of H\mathbf HH invoked in the book's proof and make (4.3) degenerate. Optimality is expressed by predicates (a minimizer over U(a,b)\mathbf U(\mathbf a,\mathbf b)U(a,b)), never by a real infimum, so no junk value of an empty infimum appears. The limit ε→0\varepsilon \to 0ε→0 is taken from the right. The values LCε\mathrm L^\varepsilon_{\mathbf C}LCε​ and LC\mathrm L_{\mathbf C}LC​ appear as the objectives at Pε\mathbf P_\varepsilonPε​ and P0⋆\mathbf P^\star_0P0⋆​.

In the goal, Pε\mathbf P_\varepsilonPε​ and P0⋆\mathbf P^\star_0P0⋆​ are given by hypotheses (any family solving (4.2) for every ε>0\varepsilon > 0ε>0, any solution of (4.3)). This is not a vacuous formalization: milestones 1 and 2 assert that such objects exist and are unique, so the hypotheses are satisfiable and determine them. Standing assumptions are exactly those of the book: a∈Σn\mathbf a \in \Sigma_na∈Σn​, b∈Σm\mathbf b \in \Sigma_mb∈Σm​, ε>0\varepsilon > 0ε>0; no positivity of a\mathbf aa, b\mathbf bb or C\mathbf CC is assumed.

A complete development needs: compactness of the transport polytope, continuity and strict concavity of x↦−xlog⁡xx \mapsto -x\log xx↦−xlogx on [0,∞)[0,\infty)[0,∞), and the Gibbs inequality on finite sums. These are reusable for the Sinkhorn and entropic-duality missions of this series. Proofs of any milestone are welcome independently.

Selected references

  • G. Peyré and M. Cuturi, Computational Optimal Transport, Foundations and Trends in Machine Learning 11(5–6):355–607, 2019. https://doi.org/10.1561/2200000073 (§4.1, pp. 425–430)
  • R. Cominetti and J. San Martín, Asymptotic analysis of the exponential penalty trajectory in linear programming, Mathematical Programming 67(1–3):169–187, 1994. https://doi.org/10.1007/BF01582220
  • M. Cuturi, Sinkhorn Distances: Lightspeed Computation of Optimal Transport, NeurIPS 2013. https://arxiv.org/abs/1306.0895
  • A. G. Wilson, The use of entropy maximizing models, in the theory of trip distribution, mode split and route split, Journal of Transport Economics and Policy, 108–126, 1969 (bibliography of Peyré and Cuturi). https://doi.org/10.1561/2200000073
  • S. Erlander, Optimal Spatial Interaction and the Gravity Model, Vol. 173, Springer-Verlag, 1980 (bibliography of Peyré and Cuturi). https://doi.org/10.1561/2200000073
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Information-Theoretic Analysis of Generalization Capability of Learning Algorithms III: The Gibbs Algorithm Has Excess Risk at Most (1/β)log(1/Q(wₒ)) + β/(2n) (Corollary 2)Research Paper

Motivation

Statistical learning algorithms fit hypotheses to data that are available during training, while their performance is judged on new data. A rule that minimizes training loss can fit peculiarities of the sample, so its training loss and population loss need not agree. Xu and Raginsky study this difference through information quantities associated with the sample and the algorithm's output. Their Gibbs example shows how a probability distribution chosen before seeing the data can guide a randomized learner and yield a population-risk guarantee with explicit dependence on the sample size and the prior's mass at a good hypothesis. This mission formalizes their countable-hypothesis result, Corollary 2, and the steps of Section 4.3 and Appendix D that support it. Xu and Raginsky, 2017

Setting

Let Z\mathcal ZZ be an instance space and W\mathcal WW a hypothesis space, each with a measurable structure. A probability measure μ\muμ on Z\mathcal ZZ generates a sample S=(Z1,…,Zn)S=(Z_1,\ldots,Z_n)S=(Z1​,…,Zn​) of nnn independent observations. A loss ℓ(w,z)\ell(w,z)ℓ(w,z) measures the cost of hypothesis www on instance zzz. Its population risk is Lμ(w)=EZ∼μℓ(w,Z)L_\mu(w)=\mathbb E_{Z\sim\mu}\ell(w,Z)Lμ​(w)=EZ∼μ​ℓ(w,Z); its empirical risk on a realized sample sss is Ls(w)=n−1∑i=1nℓ(w,zi)L_s(w)=n^{-1}\sum_{i=1}^n\ell(w,z_i)Ls​(w)=n−1∑i=1n​ℓ(w,zi​). These definitions match equations (1)–(3) of the paper. Xu and Raginsky, 2017, p. 2

A randomized learning rule is a Markov kernel PW∣SP_{W|S}PW∣S​: for each observed sample sss, it gives a probability distribution for an output hypothesis WWW. Together with the sample law μ⊗n\mu^{\otimes n}μ⊗n, it determines the joint law of (S,W)(S,W)(S,W). The expected generalization error is gen⁡(μ,PW∣S)=E[Lμ(W)−LS(W)]\operatorname{gen}(\mu,P_{W|S})=\mathbb E[L_\mu(W)-L_S(W)]gen(μ,PW∣S​)=E[Lμ​(W)−LS​(W)], as in equation (4). A probability distribution QQQ on W\mathcal WW serves as a prior. The Gibbs rule at inverse temperature β>0\beta>0β>0 weights a hypothesis by its prior mass times e−βLs(w)e^{-\beta L_s(w)}e−βLs​(w), then normalizes across the hypothesis space. Thus it favors low empirical risk without discarding the prior. Xu and Raginsky, 2017, pp. 2, 6

The associated optimization problem balances expected empirical risk against the conditional Kullback–Leibler divergence from the learning kernel to QQQ: D(PW∣S∥Q∣PS)=∫D(PW∣S=s∥Q) μ⊗n(ds)D(P_{W|S}\Vert Q\mid P_S)=\int D(P_{W|S=s}\Vert Q)\,\mu^{\otimes n}(ds)D(PW∣S​∥Q∣PS​)=∫D(PW∣S=s​∥Q)μ⊗n(ds). This penalty measures how much the output distribution changes from the prior after observing the sample. The paper's Theorem 5 identifies the Gibbs kernel as an optimizer of this relaxed problem. Xu and Raginsky, 2017, p. 6

Formalization targets

Gibbs optimization

For nonnegative loss, Theorem 5 asserts that the Gibbs kernel is a Markov learning rule, has the normalized exponential distribution at each sample, and minimizes the relaxed objective over learning kernels:

PW∣S=s∗(dw)=e−βLs(w)Q(dw)EQ[e−βLs(W)].P^*_{W|S=s}(dw)=\frac{e^{-\beta L_s(w)}Q(dw)}{\mathbb E_Q[e^{-\beta L_s(W)}]}.PW∣S=s∗​(dw)=EQ​[e−βLs​(W)]e−βLs​(w)Q(dw)​.

The milestone list also records the Appendix D empirical-risk comparison with a fixed hypothesis, its identity D(δw∥Q)=−log⁡Q({w})D(\delta_w\Vert Q)=-\log Q(\{w\})D(δw​∥Q)=−logQ({w}) when the prior has positive mass at www, and the Gibbs generalization bound quoted in equation (28). Xu and Raginsky, 2017, pp. 6–7, 13

Expected population risk

The goal is Corollary 2. If W\mathcal WW is countable, 0≤ℓ≤10\le\ell\le10≤ℓ≤1, wow_owo​ achieves the minimum population risk, and Q({wo})>0Q(\{w_o\})>0Q({wo​})>0, then

E[Lμ(W)]≤inf⁡w∈WLμ(w)+1βlog⁡1Q({wo})+β2n.\mathbb E[L_\mu(W)]\le\inf_{w\in\mathcal W}L_\mu(w) +\frac1\beta\log\frac1{Q(\{w_o\})}+\frac\beta{2n}.E[Lμ​(W)]≤w∈Winf​Lμ​(w)+β1​logQ({wo​})1​+2nβ​.

The first excess term reflects the prior mass on a population-risk minimizer; the second is controlled by sample size and inverse temperature. The target keeps the infimum over the whole hypothesis space and the constants of equation (29). Xu and Raginsky, 2017, p. 7

Significance

Corollary 2 gives a quantitative way to choose a prior and temperature: a prior that puts more mass on a good hypothesis reduces the logarithmic term, while changing β\betaβ changes both terms in opposite directions. It also connects the optimization characterization of a randomized algorithm to the population risk that matters for learning. Without the empirical-risk comparison and the separate generalization estimate, optimizing the training objective alone would not give this population statement. Xu and Raginsky, 2017, pp. 6–7, 13

The cited paper proves Corollary 2 and Theorem 5; the present task is to supply machine-checked proofs of their faithful Lean statements. The Donsker–Varadhan inequality and a tilted-measure identity are already published and proved on the platform, and the basic sample-law and risk definitions are already published. The Gibbs optimization, the Appendix D comparisons, and the quoted bound (28) are posed here as new targets. This work would leave reusable definitions for randomized learning kernels, their Gibbs specialization, and objectives with potentially infinite divergence.

Difficulty

The Gibbs rule is defined separately at every sample, but a learning algorithm must be a measurable kernel on the entire sample space. Establishing the normalized density pointwise does not by itself establish this kernel property. The relaxed objective also combines an integral of empirical risk with a conditional divergence, either of which can be infinite before bounded-loss assumptions are imposed. Equation (28), which the paper attributes to earlier work, needs a sharp β/(2n)\beta/(2n)β/(2n) constant; the looser information bound discussed immediately before it has a different dependence on β\betaβ. These are separate mathematical obligations even though the final displayed inequality is short. Xu and Raginsky, 2017, pp. 6–7, 13

Formalization scope

The Lean development represents a sample as Fin n → Z, its law as Measure.pi, and a randomized learner as Kernel (Fin n → Z) W. Population and empirical risks come from the published LearnStability.Characterization.Setting definition. The Gibbs kernel is built by a normalized density over the probability prior QQQ; Theorem 5 explicitly asserts it is a Markov kernel. The relaxed objective takes values in R≥0∪{∞}\mathbb R_{\ge0}\cup\{\infty\}R≥0​∪{∞}, so an infinite KL cost is not lost through real conversion. Generalization error remains the real expectation of the population-risk minus empirical-risk difference. The stated loss bounds ensure those real expectations are meaningful in the bounded-loss results.

The paper assumes a nonnegative loss in its general setting and requires ℓ∈[0,1]\ell\in[0,1]ℓ∈[0,1] for the later bounds. The Lean statements add joint measurability of ℓ\ellℓ and n>0n>0n>0 explicitly. Corollary 2 also makes the named minimizer's defining property and positive prior mass explicit: countability alone does not ensure an attained infimum, and a zero prior mass makes the printed logarithmic bound infinite. Theorem 5 retains its general measurable hypothesis space and nonnegative loss; countability appears only where the paper invokes it. Theorem 5 states optimality over all Markov kernels, the displayed Gibbs formula, and, for each sample, uniqueness of the Gibbs distribution as the minimizer of the samplewise problem (C.12) of Appendix C. The goal concerns the Gibbs kernel's actual population risk, rather than only the existence of a minimizer of the relaxed objective.

Useful contributions include probability-kernel measurability, control of conditional divergence and its finite conversions, the fixed-hypothesis comparison, and the sharp bounded-loss generalization estimate. The point-mass KL identity and the extended objective can be reused in other Gibbs and PAC-Bayesian formalizations. Xu and Raginsky, 2017, pp. 2, 6–7, 13

Selected references

  • A. Xu and M. Raginsky, Information-Theoretic Analysis of Generalization Capability of Learning Algorithms, Advances in Neural Information Processing Systems 30, 2017. arXiv:1705.07809v2
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A Tutorial on Thompson Sampling I: Any Algorithm Whose Information Ratio Is at Most Γ̄ Has Expected Regret at Most √(Γ̄·H(x*)·T)Research Paper

Motivation

Thompson sampling (TS) chooses each action with the posterior probability that it is optimal. Its practical success in online advertising, recommendation and experimentation raised the question of why it works and when it does not. The tutorial of Russo, Van Roy, Kazerouni, Osband and Wen (Found. Trends Mach. Learn. 11(1), 2018) answers part of that question in §8.1 with an information-theoretic regret bound due to Russo and Van Roy (JMLR 17, 2016). The bound applies to every algorithm, not only TS. It reduces the analysis of a particular algorithm to one quantity, the information ratio: the squared expected regret of a period divided by the information the period yields about the optimal action.

Timeline:

  • 2016: Russo and Van Roy, An information-theoretic analysis of Thompson sampling (JMLR 17), introduce the information ratio with the regret and the mutual information both conditioned on a realised history, and prove the regret bound and bounds on the ratio for TS (for example ∣X∣/2|\mathcal X|/2∣X∣/2 for ∣X∣|\mathcal X|∣X∣-armed bandits and d/2d/2d/2 for linear bandits).
  • 2018: Russo and Van Roy, Learning to optimize via information-directed sampling (Oper. Res. 66), design algorithms that minimise the information ratio directly.
  • 2018: Russo and Van Roy, Satisficing in time-sensitive bandit learning (arXiv:1803.02855), observe that the same bounds hold with the information ratio averaged over histories. This is the form (8.7) the tutorial uses (footnote 1, p. 75).
  • 2018: the tutorial gives the bound as (8.8), with a three-line proof on p. 76 whose last step is cited from the 2016 paper.

Setting

An agent acts in periods t=1,2,…t=1,2,\dotst=1,2,…. In each period it selects an action xtx_txt​ from a finite set X\mathcal XX and observes an outcome yty_tyt​ from a finite set Y\mathcal YY. An unknown parameter θ\thetaθ, taking values in a measurable space Θ\ThetaΘ, has a prior distribution PPP. Given θ\thetaθ and the action xxx, the outcome is drawn from a probability vector qθ(⋅∣x)q_\theta(\cdot\mid x)qθ​(⋅∣x) that depends measurably on θ\thetaθ. The agent receives the reward r(yt)r(y_t)r(yt​) for a known function rrr. The mean reward of action xxx is

μ(x,θ)=∑yqθ(y∣x) r(y),\mu(x,\theta)=\sum_{y}q_\theta(y\mid x)\,r(y),μ(x,θ)=y∑​qθ​(y∣x)r(y),

and the optimal action x∗=x∗(θ)x^*=x^*(\theta)x∗=x∗(θ) is a measurable selector of arg⁡max⁡xμ(x,θ)\arg\max_x\mu(x,\theta)argmaxx​μ(x,θ). Ties may be broken in any measurable way, and every result holds for every selector.

The history Ht\mathbb H_tHt​ is the list (x1,y1),…,(xt,yt)(x_1,y_1),\dots,(x_t,y_t)(x1​,y1​),…,(xt​,yt​). An algorithm π\piπ assigns to every history a probability vector over X\mathcal XX, from which the next action is drawn. The joint law of (θ,Ht)(\theta,\mathbb H_t)(θ,Ht​) is P(dθ)∏s≤tπ(xs∣Hs−1) qθ(ys∣xs)P(d\theta)\prod_{s\le t}\pi(x_s\mid\mathbb H_{s-1})\,q_\theta(y_s\mid x_s)P(dθ)∏s≤t​π(xs​∣Hs−1​)qθ​(ys​∣xs​), and every expectation below is taken under it. The expected cumulative regret, or Bayesian regret, is

E[Regret(T)]=E[∑t=1T(μ(x∗,θ)−μ(xt,θ))].\mathbb E[\mathrm{Regret}(T)]=\mathbb E\Big[\sum_{t=1}^T\big(\mu(x^*,\theta)-\mu(x_t,\theta)\big)\Big].E[Regret(T)]=E[t=1∑T​(μ(x∗,θ)−μ(xt​,θ))].

The entropy of the prior distribution of x∗x^*x∗ is H(x∗)=−∑aP(x∗=a)log⁡P(x∗=a)H(x^*)=-\sum_a\mathbb P(x^*=a)\log\mathbb P(x^*=a)H(x∗)=−∑a​P(x∗=a)logP(x∗=a). The conditional mutual information I(x∗;(xt,yt)∣Ht−1)I(x^*;(x_t,y_t)\mid\mathbb H_{t-1})I(x∗;(xt​,yt​)∣Ht−1​) is the expected information that the period-ttt observation carries about x∗x^*x∗ given the past, averaged over the past. The information ratio of period ttt is (8.7):

Γt=(E[μ(x∗,θ)−μ(xt,θ)])2I(x∗;(xt,yt)∣Ht−1).\Gamma_t=\frac{\big(\mathbb E[\mu(x^*,\theta)-\mu(x_t,\theta)]\big)^2}{I(x^*;(x_t,y_t)\mid\mathbb H_{t-1})}.Γt​=I(x∗;(xt​,yt​)∣Ht−1​)(E[μ(x∗,θ)−μ(xt​,θ)])2​.

Formalization targets

Goal: (8.8)

For every model and every algorithm, every horizon TTT and every Γˉ≥0\bar\Gamma\ge0Γˉ≥0 with (E[μ(x∗,θ)−μ(xt,θ)])2≤Γˉ I(x∗;(xt,yt)∣Ht−1)\big(\mathbb E[\mu(x^*,\theta)-\mu(x_t,\theta)]\big)^2\le\bar\Gamma\,I(x^*;(x_t,y_t)\mid\mathbb H_{t-1})(E[μ(x∗,θ)−μ(xt​,θ)])2≤ΓˉI(x∗;(xt​,yt​)∣Ht−1​) for t=1,…,Tt=1,\dots,Tt=1,…,T,

E[Regret(T)]≤Γˉ H(x∗) T.\mathbb E[\mathrm{Regret}(T)]\le\sqrt{\bar\Gamma\,H(x^*)\,T}.E[Regret(T)]≤ΓˉH(x∗)T​.

When every mutual information is positive, the least such Γˉ\bar\GammaΓˉ is max⁡t≤TΓt\max_{t\le T}\Gamma_tmaxt≤T​Γt​, which is the tutorial's Γˉ\bar\GammaΓˉ. A companion theorem states that literal form under the positivity hypothesis.

Milestones, in the order of the p. 76 proof

  1. Regret is additive over periods:
E[Regret(T)]=∑t=1TE[μ(x∗,θ)−μ(xt,θ)].\mathbb E[\mathrm{Regret}(T)]=\sum_{t=1}^T\mathbb E[\mu(x^*,\theta)-\mu(x_t,\theta)].E[Regret(T)]=t=1∑T​E[μ(x∗,θ)−μ(xt​,θ)].
  1. The Jensen (Cauchy–Schwarz) step: if δt2≤ΓˉIt\delta_t^2\le\bar\Gamma I_tδt2​≤ΓˉIt​ for every ttt and ∑tIt≤H\sum_tI_t\le H∑t​It​≤H, then ∑tδt≤TΓˉH\sum_t\delta_t\le\sqrt{T\bar\Gamma H}∑t​δt​≤TΓˉH​. This milestone is the published, proved theorem BanditAlgorithm.information_ratio_cumulative_bound_signed. It states the step in the form the proof uses, with the entropy budget as a hypothesis.
  2. The entropy budget:
∑t=1TI(x∗;(xt,yt)∣Ht−1)≤H(x∗).\sum_{t=1}^T I\big(x^*;(x_t,y_t)\mid\mathbb H_{t-1}\big)\le H(x^*).t=1∑T​I(x∗;(xt​,yt​)∣Ht−1​)≤H(x∗).

Significance

The result. (8.8) separates the regret analysis of an algorithm into two independent problems. One is a per-period bound on the information ratio, which depends on the structure of the problem and the algorithm. The other is the entropy of the optimal action, which depends only on the prior. Combined with the bound Γˉ≤∣X∣/2\bar\Gamma\le|\mathcal X|/2Γˉ≤∣X∣/2 that Russo and Van Roy (2016) prove for TS on ∣X∣|\mathcal X|∣X∣-armed bandits, and with H(x∗)≤log⁡∣X∣H(x^*)\le\log|\mathcal X|H(x∗)≤log∣X∣, it gives ∣X∣ Tlog⁡∣X∣/2\sqrt{|\mathcal X|\,T\log|\mathcal X|/2}∣X∣Tlog∣X∣/2​. On the shortest-path problem of p. 76, Γˉ≤d/2\bar\Gamma\le d/2Γˉ≤d/2 makes the regret depend on the number ddd of edges and on H(x∗)H(x^*)H(x∗), not on the exponentially large number of paths. The same inequality is the design criterion of information-directed sampling, which chooses actions to minimise the ratio.

Formalizing it. The bound and its proof are known. The work here is to make the probabilistic model explicit, with a general parameter space, an outcome kernel and randomized algorithms; to formalize the per-period decomposition of the regret and the chain-rule argument behind the entropy budget, which the tutorial cites rather than proves; and to obtain (8.8) for every algorithm in one statement. The Proved platform results for Lattimore and Szepesvári's Bayesian adversarial bandit (Theorem 36.5 and its chain-rule lemmas) are about a different model: one algorithm (TS), the best arm in hindsight of a reward matrix, and the budget log⁡k\log klogk. To our knowledge, (8.8) itself has not been formalized.

Difficulty

The Cauchy–Schwarz step is elementary and already proved on the platform. Milestone 1 is bookkeeping: the cumulative regret integrates over histories of length TTT, while the period-ttt term integrates over histories of length ttt, and later periods must be integrated out.

The substance is the entropy budget. The obvious attempt bounds each period's information by H(x∗)H(x^*)H(x∗), which loses a factor TTT. The bound is uniform in TTT only because the per-period informations telescope: their sum is the information that the whole history carries about x∗x^*x∗, which is at most the entropy of x∗x^*x∗. Each step requires conditional distributions of x∗x^*x∗ given histories, where θ\thetaθ lives in a general measurable space and is integrated against the prior. Zero-probability histories must also be handled consistently with the convention 0log⁡0=00\log0=00log0=0.

Formalization scope

  • X\mathcal XX and Y\mathcal YY are finite types; Θ\ThetaΘ is an arbitrary measurable space with a probability measure PPP. The tutorial allows infinite action sets and general outcomes. The finite specialization makes H(x∗)H(x^*)H(x∗) and every mutual information a finite sum. The kernel qθ(⋅∣x)q_\theta(\cdot\mid x)qθ​(⋅∣x) of §4 replaces the noise representation yt=g(xt,θ,wt)y_t=g(x_t,\theta,w_t)yt​=g(xt​,θ,wt​) of p. 70; both describe the same laws.
  • Standing hypotheses: qθ(y∣x)≥0q_\theta(y\mid x)\ge0qθ​(y∣x)≥0, ∑yqθ(y∣x)=1\sum_yq_\theta(y\mid x)=1∑y​qθ​(y∣x)=1, measurability of θ↦qθ(y∣x)\theta\mapsto q_\theta(y\mid x)θ↦qθ​(y∣x), measurability of the level sets of x∗x^*x∗, and μ(x,θ)≤μ(x∗(θ),θ)\mu(x,\theta)\le\mu(x^*(\theta),\theta)μ(x,θ)≤μ(x∗(θ),θ). They make every integrand bounded and measurable, so no integrability hypothesis is added.
  • An algorithm is a behavioural policy, giving a probability vector over actions for each history. Under perfect recall this is equivalent to an algorithm with internal randomization. Periods are 0-based in Lean: Lean period sss is tutorial period t=s+1t=s+1t=s+1.
  • Logarithms are natural in both III and HHH. The conditional mutual information is defined directly as an average of Kullback–Leibler divergences, with joint probabilities. It is not defined as a difference of unconditional mutual informations: that would make the chain rule true by definition and empty milestone 3. Γt\Gamma_tΓt​ is never written as a quotient in the goal, so a period with zero information cannot turn the bound into one with Γˉ=0\bar\Gamma=0Γˉ=0.
  • Needed infrastructure: marginalisation over later periods of the history law, the chain rule of conditional mutual information for finite variables averaged against a general prior, and I(x∗;HT)≤H(x∗)I(x^*;\mathbb H_T)\le H(x^*)I(x∗;HT​)≤H(x∗). The Proved platform results InformationTheory.kernel_average_categorical_kl_le_marginal_entropy and its _general variant (average KL to the mixture is at most the mixture's entropy), and the adversarial-bandit lemmas BanditAlgorithm.bayesian_ts_conditional_information_gain_chain_rule and bayesian_history_mutualInformation_endpoint_bound, are related tools. A chain-rule library for this history model would be reusable beyond this mission, for example for information-directed sampling. Proofs of auxiliary lemmas are welcome.

The tutorial's argument is on pp. 75–76. The tutorial cites Russo and Van Roy (2016) for the original results, including the entropy budget.

Selected references

  • D. J. Russo, B. Van Roy, A. Kazerouni, I. Osband, Z. Wen, A Tutorial on Thompson Sampling, Foundations and Trends in Machine Learning 11(1):1–96, 2018. https://doi.org/10.1561/2200000070
  • D. Russo, B. Van Roy, An Information-Theoretic Analysis of Thompson Sampling, Journal of Machine Learning Research 17(68):1–30, 2016. https://jmlr.org/papers/v17/14-087.html (arXiv: https://arxiv.org/abs/1403.5341)
  • D. Russo, B. Van Roy, Learning to Optimize via Information-Directed Sampling, Operations Research 66(1):230–252, 2018. https://doi.org/10.1287/opre.2017.1663
  • D. Russo, B. Van Roy, Satisficing in Time-Sensitive Bandit Learning, arXiv preprint, 2018. https://arxiv.org/abs/1803.02855
  • T. Lattimore, C. Szepesvári, Bandit Algorithms, Cambridge University Press, 2020, Chapter 36. https://doi.org/10.1017/9781108571401
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Mathematical PhysicsQuantum Information·Captain: wurtle

The entropy photon-number inequalityResearch Paper

Motivation

Shannon's entropy power inequality bounds the entropy of a sum of independent random vectors below by the entropies of the summands; it is a basic tool for classical Gaussian channel capacities. In optical communication, addition is replaced by passive mixing of bosonic modes at a beam splitter. Guha, Erkmen and Shapiro conjectured the sharp bosonic analogue, the entropy photon-number inequality (EPnI), stated in terms of the photon number of the thermal state with the same entropy (ITA 2008). If true, it settles the minimum output entropy of thermal attenuators at fixed input entropy and the capacity regions of bosonic broadcast and wiretap channels, which had been reduced to this inequality (PRA 2007).

This mission asks for a formal proof of the EPnI for finite-energy inputs in any finite number of modes, as stated in an OpenAI preprint dated September 24, 2026 (source). The preprint has not been peer reviewed and its claims have not been independently verified; on the platform the Lean goal is open.

Background

  • 1948–1965 — Shannon introduces entropy power; Stam (1959) and Blachman (IEEE IT 1965) prove the entropy power inequality.
  • 2004 — Capacity of the pure-loss bosonic channel (PRL 2004) and the minimum-output-entropy conjecture (PRA 2004).
  • 2007–2008 — Guha, Shapiro and Erkmen relate broadcast capacity to a minimum-output-entropy conjecture; Guha, Erkmen and Shapiro state the EPnI.
  • 2011 — Special cases (one-mode number-diagonal inputs) by Das, Sharma and Muthukrishnan (arXiv:1107.2365).
  • 2014 — König and Smith prove a quantum entropy power inequality, including S(ρC)≥ηS(ρA)+(1−η)S(ρB)S(\rho_C)\ge\eta S(\rho_A)+(1-\eta)S(\rho_B)S(ρC​)≥ηS(ρA​)+(1−η)S(ρB​) (IEEE IT 2014); De Palma, Mari and Giovannetti prove the exponential form eS(ρC)/n≥ηeS(ρA)/n+(1−η)eS(ρB)/ne^{S(\rho_C)/n}\ge\eta e^{S(\rho_A)/n}+(1-\eta)e^{S(\rho_B)/n}eS(ρC​)/n≥ηeS(ρA​)/n+(1−η)eS(ρB​)/n (Nat. Photonics 2014).
  • 2015 — Giovannetti, Holevo and García-Patrón solve the Gaussian optimizer conjecture for unconstrained minimum output entropy (CMP 2015).
  • 2016–2018 — De Palma, Trevisan and Giovannetti settle one-mode constrained problems (IEEE IT 2017; PRL 2017); De Palma and Trevisan give a rigorous finite-energy conditional EPI (CMP 2018).
  • September 2026 — The OpenAI preprint claims the two-input EPnI for all finite-energy inputs (Theorem 1.1, p. 2).

Setting

An nnn-mode bosonic system has Fock space ℓ2(Nn)\ell^2(\mathbb N^n)ℓ2(Nn) with number basis ∣k⟩|k\rangle∣k⟩, k∈Nnk\in\mathbb N^nk∈Nn. A state is a positive trace-one operator ρ\rhoρ; it has finite energy if Tr⁡ρ∑jaj†aj=∑k(k1+⋯+kn)⟨k∣ρ∣k⟩<∞\operatorname{Tr}\rho\sum_ja_j^\dagger a_j=\sum_k(k_1+\dots+k_n)\langle k|\rho|k\rangle<\inftyTrρ∑j​aj†​aj​=∑k​(k1​+⋯+kn​)⟨k∣ρ∣k⟩<∞. The von Neumann entropy is S(ρ)=−Tr⁡ρlog⁡ρS(\rho)=-\operatorname{Tr}\rho\log\rhoS(ρ)=−Trρlogρ (natural log). The thermal entropy per mode is

g(t)=(t+1)log⁡(t+1)−tlog⁡t,t≥0,g(t)=(t+1)\log(t+1)-t\log t,\qquad t\ge0,g(t)=(t+1)log(t+1)−tlogt,t≥0,

increasing from 000 to ∞\infty∞, and the entropy photon number of ρ\rhoρ is N(ρ)=g−1(S(ρ)/n)N(\rho)=g^{-1}(S(\rho)/n)N(ρ)=g−1(S(ρ)/n), the mean photon number per mode of the product thermal state with the same entropy. For independent inputs ρA,ρB\rho_A,\rho_BρA​,ρB​ and transmissivity 0≤η≤10\le\eta\le10≤η≤1, the beam-splitter output ρC\rho_CρC​ is the reduced state of the modes cj=η aj+1−η bjc_j=\sqrt\eta\,a_j+\sqrt{1-\eta}\,b_jcj​=η​aj​+1−η​bj​ after passive mixing of ρA⊗ρB\rho_A\otimes\rho_BρA​⊗ρB​. No independence among the modes within either input is assumed.

Formalization targets

Goal: Theorem 1.1 (p. 2)

For every finite n≥1n\ge1n≥1, every pair of finite-energy nnn-mode states ρA,ρB\rho_A,\rho_BρA​,ρB​ and every 0≤η≤10\le\eta\le10≤η≤1,

g−1 ⁣(S(ρC)n) ≥ η g−1 ⁣(S(ρA)n)+(1−η) g−1 ⁣(S(ρB)n).g^{-1}\!\Bigl(\frac{S(\rho_C)}n\Bigr)\ \ge\ \eta\,g^{-1}\!\Bigl(\frac{S(\rho_A)}n\Bigr)+(1-\eta)\,g^{-1}\!\Bigl(\frac{S(\rho_B)}n\Bigr).g−1(nS(ρC​)​) ≥ ηg−1(nS(ρA​)​)+(1−η)g−1(nS(ρB​)​).

Thermal inputs with a common mean photon number within each port give equality.

Significance

The result itself. The EPnI is sharper than the exponential quantum entropy power inequality when the two input entropies differ, which is exactly the regime needed for constrained minimum output entropy. The preprint derives the exact minimum output entropy at fixed input entropy for every tensor power of an identical thermal attenuator, with inputs entangled across modes (Corollary 1.2, p. 2), and the exact capacity region of the degraded two-receiver pure-loss broadcast channel (Corollary 7.1, p. 26), completing the converse of Guha, Shapiro and Erkmen.

Formalizing it. The statement involves infinite-dimensional Fock space, trace-class positive operators, continuous functional calculus for the entropy, and the partial trace after a passive unitary. The Lean development builds these concretely in the number basis. A formal proof would give machine-checked infrastructure for quantum entropy on infinite-dimensional spaces, which Mathlib currently lacks. No machine-checked version of any quantum entropy power inequality is known.

Difficulty

Heat-flow (quantum Fisher information) proofs give the linear and exponential bounds, but these are attained only for equal entropies and do not recover the thermal comparison at unequal entropy levels. The preprint instead minimizes a regularized functional over pairs of inputs and must show that minimizers are thermal. This requires an interpolation theorem for diagonal form comparisons (Theorem 3.1, p. 8), attainment and Gibbs regularity of minimizers in infinite dimensions (Lemma 4.1, Proposition 4.2, pp. 15–16), a component entropy-Hessian estimate, and a stationarity identity whose cancellation forces convergence to thermal inputs (Section 6). Compactness relies on the finite-energy hypothesis; without it entropies can be infinite.

Formalization scope

  • Fock n is lp (fun _ : Fin n → ℕ => ℂ) 2. A State is a positive bounded operator whose diagonal in the number basis sums (HasSum) to 111.
  • FiniteEnergy ρ is summability of ∑k∣k∣ ⟨k∣ρ∣k⟩\sum_k|k|\,\langle k|\rho|k\rangle∑k​∣k∣⟨k∣ρ∣k⟩.
  • entropy ρ is the sum of diagonal entries of cfc(−tlog⁡t)(ρ)\mathrm{cfc}(-t\log t)(\rho)cfc(−tlogt)(ρ); for finite-energy states it is finite, so the tsum is the true entropy.
  • gInv s = sInf {t ≥ 0 | s ≤ g t}, the inverse of ggg on [0,∞)[0,\infty)[0,∞).
  • IsBeamSplitterOutput η ρA ρB ρC requires every number-basis entry of ρC\rho_CρC​ to be the (convergent) partial-trace sum of the explicitly given beam-splitter coefficients applied to ρA⊗ρB\rho_A\otimes\rho_BρA​⊗ρB​; the inputs are arbitrary density matrices, so internal entanglement is allowed.
  • The hypotheses are satisfiable (e.g. vacuum or thermal inputs) and the conclusion is the inequality as stated.

Selected references

  • OpenAI, The entropy photon-number inequality, OpenAI Math Release preprint, September 24, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/The-entropy-photon-number-inequality-September-24-2026/paper.pdf
  • S. Guha, B. I. Erkmen, J. H. Shapiro, The entropy photon-number inequality and its consequences, ITA Workshop 2008, 128–130. https://doi.org/10.1109/ITA.2008.4601037
  • S. Guha, J. H. Shapiro, B. I. Erkmen, Classical capacity of bosonic broadcast communication and a minimum output entropy conjecture, Phys. Rev. A 76 (2007), 032303. https://doi.org/10.1103/PhysRevA.76.032303
  • R. König, G. Smith, The entropy power inequality for quantum systems, IEEE Trans. Inf. Theory 60 (2014), 1536–1548. https://doi.org/10.1109/TIT.2014.2298436
  • G. De Palma, A. Mari, V. Giovannetti, A generalization of the entropy power inequality to bosonic quantum systems, Nat. Photonics 8 (2014), 958–964. https://doi.org/10.1038/nphoton.2014.252
  • G. De Palma, D. Trevisan, The conditional entropy power inequality for bosonic quantum systems, Comm. Math. Phys. 360 (2018), 639–662. https://doi.org/10.1007/s00220-017-3082-8
  • V. Giovannetti, A. S. Holevo, R. García-Patrón, A solution of Gaussian optimizer conjecture for quantum channels, Comm. Math. Phys. 334 (2015), 1553–1571. https://doi.org/10.1007/s00220-014-2150-6
  • V. Giovannetti, S. Guha, S. Lloyd, L. Maccone, J. H. Shapiro, H. P. Yuen, Classical capacity of the lossy bosonic channel: the exact solution, Phys. Rev. Lett. 92 (2004), 027902. https://doi.org/10.1103/PhysRevLett.92.027902
  • C. E. Shannon, A mathematical theory of communication, Bell Syst. Tech. J. 27 (1948). https://doi.org/10.1002/j.1538-7305.1948.tb00917.x
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Quantum InformationStatistics·Captain: mikedeng1

Shadow Tomography of Quantum States 2: Even the Classical Special Case Needs Ω(min{D, log M}/ε²) CopiesResearch Paper

Why the copy count matters

Shadow tomography asks for predictions of many specified measurements of an unknown quantum state, while using as few prepared copies of that state as possible. The requested output is a list of acceptance probabilities, not a full description of the state. A procedure might exploit the fact that these are only MMM numbers, even when the state has dimension DDD. The natural question is how far this saving can go. Aaronson's paper gives upper bounds and separates two sources of difficulty: one already present for ordinary probability distributions, and one arising from noncommuting quantum measurements.

This mission concerns the first source. It formalizes Theorem 16, which says that even when the state and every requested measurement are diagonal in the same basis, the number of copies must grow with min⁡{D,log⁡M}/ε2\min\{D,\log M\}/\varepsilon^2min{D,logM}/ε2 in the relevant asymptotic regime. In that special case, the unknown state is an ordinary distribution on DDD outcomes. The theorem therefore puts a limit on any proposed improvement to shadow tomography that would promise fewer copies in all instances.

States, measurements, and estimates

A mixed state ρ\rhoρ on a DDD-dimensional system is a positive semidefinite D×DD\times DD×D complex matrix with trace one. A two-outcome measurement is represented by an effect EEE satisfying 0⪯E⪯I0\preceq E\preceq I0⪯E⪯I; it accepts ρ\rhoρ with probability Tr⁡(Eρ)\operatorname{Tr}(E\rho)Tr(Eρ). When ρ\rhoρ is diagonal, its diagonal entries are the probabilities of the DDD basis outcomes. When EEE is diagonal too, it specifies a randomized yes-or-no test on those outcomes. These conventions are stated in Section 3 of the paper.

Given effects E1,…,EME_1,\ldots,E_ME1​,…,EM​, a shadow-tomography strategy measures kkk independent copies ρ⊗k\rho^{\otimes k}ρ⊗k and outputs estimates b1,…,bMb_1,\ldots,b_Mb1​,…,bM​. It succeeds on ρ\rhoρ when every estimate differs from Tr⁡(Eiρ)\operatorname{Tr}(E_i\rho)Tr(Ei​ρ) by at most ε\varepsilonε. The lower bound requires success probability at least 2/32/32/3 for every diagonal mixed state. The strategy may make a joint quantum measurement on all copies and may choose its estimates from its observed outcome. This is the same measurement model used in Problem 1.

Formalization targets

Classical special-case lower bound

The goal is the classical clause of Theorem 16. There are absolute constants c>0c>0c>0 and N0N_0N0​ such that, for D≥N0D\ge N_0D≥N0​, log⁡2M≥N0\log_2 M\ge N_0log2​M≥N0​, and 0<ε≤1/60<\varepsilon\le1/60<ε≤1/6, there are MMM diagonal effects with 0/1 entries, corresponding to the known Boolean functions in Section 6.1, for which every strategy successful on all diagonal states must use

k≥c min⁡{D,log⁡2M}ε2.k\ge c\,\frac{\min\{D,\log_2 M\}}{\varepsilon^2}.k≥cε2min{D,log2​M}​.

The hard measurements are chosen before the strategy is quantified. The statement therefore also rules out a strategy with a smaller copy count that works uniformly for all quantum states and measurements. Its constants and threshold express the Ω\OmegaΩ notation in Theorem 16, rather than specifying a numerical optimum.

Supporting targets

Four milestones come from the proof on pages 20–21: the high-probability overlap bound for independently chosen half-size subsets (Eq. (1)); the acceptance probability of a subset under its associated biased distribution; an upper bound on the mutual information between the hidden subset index and the observed samples; and the exact entropy formula with a quadratic entropy deficit. These statements expose the combinatorial and information-theoretic parts of the lower bound while leaving the goal as the paper's copy-complexity result.

What the result supplies

Theorem 16 sets a floor for shadow tomography that survives even when all operators commute. Any uniform copy bound for the full quantum task must respect this floor. The result also distinguishes the difficulty of predicting many properties of a distribution from the extra difficulty possible for noncommuting states and measurements, which the paper treats in a separate lower bound. Section 6 presents both bounds.

A complete formalization would give machine-checked statements and proofs for the finite subset construction, the entropy calculation, the information inequality, and the reduction from a successful quantum measurement procedure on diagonal states to a lower bound on kkk. The theorem is proved on paper; these draft statements are open Lean goals and do not claim that its proof has been machine checked. The finite-distribution and information-theory infrastructure is reusable for other lower bounds based on hidden-index families.

Where the argument is delicate

Counting how many possible measurements there are does not by itself show that samples reveal enough about which distribution generated them. The lower bound needs a quantitative relation between estimation accuracy and information about a hidden index, while each individual sample carries limited information. The paper's printed overlap condition (1) is too weak for the next displayed ε/2\varepsilon/2ε/2 estimate: at its boundary it gives ε\varepsilonε. The milestone preserves Eq. (1) as printed; closing the goal requires the correspondingly sharper overlap fact with N/24N/24N/24, which follows from the same type of concentration statement after adjusting its constant. The printed assertion that learning the index requires mutual information at least log⁡2K\log_2 Klog2​K is also imprecise at success probability 2/32/32/3; a quantitative decoding inequality is needed. Neither incorrect display is a draft milestone.

Formalization scope

Matrices are indexed by Fin D. WildeQIT.IsDensityOperator supplies the mixed-state predicate ρ⪰0\rho\succeq0ρ⪰0 and Tr⁡(ρ)=1\operatorname{Tr}(\rho)=1Tr(ρ)=1. Diagonal states and effects use the standard matrix diagonal predicate. An effect is positive semidefinite together with its complement. The tensor power uses functions Fin k → Fin D as basis indices; at k=0k=0k=0 it is a one-by-one identity matrix. A strategy is a finite-outcome POVM on that tensor power, followed by a real estimate vector for each outcome. The output values are not restricted to [0,1][0,1][0,1]: clipping them to this interval cannot worsen an estimate of a probability. No restriction to classical estimators is placed in the goal; that would change the allowed strategies before the theorem has been proved.

The asymptotic threshold excludes the one-dimensional and single-measurement corners where the claimed rate does not describe the problem. The bound ε≤1/6\varepsilon\le1/6ε≤1/6 keeps the biased distributions used on page 20 nonnegative; ε≥1/2\varepsilon\ge1/2ε≥1/2 would permit a zero-copy constant estimate. Subset milestones require even NNN or explicitly require a half-size subset, so N/2N/2N/2 has its intended meaning. The natural logarithm appears nowhere in the lower-bound rate; entropy, mutual information, and log⁡2M\log_2 Mlog2​M use base two. At zero probability the entropy convention is 0log⁡0=00\log 0=00log0=0.

The finite distributions, entropy, conditional entropy, and mutual information reuse the published WildeQIT definitions. Contributions that prove the four source milestones, establish the sharper overlap fact, or supply the quantitative decoding step are welcome. The goal must retain its order of quantifiers: one hard measurement family, then every strategy, with success demanded on every diagonal state.

Selected references

  • Scott Aaronson, Shadow Tomography of Quantum States, arXiv preprint arXiv:1711.01053v2, 2018. Preprint.
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Operations ResearchProbability·Captain: mikedeng1

Conditional and Dynamic Convex Risk Measures II: The Conditional Entropic Risk Measure and Conditional Relative EntropyResearch Paper

Motivation

A risk measure assigns to a random financial position XXX a capital requirement ρ(X)\rho(X)ρ(X): the amount of cash that must be added to XXX to make it acceptable. The axiomatic theory of convex risk measures (Föllmer–Schied 2002; Frittelli–Rosazza Gianin 2002) treats this number as computed with no information beyond the model. In practice a regulator or a risk manager revises the requirement as information arrives, so the requirement becomes a random variable measurable with respect to the information available at the time of measurement. Detlefsen and Scandolo (SFB 649 Discussion Paper 2005-006; published in Finance and Stochastics 9(4), 2005, doi:10.1007/s00780-005-0159-6) develop this conditional theory: axioms, a robust representation, and a treatment of dynamic risk measurement.

The entropic risk measure is the standard example of a convex risk measure that is not coherent. It is the capital requirement of an agent with exponential utility uγ(x)=1−e−γxu_\gamma(x)=1-e^{-\gamma x}uγ​(x)=1−e−γx, and its penalty function in the robust representation is the relative entropy 1γH(Q∣P)\frac1\gamma H(Q\mid P)γ1​H(Q∣P) (Föllmer–Schied, Stochastic Finance, Example 4.60, as cited by the paper). Section 5 of the paper carries this example to the conditional setting and shows that its penalty is a conditional relative entropy. The same identity appears in dynamic entropic risk measures, exponential-utility indifference pricing and recursive utility, where one-period conditional entropic measures are composed over time.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) and a sub-σ\sigmaσ-algebra G⊆F\mathcal G\subseteq\mathcal FG⊆F, the information available at the time of measurement. L∞L^\inftyL∞ is the space of essentially bounded random variables and LG∞L^\infty_{\mathcal G}LG∞​ its G\mathcal GG-measurable part. All equalities and inequalities between random variables hold PPP-almost surely.

A conditional convex risk measure is a map ρ:L∞→LG∞\rho:L^\infty\to L^\infty_{\mathcal G}ρ:L∞→LG∞​ that is translation invariant (ρ(X+Z)=ρ(X)−Z\rho(X+Z)=\rho(X)-Zρ(X+Z)=ρ(X)−Z for Z∈LG∞Z\in L^\infty_{\mathcal G}Z∈LG∞​), monotone (X≤Y⇒ρ(X)≥ρ(Y)X\le Y\Rightarrow\rho(X)\ge\rho(Y)X≤Y⇒ρ(X)≥ρ(Y)), conditionally convex (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∈LG∞\Lambda\in L^\infty_{\mathcal G}Λ∈LG∞​, 0≤Λ≤10\le\Lambda\le10≤Λ≤1), and satisfies ρ(0)=0\rho(0)=0ρ(0)=0.

The relevant probability models are

PG={Q probability on (Ω,F):Q≪P, Q(A)=P(A) for all A∈G}.\mathcal P_{\mathcal G}=\{Q \text{ probability on } (\Omega,\mathcal F) : Q\ll P,\ Q(A)=P(A)\ \text{for all } A\in\mathcal G\}.PG​={Q probability on (Ω,F):Q≪P, Q(A)=P(A) for all A∈G}.

The essential supremum of a family X\mathcal XX of [−∞,+∞][-\infty,+\infty][−∞,+∞]-valued random variables is the a.s. smallest random variable that dominates every member a.s.; the essential infimum is defined symmetrically. The minimal penalty of ρ\rhoρ is

α∗(Q)=ess.sup⁡X∈L∞{−EQ(X∣G)−ρ(X)},Q∈PG.\alpha^*(Q)=\operatorname{ess.sup}_{X\in L^\infty}\{-E_Q(X\mid\mathcal G)-\rho(X)\},\qquad Q\in\mathcal P_{\mathcal G}.α∗(Q)=ess.supX∈L∞​{−EQ​(X∣G)−ρ(X)},Q∈PG​.

For a risk aversion γ>0\gamma>0γ>0, the conditional entropic risk measure is

ργ(X)=1γlog⁡EP(e−γX∣G),\rho_\gamma(X)=\frac1\gamma\log E_P\big(e^{-\gamma X}\mid\mathcal G\big),ργ​(X)=γ1​logEP​(e−γX∣G),

the capital requirement for the acceptance set Aγ={X∈L∞:EP(e−γX∣G)≤1}A_\gamma=\{X\in L^\infty : E_P(e^{-\gamma X}\mid\mathcal G)\le1\}Aγ​={X∈L∞:EP​(e−γX∣G)≤1}. For Q∈PGQ\in\mathcal P_{\mathcal G}Q∈PG​ with density φ=dQ/dP\varphi=dQ/dPφ=dQ/dP, the conditional relative entropy is

HG(Q∣P)=EP(φlog⁡φ∣G)∈[0,+∞],0log⁡0=0.H_{\mathcal G}(Q\mid P)=E_P(\varphi\log\varphi\mid\mathcal G)\in[0,+\infty],\qquad 0\log0=0.HG​(Q∣P)=EP​(φlogφ∣G)∈[0,+∞],0log0=0.

Formalization targets

Goal: Proposition 5.4

For every γ>0\gamma>0γ>0:

ργ(X)=ess.sup⁡Q∈PG{−EQ(X∣G)−1γHG(Q∣P)}(X∈L∞),α∗(Q)=1γHG(Q∣P)(Q∈PG).\rho_\gamma(X)=\operatorname{ess.sup}_{Q\in\mathcal P_{\mathcal G}}\Big\{-E_Q(X\mid\mathcal G)-\tfrac1\gamma H_{\mathcal G}(Q\mid P)\Big\}\quad(X\in L^\infty),\qquad \alpha^*(Q)=\tfrac1\gamma H_{\mathcal G}(Q\mid P)\quad(Q\in\mathcal P_{\mathcal G}).ργ​(X)=ess.supQ∈PG​​{−EQ​(X∣G)−γ1​HG​(Q∣P)}(X∈L∞),α∗(Q)=γ1​HG​(Q∣P)(Q∈PG​).

The first identity is representability with the minimal penalty as the penalty; the second identifies that penalty.

Milestones

  1. (Section 5, p. 12) ργ\rho_\gammaργ​ is a conditional convex risk measure.
  2. (Section 5, p. 12) ργ(X)=ess.inf⁡{Y∈LG∞:X+Y∈Aγ}=ess.inf⁡{Y∈LG∞:EP(e−γX∣G)≤eγY}\rho_\gamma(X)=\operatorname{ess.inf}\{Y\in L^\infty_{\mathcal G}: X+Y\in A_\gamma\}=\operatorname{ess.inf}\{Y\in L^\infty_{\mathcal G}: E_P(e^{-\gamma X}\mid\mathcal G)\le e^{\gamma Y}\}ργ​(X)=ess.inf{Y∈LG∞​:X+Y∈Aγ​}=ess.inf{Y∈LG∞​:EP​(e−γX∣G)≤eγY}.
  3. (Proof of Proposition 5.4) ργ\rho_\gammaργ​ is continuous from above: Xn↘XX_n\searrow XXn​↘X implies ργ(Xn)↗ργ(X)\rho_\gamma(X_n)\nearrow\rho_\gamma(X)ργ​(Xn​)↗ργ​(X).
  4. (Section 5, p. 13) For Q∈PGQ\in\mathcal P_{\mathcal G}Q∈PG​: EP(φ∣G)=1E_P(\varphi\mid\mathcal G)=1EP​(φ∣G)=1 and HG(Q∣P)=EQ(log⁡φ∣G)H_{\mathcal G}(Q\mid P)=E_Q(\log\varphi\mid\mathcal G)HG​(Q∣P)=EQ​(logφ∣G).
  5. (Proof of Proposition 5.4) α∗(Q)=1γess.sup⁡Z∈L∞{EQ(Z∣G)−log⁡EP(eZ∣G)}\alpha^*(Q)=\frac1\gamma\operatorname{ess.sup}_{Z\in L^\infty}\{E_Q(Z\mid\mathcal G)-\log E_P(e^Z\mid\mathcal G)\}α∗(Q)=γ1​ess.supZ∈L∞​{EQ​(Z∣G)−logEP​(eZ∣G)}.
  6. (Lemma 5.5) The conditional Donsker–Varadhan formula
ess.sup⁡Z∈L∞{EQ(Z∣G)−log⁡EP(eZ∣G)}=HG(Q∣P),Q∈PG.\operatorname{ess.sup}_{Z\in L^\infty}\{E_Q(Z\mid\mathcal G)-\log E_P(e^Z\mid\mathcal G)\}=H_{\mathcal G}(Q\mid P),\qquad Q\in\mathcal P_{\mathcal G}.ess.supZ∈L∞​{EQ​(Z∣G)−logEP​(eZ∣G)}=HG​(Q∣P),Q∈PG​.

Significance

The result gives the conditional entropic risk measure an explicit dual description: the capital requirement is a worst case over conditional models, each penalized by its conditional relative entropy. This duality is what makes entropic risk measures computable in dynamic settings. Recursive compositions of ργ\rho_\gammaργ​ over a filtration are time consistent, and their penalties add up by the chain rule for conditional relative entropy. Lemma 5.5 is also the conditional form of the Donsker–Varadhan (Gibbs) variational principle, which is used on its own in large deviations and in PAC-Bayesian bounds.

On status: the results are proved in the paper, and the unconditional versions are textbook material. Mathlib has unconditional Kullback–Leibler divergence, tilted measures, conditional Jensen's inequality and a [0,+∞][0,+\infty][0,+∞]-valued conditional expectation. As far as the platform search could establish, neither the conditional relative entropy nor the conditional Donsker–Varadhan formula nor any conditional risk measure has been formalized. This mission produces the first machine-checked conditional version, with HGH_{\mathcal G}HG​ allowed to be infinite.

Difficulty

In the unconditional case both sides of Lemma 5.5 are numbers, and the supremum is a supremum over reals. Conditionally, both sides are random variables. The supremum over the uncountable family indexed by L∞L^\inftyL∞ must be taken in the essential sense, and a pointwise supremum is neither measurable nor meaningful. The conditional relative entropy can be +∞+\infty+∞ on a set of positive probability. The integrand φlog⁡φ\varphi\log\varphiφlogφ need not be integrable, so the usual conditional expectation of L1L^1L1 is not available for it, and the "≥\ge≥" direction must reach an unbounded target through bounded test variables while controlling log⁡EP(eZ∣G)\log E_P(e^{Z}\mid\mathcal G)logEP​(eZ∣G) at the same time. The ess.sup in the goal ranges over measures, not random variables, and each EQ(⋅∣G)E_Q(\cdot\mid\mathcal G)EQ​(⋅∣G) is a conditional expectation under a different measure. These are identified with PPP-a.s. objects through the condition Q=PQ=PQ=P on G\mathcal GG.

Formalization scope

  • (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) is a probability space (IsProbabilityMeasure P), and G\mathcal GG is m : MeasurableSpace Ω with hm : m ≤ mΩ. Payoffs are real functions with MemLp X ⊤ P. LG∞L^\infty_{\mathcal G}LG∞​ membership is StronglyMeasurable[m] plus MemLp ⊤. Every (in)equality between random variables is PPP-a.e.
  • PG\mathcal P_{\mathcal G}PG​ is the subtype of probability measures Q≪PQ\ll PQ≪P with Q(A)=P(A)Q(A)=P(A)Q(A)=P(A) for all A∈GA\in\mathcal GA∈G. This is equality on G\mathcal GG, not equivalence of measures.
  • EP(⋅∣G)E_P(\cdot\mid\mathcal G)EP​(⋅∣G) and EQ(⋅∣G)E_Q(\cdot\mid\mathcal G)EQ​(⋅∣G) on bounded variables are Mathlib's conditional expectations P[·|m] and Q[·|m]. Bounded variables are integrable under every Q≪PQ\ll PQ≪P, so no junk value arises.
  • ργ\rho_\gammaργ​ is the paper's closed form 1γlog⁡EP(e−γX∣G)\frac1\gamma\log E_P(e^{-\gamma X}\mid\mathcal G)γ1​logEP​(e−γX∣G). The ess.inf descriptions are a milestone, and no positivity hypothesis on XXX is imposed.
  • φ\varphiφ is the real part of the Radon–Nikodym derivative Q.rnDeriv P. HG(Q∣P)H_{\mathcal G}(Q\mid P)HG​(Q∣P) and EQ(log⁡φ∣G)E_Q(\log\varphi\mid\mathcal G)EQ​(logφ∣G) are generalized conditional expectations, E(f+∣G)−E(f−∣G)E(f^+\mid\mathcal G)-E(f^-\mid\mathcal G)E(f+∣G)−E(f−∣G), built from Mathlib's [0,+∞][0,+\infty][0,+∞]-valued condLExp and valued in EReal. The negative parts are integrable, so +∞−(+∞)+\infty-(+\infty)+∞−(+∞) never arises. In EReal, a real number minus +∞+\infty+∞ is −∞-\infty−∞, which is how a model with infinite entropy drops out of the supremum.
  • Essential suprema and infima are predicates (IsEssSup, IsEssInf) on a candidate PPP-a.e. measurable EReal-valued function. The candidate must dominate every member a.s. and lie a.s. below every a.s. upper bound.
  • Continuity from above means: a.s. monotone convergence Xn↘XX_n\searrow XXn​↘X in L∞L^\inftyL∞ implies a.s. monotone convergence ρ(Xn)↗ρ(X)\rho(X_n)\nearrow\rho(X)ρ(Xn​)↗ρ(X).
  • γ\gammaγ is a real constant with γ>0\gamma>0γ>0. The random risk aversion of Remark 5.6 is not formalized.
  • Ruled out: defining HGH_{\mathcal G}HG​ through the Bochner conditional expectation P[φ * log φ | m] (which returns 000 when φlog⁡φ\varphi\log\varphiφlogφ is not integrable) or α∗\alpha^*α∗ through a pointwise supremum would make the goal false or vacuous, and so would stating it for an abstract convex risk measure in place of ργ\rho_\gammaργ​. The formalization uses the extended-valued HGH_{\mathcal G}HG​, the essential supremum, and the explicit ργ\rho_\gammaργ​.
  • The mission is self-contained. It redefines conditional convex risk measures, PG\mathcal P_{\mathcal G}PG​ and the essential supremum in its own namespace CondConvexRisk.Entropic and does not assume the general representation theorem (Theorem 3.2). The generalized conditional expectation and the conditional Donsker–Varadhan formula are reusable beyond risk measures. Contributions are welcome on the ess.sup API (existence, upward-directed families), on conditional monotone convergence for condExp, and on the conditional Jensen step for xlog⁡xx\log xxlogx.

Selected references

  • S. Detlefsen, G. Scandolo, Conditional and Dynamic Convex Risk Measures, SFB 649 Discussion Paper 2005-006, Humboldt-Universität zu Berlin, 2005 (the version formalized; published in Finance and Stochastics 9(4), 2005, https://doi.org/10.1007/s00780-005-0159-6).
  • H. Föllmer, A. Schied, Stochastic Finance: An Introduction in Discrete Time, de Gruyter, Berlin, 2002 (reference [8] of the paper).
  • H. Föllmer, A. Schied, Convex measures of risk and trading constraints, Finance and Stochastics 6:429–447, 2002. https://doi.org/10.1007/s007800200072
  • M. D. Donsker, S. R. S. Varadhan, Asymptotic evaluation of certain Markov process expectations for large time, III, Comm. Pure Appl. Math. 29:389–461, 1976. https://doi.org/10.1002/cpa.3160290405
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Active InferenceProbability·Captain: ActiveInference

Free Energy Principle II: expected free energy, Markov blankets, Gaussian variational free energy, and Bayesian model reductionResearch Paper

Free Energy Principle II: expected free energy, Markov blankets, Gaussian variational free energy, and Bayesian model reduction

Motivation

Mission Free Energy Principle I published the core variational step of the free energy principle (FEP): whatever recognition density a system carries, the posterior-form variational free energy never undercuts the data's surprisal, the bound is exact at the Bayesian posterior, and equality characterizes the posterior. That mission's shared finite substrate — normalized finite laws, finite kernels, entropy/cross-entropy/KL, and the finite generative model — now exists as platform definitions in the namespace FreeEnergyPrinciple.

The Free Energy Principle II mission formalizes the four structures the FEP literature builds on top of that core, all already machine-checked in the source repository fep_lean / fep_formal (Active Inference Institute):

  • Expected free energy — the policy-selection functional of active inference: what a course of action is expected to cost in preference divergence and what it is expected to reveal. Its canonical decomposition [Friston et al. 2017] splits GGG into risk (pragmatic divergence of predicted outcomes from preferences) plus ambiguity (expected entropy of outcomes given latent states), with epistemic value fixing the sign.
  • Markov blankets — the partition that makes a self-organizing system statable: internal states are conditionally independent of external states given the sensory-active blanket. The source development proves this at the level of Mathlib's native conditional distributions, not as a finite mutual-information proxy.
  • Gaussian variational free energy — the closed-form instantiation of the FEP-I bound for the exact scalar Gaussian filter, where the native Gaussian KL is exactly the squared mean error over twice the posterior variance.
  • Bayesian model reduction — model comparison by Bayes factors: posterior odds equal prior odds times the likelihood ratio, the multiplicative update applied whenever a reduced model is compared against the model it was reduced from [Friston & Penny 2011].

Timeline of the mathematical content this mission formalizes:

  • 2006/2010 — Friston's free energy principle: variational free energy as the quantity a self-organizing system minimizes (formalized in FEP-I).
  • 2011 — Friston & Penny, Post hoc Bayesian model selection: Bayesian model reduction — evidence of reduced models evaluated by the free-energy difference; comparison by Bayes factors.
  • 2015 — Friston, Rigoli, Sengupta, Pezzulo — the Markov-blanket partition (sensory/active states) as the geometry of the FEP.
  • 2017 — Friston, FitzGerald, Rigoli, Schwartenbeck, Pezzulo, Active inference: a process theory: expected free energy G(π)=risk+ambiguityG(\pi) = \text{risk} + \text{ambiguity}G(π)=risk+ambiguity drives policy selection.
  • 2022 — Parr, Pezzulo, Friston, Active Inference (MIT Press): Gaussian treatments of filtering and the posterior-form free energy as the working equations.
  • 2026 — fep_formal (Active Inference Institute): a machine-checked Lean 4 catalogue of 155 FEP topics compiled with zero proof holes against a pinned Mathlib. This mission transcribes the proved modules behind expected free energy, native Markov blankets, the scalar Gaussian filter/VFE, and Bayesian model reduction onto the platform.

Setting

Two carriers, both fully machine-checked in the source repository:

  • Finite (reusing FEP-I's published substrate). Laws are normalized real mass functions on finite types; kernels are normalized rows. This mission's expected-free-energy, model-reduction, and Markov-blanket families import the published Definitions.Def_fep_finite_laws, Def_fep_finite_information, and Def_fep_generative_model — no substrate is re-published. Zero-mass atoms are handled by the same totalized conventions as FEP-I: entropy uses Real.negMulLog (so 0log⁡0=00\log 0 = 00log0=0 exactly), KL is the nonnegative klFun integrand, and division premises are explicit.
  • Native Gaussian (self-contained on Mathlib). The Gaussian family is Mathlib's own gaussianReal/gaussianPDF at a fixed strictly positive variance; the scalar OU prediction and the closed filter update give the posterior mean/variance the recognition family varies over. The native KL between two family members is exactly (μ1−μ2)22v\frac{(\mu_1-\mu_2)^2}{2v}2v(μ1​−μ2​)2​ — proved against Mathlib's log-likelihood-ratio definition.

The four definition items of this mission package exactly these carriers:

  • Def_fep2_expected_free_energy — the predicted state-outcome joint, preference risk, likelihood ambiguity, epistemic value, pragmatic cost, expected free energy (epistemic sign fixed by definition), the full-support contract, and the marginal/product/conditional-entropy/mutual-information lemmas the decomposition needs. Imports FEP-I.
  • Def_fep2_gaussian_vfe — fixed-variance Gaussian family with its exact KL, scalar OU parameters, the exact scalar Gaussian filter (prediction, observation kernel, gain, closed posterior, evidence law), evidence surprisal, and the posterior-form Gaussian variational free energy. Self-contained.
  • Def_fep2_bayesian_model_reduction — posterior odds, Bayes factor, and the model-odds update odds←odds×Zf/Zrodds \leftarrow odds \times Z_f/Z_rodds←odds×Zf​/Zr​, with totalized division boundaries kept explicit. Imports FEP-I.
  • Def_fep2_native_blanket — the static blanket factorization, the Dirac-mass embedding of finite laws into native measures, blanket/internal/external coordinates, the conditional-pair kernel, and the marginal/composition identifications the independence proof needs. Imports FEP-I.

Formalization targets

Goal: expected free energy decomposes into risk plus ambiguity

For every finite generative model, every policy π\piπ, and every model with full support:

G[π]  =  KL(P(o∣π) ∥ C)  +  ∑sP(s∣π) H(A[⋅∣s]).G[\pi] \;=\; \mathrm{KL}\big(P(o\mid\pi)\,\|\,C\big) \;+\; \sum_s P(s\mid\pi)\,H\big(A[\cdot\mid s]\big).G[π]=KL(P(o∣π)∥C)+s∑​P(s∣π)H(A[⋅∣s]).

The epistemic-value sign is fixed by definition (G[π]=G[\pi] = G[π]= pragmatic cost −-− epistemic value); the decomposition follows from two entropy identities: epistemic value I(s;o∣π)I(s;o\mid\pi)I(s;o∣π) is predicted outcome entropy minus ambiguity, and risk is cross-entropy minus the same entropy (Gibbs' inequality under full reference support). Nonnegativity of GGG follows as a corollary — but the decomposition, not the bound, is the target.

Gaussian variational free energy in closed form

For the exact scalar Gaussian filter, the posterior-form variational free energy at recognition mean μ\muμ is

F[μ]=(μ−m∗)22v∗+S(o),F[\mu] = \frac{(\mu - m^*)^2}{2v^*} + S(o),F[μ]=2v∗(μ−m∗)2​+S(o),

the exact fixed-variance Gaussian KL (the recognition-to-posterior gap) plus the density-relative evidence surprisal. Equality with the surprisal holds exactly at the posterior mean — the Gaussian analogue of FEP-I's exactness theorem.

Odds recursion of Bayesian model reduction

Bayes' rule in odds form: at positive evidence,

P(hf∣e)P(hr∣e)=P(hf)P(hr)⋅P(e∣hf)P(e∣hr),\frac{P(h_f\mid e)}{P(h_r\mid e)} = \frac{P(h_f)}{P(h_r)}\cdot\frac{P(e\mid h_f)}{P(e\mid h_r)},P(hr​∣e)P(hf​∣e)​=P(hr​)P(hf​)​⋅P(e∣hr​)P(e∣hf​)​,

with the reference prior mass and reference likelihood as exact division premises. The multiplicative Bayes-factor structure (topic fep-120: factorized evidence ratios multiply; sequential model-odds updates agree with one update by product evidence) is available from the same definition layer as a further target.

Native Markov blanket conditional independence

The embedded static blanket factorization satisfies Mathlib's native CondIndepFun predicate: internal coordinates are conditionally independent of external coordinates given the blanket coordinate. The result is obtained by identifying the authored finite conditional kernels with Mathlib conditional distributions (the embedding preserves marginals and joints exactly on discrete carriers) — not by a finite mutual-information argument.

Significance

These four results are the load-bearing extensions of FEP-I's bound: expected free energy converts the variational principle into a theory of action selection; Markov blankets make "internal states" and "external states" well-defined relative to a blanket, which is what lets the FEP talk about self-organizing systems at all; the Gaussian filter is the tractable regime in which the variational machinery becomes the Kalman update; and Bayesian model reduction is the learning/comparison step that updates structure, not just parameters.

Formalizing them. All four families are proved with zero proof holes in the source repository, against a pinned Mathlib; the definition layer here is faithful (same carriers, same totalized conventions, same support contracts made explicit) and every item below compiles locally against the platform environment. The mission's value is reusable community infrastructure: the definition items publish the EFE layer, the Gaussian filter, the odds layer, and the native-blanket embedding in the shared namespace FreeEnergyPrinciple, so later missions (policy trees, collective inference, predictive coding) can import them instead of re-deriving. Status honesty: all eight items below are formalized and machine-checked locally against the platform environment; each is an open problem on the platform only in the sense that no proof has yet been submitted to it.

Difficulty

  • The EFE decomposition looks like an algebraic rearrangement but the sign conventions are load-bearing: the epistemic value enters GGG with a minus sign, and the two helper identities (epistemic value = outcome entropy −-− ambiguity; risk = cross-entropy −-− outcome entropy) both hold only under the full-support contract, which the definition makes explicit rather than hiding in a carrier.
  • The Gaussian identity requires the exact native KL between Gaussian laws — the proof goes through Mathlib's log-likelihood-ratio definition and the Gaussian first moment — and the closed-form update's positivity (positive prediction variance, positive innovation variance) is what makes the recognition family genuine rather than degenerate.
  • The odds recursion is a field-simp identity, but the premises are the point: a plausible rendering that hides division by zero behind totalized division changes the statement.
  • The blanket theorem is the most intricate item: it must transport a finite factorization through the Dirac-mass embedding into Mathlib's conditional-distribution machinery, with nonemptiness premises for the conditional distributions to exist. A "proof" via finite mutual information would prove something weaker than the source.

Formalization scope

Committed conventions of this mission's Lean development:

  • The expected-free-energy and model-reduction families reuse the published Free Energy Principle I finite substrate (namespace FreeEnergyPrinciple, definitions Def_fep_finite_laws, Def_fep_finite_information, Def_fep_generative_model); this mission adds definition items Def_fep2_expected_free_energy, Def_fep2_gaussian_vfe, Def_fep2_bayesian_model_reduction, and Def_fep2_native_blanket, all in the same namespace.
  • The Gaussian family is deliberately native: Mathlib gaussianReal/gaussianPDF, no finite substrate, no manifold geometry, no singular (zero-variance) branch.
  • Totalized real division boundaries (zero evidence, zero reference mass) are stated, never silently absorbed.
  • The natural-gradient / dynamic-flow layer of the source's Gaussian module (natural gradient flow, strict descent away from the posterior) is deliberately left out of this mission and is a natural extension target; likewise the row-wise dynamical blanket theorem (every authored factorized transition row preserves the native blanket conditional independence), which follows directly from the static theorem via the source's nextStaticModel construction.
  • Contributions welcome: the epistemic/pragmatic ENNReal balance (catalogue topic fep-021) onto this substrate, the treewise EFE decomposition (fep-133), Bayes-factor multiplicativity (fep-120), and blanket nonvacuity witnesses.

Selected references

  • K. Friston, A free energy principle for the brain, Journal of Physiology (Paris) 100 (2006) 70–87. https://doi.org/10.1016/j.jphysparis.2006.10.001
  • K. Friston, The free-energy principle: a unified brain theory?, Nature Reviews Neuroscience 11 (2010) 127–138. https://doi.org/10.1038/nrn2787
  • K. Friston & W. Penny, Post hoc Bayesian model selection, NeuroImage 56 (2011) 2089–2099. https://doi.org/10.1016/j.neuroimage.2011.03.062
  • K. Friston, T. FitzGerald, F. Rigoli, P. Schwartenbeck, G. Pezzulo, Active inference: a process theory, Neural Computation 29 (2017) 1–49. https://doi.org/10.1162/neco_a_00912
  • T. Parr, G. Pezzulo, K. J. Friston, Active Inference: The Free Energy Principle in Mind, Brain, and Behavior, MIT Press (2022). https://mitpress.mit.edu/9780262045354/active-inference/
  • D. A. Friedman, fep_formal: Towards Lean 4 Formalization of the Free Energy Principle (v1.2.0), Active Inference Institute (2026), the formal source of truth for this mission. https://github.com/ActiveInferenceInstitute/fep_formal
  • D. A. Friedman, Towards Lean 4 Formalization of the Free Energy Principle: AI-Driven Theorem Sketching and Verification for Active Inference and Bayesian Mechanics, Active Inference Journal (2026). https://doi.org/10.5281/zenodo.19699233
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Mathematical Physics·Captain: Lucas

Boltzmann Constant: Kinetic Theory, Boltzmann Factors and EntropyTextbook

Motivation

The Boltzmann constant kBk_BkB​ is the proportionality factor relating the average thermal energy of the particles of a system to its thermodynamic temperature. It appears wherever a microscopic energy has to be compared with a macroscopic temperature: in the ideal gas law written per molecule, in the equipartition theorem, in the Boltzmann factor e−E/kBTe^{-E/k_BT}e−E/kB​T that governs equilibrium occupation probabilities, in Boltzmann's entropy formula S=klog⁡WS = k\log WS=klogW, in the thermal voltage of a ppp–nnn junction, and in the Johnson noise of a resistor.

The constant also has an unusual documentary history. Boltzmann linked entropy and probability in 1877 but never introduced a constant; Max Planck first wrote kkk, and gave the first numerical value (1.346×10−231.346\times10^{-23}1.346×10−23 J/K, about 2.5% below the modern figure), in his 1900–1901 derivation of the black-body law — the terse S=klog⁡WS = k\log WS=klogW on Boltzmann's tombstone is Planck's formulation. For most of the twentieth century kBk_BkB​ was a measured quantity; the 2017 acoustic gas thermometry campaign reached a relative uncertainty of 0.2 ppm, and as part of the 2019 revision of the SI the constant was defined to the exact value 1.380649×10−231.380649\times10^{-23}1.380649×10−23 J·K⁻¹, which is now what fixes the kelvin.

This mission formalizes the elementary quantitative content of that picture: the identities that make kBk_BkB​ a conversion factor, and the exact arithmetic that the 2019 SI definitions make possible.

Setting

Work throughout with real numbers; units are carried in the prose, not in the types. Fix the exact post-2019 SI values

kB=1.380649×10−23 J K−1,NA=6.02214076×1023 mol−1,q=1.602176634×10−19 C,k_B = 1.380649\times10^{-23}\ \mathrm{J\,K^{-1}}, \qquad N_A = 6.02214076\times10^{23}\ \mathrm{mol^{-1}}, \qquad q = 1.602176634\times10^{-19}\ \mathrm{C},kB​=1.380649×10−23 JK−1,NA​=6.02214076×1023 mol−1,q=1.602176634×10−19 C,

and define the molar gas constant as the product R=kBNAR = k_B N_AR=kB​NA​.

A gas sample is described by its pressure ppp, volume VVV, absolute temperature TTT, amount of substance nnn, molecule count N=nNAN = nN_AN=nNA​, particle mass mmm, and mean square particle speed ⟨v2⟩\langle v^2\rangle⟨v2⟩. A system with a finite set sss of microstates is described by an energy function E:s→RE : s \to \mathbb{R}E:s→R; its partition function is Z=∑i∈se−Ei/(kBT)Z = \sum_{i\in s} e^{-E_i/(k_BT)}Z=∑i∈s​e−Ei​/(kB​T) and its Boltzmann probabilities are Pi=e−Ei/(kBT)/ZP_i = e^{-E_i/(k_BT)}/ZPi​=e−Ei​/(kB​T)/Z. For a distribution ppp on sss, the Gibbs entropy is S=−kB∑ipilog⁡piS = -k_B\sum_i p_i\log p_iS=−kB​∑i​pi​logpi​, the Shannon entropy (in nats) is −∑ipilog⁡pi-\sum_i p_i\log p_i−∑i​pi​logpi​, and for WWW equiprobable microstates Boltzmann's entropy is kBlog⁡Wk_B \log WkB​logW. The thermal voltage is VT(T)=kBT/qV_T(T) = k_BT/qVT​(T)=kB​T/q. All logarithms are natural.

Target

The goal theorem is the statement that fixes the physical meaning of kBk_BkB​: kinetic theory plus the per-molecule gas law determine the mean translational kinetic energy. From

pV=13Nm⟨v2⟩andpV=NkBTpV = \tfrac{1}{3}Nm\langle v^2\rangle \qquad\text{and}\qquad pV = Nk_BTpV=31​Nm⟨v2⟩andpV=NkB​T

conclude

12m⟨v2⟩=32kBT,vrms=3kBT/m.\tfrac{1}{2}m\langle v^2\rangle = \tfrac{3}{2}k_BT, \qquad v_{\mathrm{rms}} = \sqrt{3k_BT/m}.21​m⟨v2⟩=23​kB​T,vrms​=3kB​T/m​.

The milestones are the surrounding identities, in the order of the source: the equivalence pV=nRT  ⟺  pV=NkBTpV = nRT \iff pV = Nk_BTpV=nRT⟺pV=NkB​T; equipartition, 12m⟨vx2⟩=12kBT\tfrac{1}{2}m\langle v_x^2\rangle = \tfrac{1}{2}k_BT21​m⟨vx2​⟩=21​kB​T per degree of freedom; the ratio law vrms(m1)/vrms(m2)=m2/m1v_{\mathrm{rms}}(m_1)/v_{\mathrm{rms}}(m_2) = \sqrt{m_2/m_1}vrms​(m1​)/vrms​(m2​)=m2​/m1​​; normalisation of the Boltzmann factors, ∑iPi=1\sum_i P_i = 1∑i​Pi​=1; the reduction of the Gibbs entropy on the uniform distribution to S=kBlog⁡WS = k_B\log WS=kB​logW; the identification S/kB=S/k_B = S/kB​= Shannon entropy; the energy kBTk_BTkB​T of one nat of rescaled entropy; and three numerical facts — VT(300 K)≈25.85V_T(300\ \mathrm{K}) \approx 25.85VT​(300 K)≈25.85 mV, kB≈8.617333262×10−5k_B \approx 8.617333262\times10^{-5}kB​≈8.617333262×10−5 eV/K, and the exact value R=8.31446261815324R = 8.31446261815324R=8.31446261815324 J·K⁻¹·mol⁻¹.

Significance

The results. Individually these are the standard first facts of kinetic theory and statistical mechanics; together they pin down what the constant does. The equipartition chain converts a temperature into a velocity distribution scale and explains the measured room-temperature rms speeds from helium (about 1370 m/s) to xenon (about 240 m/s). The entropy statements make precise the claim that thermodynamic entropy is Shannon entropy in energy units, with kBk_BkB​ as the exchange rate — the statement behind the natural-unit convention kB=1k_B = 1kB​=1. The numerical milestones exercise the consequence of the 2019 SI revision that unit conversions involving kBk_BkB​ are now exact rational arithmetic rather than propagated measurement uncertainty.

Formalizing them. All of these are settled physics; nothing here is open. What the mission produces is a small, reusable Lean development of the SI defining constants and of the elementary statistical-mechanical vocabulary (Boltzmann weights, partition function, Gibbs/Shannon/Boltzmann entropies), with each textbook identity stated against that shared model rather than re-derived ad hoc. It is a suitable entry-level mission and a foundation other physics missions can import.

Difficulty

The mathematics is elementary; the difficulty is entirely one of faithful modelling, and solvers should expect the friction to be there rather than in the proofs. Three specific points. First, Lean's division and logarithm are total: e−E/(kBT)e^{-E/(k_BT)}e−E/(kB​T) is defined at T=0T = 0T=0 and evaluates to 111, and log⁡x=0\log x = 0logx=0 for x≤0x \le 0x≤0, so statements must carry the positivity hypotheses that keep them physically meaningful rather than relying on the definitions to exclude bad inputs. Second, the entropy definitions are stated for an arbitrary real-valued weight function, not for a distribution; normalisation is a hypothesis where it is needed, never an assumption baked into the type. Third, the numerical milestones are claims about specific decimal numerals, and the tolerance in each is part of the statement: two of them are genuine approximations and one, the value of RRR, is an exact identity, which is only true because both factors are exact SI numerals.

Formalization scope

Quantities are real numbers (ℝ); no dimensional-analysis layer is used, and unit correctness is a convention of the prose. Finite state spaces are Finsets over an arbitrary index type, with nonemptiness stated as a hypothesis where the partition function must be nonzero. Entropies use the natural logarithm, so they are measured in nats, and the Shannon entropy is the Gibbs entropy divided by kBk_BkB​ by construction. Temperatures, masses, volumes and particle counts are positive reals where the physics requires it. The mean square speed is a free real variable constrained only by the stated equations; it is not built from a velocity distribution, and extending the development to an actual Maxwell–Boltzmann distribution is out of scope here and a natural follow-up mission.

The statements are deliberately non-vacuous: every hypothesis set in the mission is satisfiable (positive temperature, positive mass, nonempty state space), and the numerical items admit no trivializing reading since they are closed claims about fixed numerals. Only Mathlib is required — Real.exp, Real.log, Real.sqrt, and Finset.sum. The definition file is intended to be reusable: any later mission about thermodynamics, black-body radiation, or the Shockley diode equation can import the SI constants and entropy vocabulary unchanged.

Selected references

  • Wikipedia, Boltzmann constant — the source text this mission formalizes: https://en.wikipedia.org/wiki/Boltzmann_constant
  • D. B. Newell and E. Tiesinga (eds.), The International System of Units (SI), NIST Special Publication 330 (2019). DOI: https://doi.org/10.6028/NIST.SP.330-2019 — the exact defining values of kBk_BkB​, NAN_ANA​ and qqq.
  • M. Planck, "Ueber das Gesetz der Energieverteilung im Normalspectrum", Annalen der Physik 309(3):553–563 (1901). DOI: https://doi.org/10.1002/andp.19013090310 — the first introduction of kkk and of S=klog⁡WS = k\log WS=klogW.
  • R. P. Feynman, R. B. Leighton and M. Sands, The Feynman Lectures on Physics, Vol. I, ch. 39 (kinetic theory of gases): https://www.feynmanlectures.caltech.edu/I_39.html
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Probability·Captain: marwahaha

The exact reconstruction threshold for the three-state symmetric channelOpen Problem

Motivation

Broadcasting a label through noisy tree edges models how information decays with distance. The source studies when observations far from the root retain information about its three-state label. The source is OpenAI's September 2026 manuscript.

Setting

The symmetric channel preserves the input with probability (1+2λ)/3(1+2\lambda)/3(1+2λ)/3 and sends it to each other state with probability (1−λ)/3(1-\lambda)/3(1−λ)/3. Reconstruction advantage is the expected total variation between the posterior root law and the uniform prior.

Formalization targets

b≥2,−1/2≤λ≤1,bλ2>1⟹Advantage⁡n→L>0.b\ge2,\quad-1/2\le\lambda\le1,\quad b\lambda^2>1\quad\Longrightarrow\quad\operatorname{Advantage}_n\to L>0.b≥2,−1/2≤λ≤1,bλ2>1⟹Advantagen​→L>0.

For every natural number b ≥ 2 and every real λ that is admissible, meaning −1/2 ≤ λ ≤ 1, if b·λ² > 1 then the sequence of regular-tree advantages reconstructs. Here a three-state spin (an element of Fin 3) is passed through a symmetric channel that keeps the spin with probability (1+2λ)/3 and moves to each other spin with probability (1−λ)/3. The observation at depth 0 is the root spin, and the observation at depth n+1 is a multiset of depth-n observations, one for each of the offspring of the root, where the offspring count is the constant b (the regular case) and each child spin is obtained by passing the parent spin through the channel and then observed recursively. With a uniformly random root spin, the posterior of each spin given an observation is its conditional probability, defaulting to 1/3 when the observation has probability zero. The advantage of a family of laws indexed by the root spin is the sum over observations y of the marginal probability of y times half the sum over spins i of |posterior(y,i) − 1/3|. The regular advantage at depth n is this advantage for the regular b-ary observation law. Reconstructs means that this sequence in n converges to some limit L > 0. The statement is an admitted theorem, with its proof left as sorry.

The goal is OAI.ThreeState.regular_supercritical. Supporting targets are listed below; they retain their individual hypotheses and are separate statements.

  • poisson supercritical.
  • poisson reconstructs above KS.
  • regular reconstructs above KS.

Significance

The selected goal is the regular-tree supercritical direction. Supporting published targets give Poisson reconstruction and equivalent supercritical formulations in a second definition group. The manuscript presents a mathematical argument; the attached goal currently has status Open, so the requested contribution is a Lean proof of the displayed formal target.

Difficulty

The observation contains the full nested collection of descendants, and the posterior depends on correlated information inherited from their common ancestor. A single root-to-leaf correlation is insufficient to describe reconstruction.

Formalization scope

Observations are nested multisets with a uniform three-state root. The attached targets establish reconstruction above the displayed threshold; non-reconstruction at or below equality and stochastic-block-model recovery are outside this draft’s formal scope.

The shared definitions are supplied by ThreeStateSupercritical, ThreeStateTreeClauses. The target uses Lean 4.33.1 with the pinned Mathlib environment. Contributions should preserve the existing statement and develop reusable supporting lemmas in its definitions.

Selected references

  • OpenAI, The exact reconstruction threshold for the three-state symmetric channel, preprint, September 2026. Manuscript.
  • OpenAI, accompanying Lean statement. Pinned source.
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Quantum Information·Captain: wurtle

Classical capacity and entropy inequalities for generalized amplitude dampingResearch Paper

Motivation: the classical capacity of a thermal qubit channel

A quantum channel models how a physical system, used to carry information, is corrupted by its environment. The classical capacity of a channel is the largest rate, in bits per use, at which classical messages can be sent with vanishing error when the sender may encode into arbitrary — possibly entangled — states of many uses and the receiver may measure all outputs jointly. The Holevo–Schumacher–Westmoreland coding theorem (Holevo 1998; Schumacher–Westmoreland 1997) expresses this capacity as a regularized limit of the Holevo information over ever larger blocks of uses. Since Holevo information is not additive in general (Hastings 2009), computing the capacity of any specific channel requires a channel-specific additivity argument, and exact formulas are known only for a few families.

Generalized amplitude damping is the standard model of a qubit relaxing toward a thermal state: it loses or gains an excitation with probabilities set by a damping strength γ\gammaγ and a stationary excited population ν\nuν, and its coherences decay. It is one of the basic noise models of quantum information theory.

Background timeline

  • 1996–1998 — Coding theorems for pure and mixed signals establish the regularized capacity formula (Hausladen et al. 1996; Schumacher–Westmoreland 1997; Holevo 1998).
  • 2002 — Additivity for unital qubit channels (King 2002) and for entanglement-breaking channels (Shor 2002) settles some parameter regions of the family; Bennett, Shor, Smolin and Thapliyal describe the two-signal optimization for ordinary amplitude damping (BSST 2002).
  • 2005 — Giovannetti and Fazio derive the optimized one-use expression for ordinary amplitude damping (Giovannetti–Fazio 2005); Berry studies qubit channels achieving capacity with two states (Berry 2005).
  • 2007 — Hou and Fang characterize the one-use Holevo optimum of the generalized channel (Hou–Fang 2007).
  • 2009 — Hastings shows that Holevo information is not additive in general (Hastings 2009).
  • 2018 — Leditzky, Kaur, Datta and Wilde note that the unrestricted classical capacity of amplitude damping had not been determined (LKDW 2018).
  • 2020 — Khatri, Sharma and Wilde collect upper bounds for the generalized family (KSW 2020).
  • 2026 — Tang, Zhu, Bai and Wang prove additivity for qubit channels with a pure output, including ordinary amplitude damping (arXiv:2609.28592); Fang gives a close converse bound for the generalized family (arXiv:2609.14621).
  • 2026 — An OpenAI preprint, Classical capacity and entropy inequalities for generalized amplitude damping (OpenAI Math Release, September 24, 2026), claims the capacity for all (γ,ν)∈[0,1]2(\gamma,\nu)\in[0,1]^2(γ,ν)∈[0,1]2. The preprint has not been peer reviewed, and its results are not formally verified.

Setting

For γ,ν∈[0,1]\gamma,\nu\in[0,1]γ,ν∈[0,1] the generalized amplitude-damping channel acts on a qubit density matrix by

Aγ,ν(1−qzzˉq)=(1−t1−γ z1−γ zˉt),t=(1−γ)q+γν,\mathcal A_{\gamma,\nu}\begin{pmatrix}1-q&z\\\bar z&q\end{pmatrix}=\begin{pmatrix}1-t&\sqrt{1-\gamma}\,z\\\sqrt{1-\gamma}\,\bar z&t\end{pmatrix},\qquad t=(1-\gamma)q+\gamma\nu,Aγ,ν​(1−qzˉ​zq​)=(1−t1−γ​zˉ​1−γ​zt​),t=(1−γ)q+γν,

and nnn independent uses act as Aγ,ν⊗n\mathcal A_{\gamma,\nu}^{\otimes n}Aγ,ν⊗n​ on 2n×2n2^n\times2^n2n×2n matrices. With S(P)=−Tr⁡Pln⁡PS(P)=-\operatorname{Tr}P\ln PS(P)=−TrPlnP, the Holevo information in bits is

χ(N)=1ln⁡2sup⁡{qa,ρa}{S(∑aqaN(ρa))−∑aqaS(N(ρa))},\chi(\mathcal N)=\frac1{\ln2}\sup_{\{q_a,\rho_a\}}\Bigl\{S\Bigl(\sum_aq_a\mathcal N(\rho_a)\Bigr)-\sum_aq_aS(\mathcal N(\rho_a))\Bigr\},χ(N)=ln21​{qa​,ρa​}sup​{S(a∑​qa​N(ρa​))−a∑​qa​S(N(ρa​))},

over all finite ensembles of input states (entangled across uses when N=A⊗n\mathcal N=\mathcal A^{\otimes n}N=A⊗n). The classical capacity C(N)C(\mathcal N)C(N) is the supremum of rates RRR for which there are nnn-use codes — arbitrary input states for each of MnM_nMn​ equiprobable messages and one joint measurement of all outputs — with average error tending to zero and lim inf⁡nn−1log⁡2Mn≥R\liminf_n n^{-1}\log_2M_n\ge Rliminfn​n−1log2​Mn​≥R; there is no shared entanglement or feedback. Write hhh for binary entropy in nats, g(u)=h((1+1−4u)/2)g(u)=h\bigl((1+\sqrt{1-4u})/2\bigr)g(u)=h((1+1−4u​)/2) and vγ,ν(p)=γν(1−ν)+γ(1−γ)(p−ν)2v_{\gamma,\nu}(p)=\gamma\nu(1-\nu)+\gamma(1-\gamma)(p-\nu)^2vγ,ν​(p)=γν(1−ν)+γ(1−γ)(p−ν)2.

Formalization targets

Goal: additivity and capacity formula (Theorem 1.1)

For all γ,ν∈[0,1]\gamma,\nu\in[0,1]γ,ν∈[0,1] and every n≥1n\ge1n≥1,

χ(Aγ,ν⊗n)=n χ(Aγ,ν)=nln⁡2max⁡0≤p≤1{h((1−γ)p+γν)−g(vγ,ν(p))},\chi(\mathcal A_{\gamma,\nu}^{\otimes n})=n\,\chi(\mathcal A_{\gamma,\nu})=\frac n{\ln 2}\max_{0\le p\le1}\bigl\{h((1-\gamma)p+\gamma\nu)-g(v_{\gamma,\nu}(p))\bigr\},χ(Aγ,ν⊗n​)=nχ(Aγ,ν​)=ln2n​0≤p≤1max​{h((1−γ)p+γν)−g(vγ,ν​(p))},

the maximum is attained, C(Aγ,ν)=χ(Aγ,ν)C(\mathcal A_{\gamma,\nu})=\chi(\mathcal A_{\gamma,\nu})C(Aγ,ν​)=χ(Aγ,ν​), and for every maximizer ppp the equiprobable independent products of the two signals ϕ±=1−p ∣0⟩±p ∣1⟩\phi_\pm=\sqrt{1-p}\,|0\rangle\pm\sqrt p\,|1\rangleϕ±​=1−p​∣0⟩±p​∣1⟩ attain χ(Aγ,ν⊗n)\chi(\mathcal A_{\gamma,\nu}^{\otimes n})χ(Aγ,ν⊗n​) at every block length. The goal is published on the platform with status Open.

Significance

The result itself. The theorem gives a closed one-variable formula for the classical capacity of every generalized amplitude-damping channel, removing the regularization over block lengths: entangled input signals across uses give no advantage, and a simple product code with two signals per use is optimal. This settles the ordinary amplitude-damping case listed as open by LKDW 2018 and extends beyond the pure-output criterion of Tang et al. to the thermal regime, where the channel has no pure output. The source further proves additivity of Holevo capacity, minimum output entropy and classical capacity when the channel is used in parallel with any finite-dimensional partner channel (Corollary 1.2); that corollary is not part of this goal.

Formalizing it. The goal ties together an operational capacity (codes and error probabilities), an entropic quantity (a supremum over unrestricted ensembles on 2n2^n2n-dimensional matrices), and a scalar optimization. A machine-checked proof would certify both the matrix entropy inequality at the heart of the argument and the converse direction of the coding theorem. Mathlib does not currently contain quantum channel capacity theory, so the definitions here are new infrastructure.

Difficulty

Optimizing a single use gives a lower bound on capacity; the difficulty is the matching upper bound for all nnn simultaneously, where an input may be entangled across all uses. Holevo additivity is false for general channels, so no abstract argument applies, and for interior thermal occupation 0<ν<10<\nu<10<ν<1 with γ>0\gamma>0γ>0 the channel has no pure output, which rules out the recent pure-output criterion. The proof needs a lower bound on the entropy of the output of an arbitrary entangled block input, i.e. a matrix entropy inequality for 2×22\times22×2 block-structured states that is tight on product inputs. Identifying the capacity with the regularized Holevo quantity also requires the full coding theorem and a Fano-type converse.

Formalization scope

  • Matrices are indexed by Fin n → Fin 2; the nnn-use channel is given by tensor products of the four standard Kraus operators of generalized amplitude damping, which reproduce the displayed action exactly.
  • Entropy is Tr (cfc negMulLog P) (nats, 0ln⁡0=00\ln0=00ln0=0); Holevo values are divided by ln⁡2\ln 2ln2 (bits). holevo γ ν n is the sSup over all finite ensembles of arbitrary 2n2^n2n-dimensional states, with no product or purity restriction.
  • capacity is the sSup of operationally achievable rates: codes with any positive number of messages, arbitrary state encodings, an arbitrary POVM decoder, average error tending to 000, and the liminf rate condition. It is defined operationally, not by regularization, so the identity C=χC=\chiC=χ includes the coding theorem.
  • The scalar objective uses Real.binEntropy (nats); the maximizer is over p∈[0,1]p\in[0,1]p∈[0,1]. The final clause also asserts that the phase-product signals are states.
  • Parameters range over the closed square [0,1]2[0,1]^2[0,1]2, including boundary cases (identity channel at γ=0\gamma=0γ=0, full replacement at γ=1\gamma=1γ=1).
  • Needed infrastructure: matrix entropy and its concavity, CPTP maps and Kraus representations, Holevo's bound, Fano's inequality, the HSW coding theorem for finite ensembles, and Fekete-type superadditivity. These are reusable for any quantum Shannon-theory mission.

Selected references

  • P. Hausladen, R. Jozsa, B. Schumacher, M. Westmoreland, W. K. Wootters, Classical information capacity of a quantum channel, Phys. Rev. A 54 (1996), 1869–1876. https://doi.org/10.1103/PhysRevA.54.1869
  • B. Schumacher and M. D. Westmoreland, Sending classical information via noisy quantum channels, Phys. Rev. A 56 (1997), 131–138. https://doi.org/10.1103/PhysRevA.56.131
  • A. S. Holevo, The capacity of the quantum channel with general signal states, IEEE Trans. Inf. Theory 44 (1998), 269–273. https://doi.org/10.1109/18.651037
  • C. King, Additivity for unital qubit channels, J. Math. Phys. 43 (2002), 4641–4653. https://doi.org/10.1063/1.1500791
  • P. W. Shor, Additivity of the classical capacity of entanglement-breaking quantum channels, J. Math. Phys. 43 (2002), 4334–4340. https://doi.org/10.1063/1.1498000
  • C. H. Bennett, P. W. Shor, J. A. Smolin, A. V. Thapliyal, Entanglement-assisted capacity of a quantum channel and the reverse Shannon theorem, IEEE Trans. Inf. Theory 48 (2002), 2637–2655. https://doi.org/10.1109/TIT.2002.802612
  • V. Giovannetti and R. Fazio, Information-capacity description of spin-chain correlations, Phys. Rev. A 71 (2005), 032314. https://doi.org/10.1103/PhysRevA.71.032314
  • D. W. Berry, Qubit channels that achieve capacity with two states, Phys. Rev. A 71 (2005), 032334. https://doi.org/10.1103/PhysRevA.71.032334
  • L.-Z. Hou and M.-F. Fang, The Holevo capacity of a generalized amplitude-damping channel, Chinese Physics 16 (2007), 1843–1847. https://doi.org/10.1088/1009-1963/16/7/006
  • M. B. Hastings, Superadditivity of communication capacity using entangled inputs, Nature Physics 5 (2009), 255–257. https://doi.org/10.1038/nphys1224
  • F. Leditzky, E. Kaur, N. Datta, M. M. Wilde, Approaches for approximate additivity of the Holevo information of quantum channels, Phys. Rev. A 97 (2018), 012332. https://doi.org/10.1103/PhysRevA.97.012332
  • S. Khatri, K. Sharma, M. M. Wilde, Information-theoretic aspects of the generalized amplitude-damping channel, Phys. Rev. A 102 (2020), 012401. https://doi.org/10.1103/PhysRevA.102.012401
  • Z. Tang, C. Zhu, G. Bai, X. Wang, Classical capacity and entanglement cost of the amplitude damping channel, arXiv:2609.28592 (2026). https://arxiv.org/abs/2609.28592v1
  • K. Fang, A pretty-tight converse on the classical capacity of generalized amplitude-damping channels, arXiv:2609.14621 (2026). https://arxiv.org/abs/2609.14621v1
  • OpenAI, Classical capacity and entropy inequalities for generalized amplitude damping, OpenAI Math Release preprint, September 24, 2026 (Theorem 1.1, p. 3). https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Classical-capacity-and-entropy-inequalities-for-generalized-amplitude-damping-September-24-2026/paper.pdf
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