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EconomicsOperations ResearchOptimization·Captain: mikedeng1

Platform Tokenization: Financing, Governance, and Moral Hazard: For Small Capacity Cost the Blockchain-Based Business Model Strictly Dominates the Traditional OneResearch Paper

Motivation

Digital platforms (marketplaces, payment networks, sharing services) need large up-front investments in capacity before any revenue arrives, and their founders typically finance them by selling equity to venture capitalists. Since 2017 an alternative has been available: issuing a platform-specific cryptocurrency (a utility token) in an initial coin offering (ICO), and running the platform on a blockchain whose fee rules are fixed in a smart contract. Whether this is merely a new funding channel or a better business model is a question for operations management, corporate finance and platform economics alike.

J. Chod, N. Trichakis and S. A. Yang (Platform Tokenization: Financing, Governance, and Moral Hazard, Management Science, 2022) answer it in a model in which the entrepreneur's effort is not contractible. They show that the answer depends on the cost of building capacity: when capacity is expensive, equity wins (their Proposition 1), and when it is cheap, tokens win (their Proposition 2). This mission formalizes the second result.

Setting

An entrepreneur builds a platform of capacity QQQ at cost C(Q)=KQkC(Q)=KQ^kC(Q)=KQk and exerts effort eee at private cost γe\gamma eγe. Buyers' inverse demand is d(e,q)=eaq−bd(e,q)=e^aq^{-b}d(e,q)=eaq−b and sellers' supply curve is s(q)=mqns(q)=mq^ns(q)=mqn, with 0<a<b<10<a<b<10<a<b<1, m,n≥0m,n\ge0m,n≥0 and k>(1−b)/(1−a)k>(1-b)/(1-a)k>(1−b)/(1−a). Sellers pay a one-time cost ccc to join, cash flows are discounted by δ∈(0,1)\delta\in(0,1)δ∈(0,1), and each token is used v≥1v\ge1v≥1 times per period. The per-period surplus is

F(e,q)=q(d(e,q)−s(q)),\mathcal F(e,q)=q\bigl(d(e,q)-s(q)\bigr),F(e,q)=q(d(e,q)−s(q)),

with partial derivatives Fe\mathcal F_eFe​, ded_ede​ in eee. The entrepreneur's objective in both models is the net present value

F(e,Q)1−δ−cQ−C(Q)−γe.\frac{\mathcal F(e,Q)}{1-\delta}-cQ-C(Q)-\gamma e .1−δF(e,Q)​−cQ−C(Q)−γe.

In the traditional model the entrepreneur sells an equity share α\alphaα to a venture capitalist and can raise the fee once sellers have sunk their joining cost (holdup), which forces a first-period subsidy. Its equilibrium payoff \Pi^\$$ is the maximum of the objective subject to (1-\alpha)\mathcal F_e/(1-\delta)=\gamma,where, where ,where\alphaistheVC′sbreak−evenshare,(17)–(20).Inthe∗∗blockchain−basedmodel∗∗shesellsafractionis the VC's break-even share, (17)–(20). In the **blockchain-based model** she sells a fractionistheVC′sbreak−evenshare,(17)–(20).Inthe∗∗blockchain−basedmodel∗∗shesellsafraction\alphaofthetokensandcommitstothefee;thepayoffof the tokens and commits to the fee; the payoffofthetokensandcommitstothefee;thepayoff\Pi^Bisthemaximumsubjecttois the maximum subject toisthemaximumsubjectto\mathcal F_e/(1-\delta)-\alpha\frac1v d_eQ=\gammaandandand\alpha,d(e,Q)Q=vC(Q)withwithwith\alpha\le1,(33)–(36).Corollary1rewritesbothasoneprogramwitheffortfactors, (33)–(36). Corollary 1 rewrites both as one program with effort factors ,(33)–(36).Corollary1rewritesbothasoneprogramwitheffortfactors\beta^$,, ,\beta^B,theblockchainonecarryingtheextracap, the blockchain one carrying the extra cap ,theblockchainonecarryingtheextracapd(e,Q)Q\ge vC(Q)$.

Formalization targets

Goal: Proposition 2

With all other parameters fixed and c>0c>0c>0 or m>0m>0m>0, there is ε>0\varepsilon>0ε>0 such that for every K∈(0,ε]K\in(0,\varepsilon]K∈(0,ε] both suprema are finite and ΠB>Π$unlessΠB=Π$=0.\Pi^B>\Pi^\$\qquad\text{unless}\qquad\Pi^B=\Pi^\$=0 .ΠB>Π$unlessΠB=Π$=0. No value of ε\varepsilonε is fixed: the goal asserts only the existence of a cheap-capacity regime.

Milestones

  1. Corollary 1 for i=Bi=Bi=B and $i=$$: Lemmas 2–3's programs equal (37)–(40).
  2. (B.19)–(B.20): for small KKK the token cap (39) does not bind.
  3. Claim (i): h(e,Q)>g(e,Q)h(e,Q)>g(e,Q)h(e,Q)>g(e,Q), i.e. \beta^B>\beta^\$$ wherever d>s$.
  4. (B.29): e^\(Q)<e^B(Q)<e^*(Q)$, in root form.
  5. Claim (ii): the objective is strictly concave in eee with unique maximizer e∗(Q)e^*(Q)e∗(Q).

Significance

Proposition 2 is the paper's headline. It isolates two advantages of tokenization that hold even without any cost or technology difference: token investors are exposed to platform revenue rather than profit, which is less sensitive to effort, so the entrepreneur internalizes more of the marginal value of her effort; and a fee committed on a blockchain removes the holdup problem and with it the subsidy the traditional platform must finance. Together with Proposition 1 it delineates when a platform should tokenize.

The result is proved in the paper (Appendix B, pp. 19–20). It has not been machine-checked. The proof is short but leaves two steps informal: the relaxation of the cap (39) "by continuity", and the existence of optimal solutions behind the printed "max". A formal proof settles both, and fixes the exact hypotheses under which the claim holds (see the scope section).

Difficulty

The algebra of Corollary 1 and of Claim (i) is routine. The difficulty is analytic. The naive argument compares the two programs pointwise in QQQ at their largest effort roots, but the payoffs are suprema over non-compact feasible sets, and the comparison only transfers to the suprema if the traditional supremum is attained, or approached at capacities bounded away from 000 and ∞\infty∞. The relaxation of (39) requires a bound, uniform in small KKK, showing that points violating the cap cannot approach the relaxed supremum; this is where c>0c>0c>0 or m>0m>0m>0 enters, since with c=m=0c=m=0c=m=0 the objective near such points is not controlled as K→0K\to0K→0.

Formalization scope

Parameters are a structure Params with real fields a,b,m,n,K,k,c,γ,δ,va,b,m,n,K,k,c,\gamma,\delta,va,b,m,n,K,k,c,γ,δ,v; Params.Standing collects the printed assumptions (0<a<b<10<a<b<10<a<b<1, m,n≥0m,n\ge0m,n≥0, k>(1−b)/(1−a)k>(1-b)/(1-a)k>(1−b)/(1−a), v≥1v\ge1v≥1) and four the paper uses without stating (0<δ<10<\delta<10<δ<1, c≥0c\ge0c≥0, γ>0\gamma>0γ>0, K≥0K\ge0K≥0). Powers are Real.rpow, with Lean's 0y=00^y=00y=0 for y≠0y\ne0y=0; the partials Fe=aea−1Q1−b\mathcal F_e=ae^{a-1}Q^{1-b}Fe​=aea−1Q1−b, de=aea−1Q−bd_e=ae^{a-1}Q^{-b}de​=aea−1Q−b are closed forms, certified by two HasDerivAt helper theorems, and e∗(Q)e^*(Q)e∗(Q) is a closed form certified as the argmax by Claim (ii).

\Pi^\$$ and \Pi^Bare∗defined∗bytheprogramsofLemmas2and3;theunderlyingdynamicgameisnotmodelled.Eachpayoffisare *defined* by the programs of Lemmas 2 and 3; the underlying dynamic game is not modelled. Each payoff isare∗defined∗bytheprogramsofLemmas2and3;theunderlyingdynamicgameisnotmodelled.Eachpayoffis\max{0,\sup(\text{objective over the feasible set})}:thesupremumreplacestheprintedmax,nevershownattained,and: the supremum replaces the printed max, never shown attained, and :thesupremumreplacestheprintedmax,nevershownattained,and0$ is the outside option of not starting the venture, invoked in the last paragraph of the paper's proof.

Departures from the printed statement, all disclosed in the items:

  • K∈(0,ε]K\in(0,\varepsilon]K∈(0,ε] instead of [0,ε][0,\varepsilon][0,ε]: at K=0K=0K=0 the Corollary 1 payoff programs coincide on the branch c≤d−sc\le d-sc≤d−s (e.g. c=0c=0c=0, m=1m=1m=1), contradicting the printed strict claim. Lemma 2's literal 0<α0<\alpha0<α constraint omits that zero-investment boundary, so this mission states the common positive-KKK regime.
  • The added hypothesis c>0c>0c>0 or m>0m>0m>0: with c=m=0c=m=0c=m=0, \beta^\=\beta^Bandtheblockchainprogramisthetraditionaloneplusacap,soand the blockchain program is the traditional one plus a cap, soandtheblockchainprogramisthetraditionaloneplusacap,so\Pi^B\le\Pi^$foreveryfor everyforeveryK>0$.
  • Corollary 1 for i=\$$ is posed for K>0andasanequalityofpayoffs:atand as an equality of payoffs: atandasanequalityofpayoffs:atK=0,(19)gives, (19) gives ,(19)gives\alpha=0$, which (20) excludes.

The goal cannot be met vacuously: it asserts that both objective images are bounded above, so the suprema are not Lean's junk value 000, and the helper piTrad_pos_example states \Pi^\>0attheFigure1parameters( at the Figure 1 parameters (attheFigure1parameters(k=1,, ,K=0.01$), ruling out an empty traditional program.

A complete development needs real-power calculus, the intermediate value theorem, strict concavity of e↦eae\mapsto e^ae↦ea, and a compactness or coercivity argument for the suprema. The coercivity bounds for programs of the form "maximize a concave revenue minus a power cost subject to a first-order condition" are reusable for other effort-and-capacity models. Proofs of any milestone are welcome, as are proofs of the helpers.

Selected references

  • J. Chod, N. Trichakis, S. A. Yang, Platform Tokenization: Financing, Governance, and Moral Hazard, Management Science, Articles in Advance, 2022. https://doi.org/10.1287/mnsc.2021.4225
  • M. C. Jensen, W. H. Meckling, Theory of the Firm: Managerial Behavior, Agency Costs and Ownership Structure, Journal of Financial Economics 3(4), 1976. https://doi.org/10.1016/0304-405X(76)90026-X
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Algorithmic Game TheoryEconomicsOperations Research·Captain: mikedeng1

Managing Congestion in Matching Markets: The Unique Mean-Field Equilibrium Has Acceptance Probability min(p̂, p̄) and Explicit Welfare for Both SidesResearch Paper

Why congestion in matching markets matters

Online matching platforms (labor platforms such as Upwork or TaskRabbit, dating sites, short-term rental platforms) make it cheap to contact potential partners, but not cheap to find one who is still available. A worker who has already accepted a job, or a listing that is already booked, keeps receiving applications and keeps being screened. Arnosti, Johari and Kanoria, Managing Congestion in Matching Markets (M&SOM 23(3):620–636, 2021), build a stochastic game-theoretic model of this effect, in which applicants pay to apply and employers pay to screen, and employers cannot see which applicants have already matched. They prove that the model has a unique equilibrium, compute both sides' welfare in it in closed form, and use the formulas to evaluate platform interventions (application limits, application fees, a market-wide wage).

This mission formalizes the equilibrium characterization: the closed-form equilibrium welfare of Theorem 2, together with the existence and uniqueness results (Proposition 2, Theorem 1) and the identities from the paper's endnotes that connect them.

The stationary mean-field model

A market has four parameters: r>0r>0r>0, the number of applicants per employer; β∈(0,1]\beta\in(0,1]β∈(0,1], the probability that an applicant is qualified for a given employer; cac_aca​, the cost of one application; and csc_scs​, the cost of screening one applicant. Throughout, Assumption 1 holds: max⁡(ca,cs)<β\max(c_a,c_s)<\betamax(ca​,cs​)<β. Write cs′=cs/βc'_s = c_s/\betacs′​=cs​/β.

Applicants choose an application intensity m≥0m\ge0m≥0: an applicant sends a Poisson(mmm) number of applications, each of which becomes an offer independently with probability ppp, the acceptance probability. The applicant takes the first offer, so the expected payoff is

Wa(m,p)=1−e−mp−cam,(2)W_a(m,p) = 1-e^{-mp}-c_a m, \tag{2}Wa​(m,p)=1−e−mp−ca​m,(2)

maximized by the applicant best response

M(p)=0  if p≤ca,M(p)=1plog⁡(pca)  if p>ca.(3)\mathcal M(p) = 0 \ \text{ if } p\le c_a, \qquad \mathcal M(p)=\tfrac1p\log\bigl(\tfrac p{c_a}\bigr)\ \text{ if } p>c_a. \tag{3}M(p)=0  if p≤ca​,M(p)=p1​log(ca​p​)  if p>ca​.(3)

Employers receive a Poisson(rmrmrm) number of applications. Each applicant is qualified with probability β\betaβ and still available with probability qqq. An employer either screens sequentially until it hires (screening probability α\alphaα) or exits. The employer best-response correspondence is

A(q)={0} if q<cs′,[0,1] if q=cs′,{1} if q>cs′,(4)\mathcal A(q) = \{0\}\ \text{if } q<c'_s,\qquad [0,1]\ \text{if } q=c'_s,\qquad \{1\}\ \text{if } q>c'_s, \tag{4}A(q)={0} if q<cs′​,[0,1] if q=cs′​,{1} if q>cs′​,(4)

and the employer payoff is We(α,m,q)=α(1−e−rmβq)(1−cs′/q)W_e(\alpha,m,q) = \alpha(1-e^{-rm\beta q})(1-c'_s/q)We​(α,m,q)=α(1−e−rmβq)(1−cs′​/q) (5).

With E(x)=(1−e−x)/xE(x) = (1-e^{-x})/xE(x)=(1−e−x)/x (E(0)=1E(0)=1E(0)=1), the consistency conditions are

q=E(mp),p=αβ E(rmβq).(6–7)q = E(mp), \qquad p = \alpha\beta\,E(rm\beta q). \tag{6–7}q=E(mp),p=αβE(rmβq).(6–7)

A solution (p,q)(p,q)(p,q) is a mean-field steady state of the strategies (m,α)(m,\alpha)(m,α). A mean-field equilibrium (MFE) is a pair (m∗,α∗)(m^*,\alpha^*)(m∗,α∗) with a steady state (p∗,q∗)(p^*,q^*)(p∗,q∗) such that m∗=M(p∗)m^* = \mathcal M(p^*)m∗=M(p∗) and α∗∈A(q∗)\alpha^*\in\mathcal A(q^*)α∗∈A(q∗) (Definition 1). Equilibrium welfare is Πa∗=Wa(m∗,p∗)\Pi^*_a = W_a(m^*,p^*)Πa∗​=Wa​(m∗,p∗) and Πe∗=We(α∗,m∗,q∗)\Pi^*_e = W_e(\alpha^*,m^*,q^*)Πe∗​=We​(α∗,m∗,q∗).

Formalization targets

Goal: Theorem 2 (p. 628)

There are unique p^,pˉ>ca\hat p,\bar p>c_ap^​,pˉ​>ca​ with

r(1−cap^)=1−e−rβp^(1−cap^),1−capˉ+csβlog⁡(capˉ)=0,(13–14)r\Bigl(1-\frac{c_a}{\hat p}\Bigr) = 1-e^{-\frac{r\beta}{\hat p}\left(1-\frac{c_a}{\hat p}\right)}, \qquad 1-\frac{c_a}{\bar p}+\frac{c_s}{\beta}\log\Bigl(\frac{c_a}{\bar p}\Bigr)=0, \tag{13–14}r(1−p^​ca​​)=1−e−p^​rβ​(1−p^​ca​​),1−pˉ​ca​​+βcs​​log(pˉ​ca​​)=0,(13–14)

the MFE is unique, and in it

p∗=min⁡(p^,pˉ),Πa∗=1−cap∗+cap∗log⁡cap∗,Πe∗=r(1−cap∗+csβlog⁡cap∗).(15–16)p^*=\min(\hat p,\bar p),\qquad \Pi^*_a = 1-\frac{c_a}{p^*}+\frac{c_a}{p^*}\log\frac{c_a}{p^*},\qquad \Pi^*_e = r\Bigl(1-\frac{c_a}{p^*}+\frac{c_s}{\beta}\log\frac{c_a}{p^*}\Bigr). \tag{15–16}p∗=min(p^​,pˉ​),Πa∗​=1−p∗ca​​+p∗ca​​logp∗ca​​,Πe∗​=r(1−p∗ca​​+βcs​​logp∗ca​​).(15–16)

The theorem is exact; it has no constants to improve.

Milestones

  1. Proposition 2 (p. 626): for fixed m≥0m\ge0m≥0, α∈[0,1]\alpha\in[0,1]α∈[0,1], rrr, β\betaβ, the system (6)–(7) has a unique solution.
  2. Theorem 2, (13) and Theorem 2, (14) (p. 628): the two root equations each have a unique root above cac_aca​.
  3. Endnote 13 (p. 635): at the applicant best response, consistency (7) with every employer screening (α=1\alpha=1α=1) is equation (13).
  4. §5.1 (p. 628): at the applicant best response, employers are exactly indifferent (q=cs′q=c'_sq=cs′​) iff (14) holds.
  5. Theorem 1 (p. 627): the MFE exists and is unique.
  6. Endnote 12 (p. 635): the welfare identities (15) and (16) at the best response and a steady state.

Significance

Theorem 2 reduces equilibrium welfare on both sides to one scalar, p∗=min⁡(p^,pˉ)p^*=\min(\hat p,\bar p)p∗=min(p^​,pˉ​), and splits markets into two regimes (Definition 2): application-limited (pˉ>p^\bar p>\hat ppˉ​>p^​; all employers screen; applicants compete in a "tragedy of the commons") and screening-limited (pˉ<p^\bar p<\hat ppˉ​<p^​; employers are indifferent and their welfare is zero, by (14) and (16)). All of the paper's later results, including the welfare bounds of Theorem 3, the effect of application limits (Theorems 4–5), application costs (Theorem 6) and wages (Theorem 7), are computed from these formulas.

Proposition 2, Theorem 1 and Theorem 2 are stated in the article but their proofs are in a technical report (Arnosti, Johari, Kanoria 2019, SSRN), not reproduced in the article and not used here. To our knowledge none of these results has a machine-checked proof. A formal development would give a self-contained, checked proof of the equilibrium characterization from the article's definitions alone.

Where the difficulty lies

The welfare identities (15)–(16) are algebra once m∗=M(p∗)m^*=\mathcal M(p^*)m∗=M(p∗) and p∗>cap^*>c_ap∗>ca​ are known. The root statements are one-variable analysis. The hard part is the equilibrium itself. Proposition 2 is a fixed-point problem: substituting (7) into (6) gives an increasing map q↦E(mαβE(rmβq))q\mapsto E(m\alpha\beta E(rm\beta q))q↦E(mαβE(rmβq)), and an increasing map can have several fixed points, so a monotonicity argument alone does not give uniqueness. Theorem 1 then has to handle the correspondence A\mathcal AA: an equilibrium may sit at the kink q∗=cs′q^*=c'_sq∗=cs′​ with an interior α∗\alpha^*α∗, and the case analysis has to show that exactly one of the regimes α∗=1\alpha^*=1α∗=1, α∗<1\alpha^*<1α∗<1 applies and that it pins down (m∗,α∗)(m^*,\alpha^*)(m∗,α∗).

Formalization scope

All objects live in the namespace MatchCongestion.Welfare, over ℝ. The conventions are:

  • Positivity. Params.Standing is Assumption 1 together with 0<r0<r0<r, 0<β≤10<\beta\le10<β≤1, 0<ca0<c_a0<ca​, 0<cs0<c_s0<cs​, which the paper uses without listing them ("costs", β\betaβ a probability). Without cs>0c_s>0cs​>0, (14) has no root above cac_aca​.
  • The ratio at zero. The page leaves (6)–(7) undefined at mp=0mp=0mp=0 and rmβq=0rm\beta q=0rmβq=0. They are written through EEE with E(0)=1E(0)=1E(0)=1, the continuous extension.
  • Definition 1. It composes M\mathcal MM and A\mathcal AA with the steady-state maps P,Q\mathcal P,\mathcal QP,Q. IsMFE instead asks for some steady state (p,q)(p,q)(p,q); by Proposition 2 the two readings agree.
  • The correspondence. A(q)\mathcal A(q)A(q) is a Set ℝ.
  • Roots and welfare. p^,pˉ\hat p,\bar pp^​,pˉ​ are quantified (any roots above cac_aca​), not chosen. Πa∗,Πe∗\Pi^*_a,\Pi^*_eΠa∗​,Πe∗​ are Wa,WeW_a,W_eWa​,We​ at the MFE's own steady state. log⁡\loglog is Real.log.

Several formalizations would make the goal trivial or false, and none is used:

  • a raw division (1 - exp (-x)) / x in (6)–(7) would make (m,α,p,q)=(0,0,0,0)(m,\alpha,p,q)=(0,0,0,0)(m,α,p,q)=(0,0,0,0) a spurious second equilibrium;
  • an "every MFE satisfies …" goal without the existence-and-uniqueness conjunct would be vacuous;
  • choosing p^,pˉ\hat p,\bar pp^​,pˉ​ by Classical.choose, or P,Q\mathcal P,\mathcal QP,Q in Definition 1, would leave junk values unconstrained;
  • A\mathcal AA as a function would erase the screening-limited equilibrium, which has an interior α∗\alpha^*α∗;
  • M\mathcal MM without the case split p≤cap\le c_ap≤ca​ would make the best response negative.

Proposition 1 (the employer's sequential screening problem, specified only in an online appendix), the application-limit model (8)–(9) with Proposition 3, Theorems 3–7 and the finite-system limit theorems 8–10 are out of scope. Contributions of independent interest are a general lemma on unique roots of strictly convex or concave one-variable functions on an interval, and analytic facts about EEE (positivity, strict monotonicity, E≤1E\le1E≤1 on [0,∞)[0,\infty)[0,∞)).

Selected references

  • N. Arnosti, R. Johari, Y. Kanoria, Managing Congestion in Matching Markets, Manufacturing & Service Operations Management 23(3):620–636, 2021. https://doi.org/10.1287/msom.2020.0927
  • N. Arnosti, R. Johari, Y. Kanoria, Managing Congestion in Matching Markets (full technical report), preprint, 2019. http://dx.doi.org/10.2139/ssrn.2427960
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Theoretical Computer Science·Captain: Yuxuan Xu

Average sensitivity 3.762: refined coupling and a complete Lean proofResearch Paper

Motivation

A polynomial threshold function makes a Boolean decision by evaluating a real polynomial and keeping only its sign. Its average sensitivity measures how often that decision changes after one uniformly chosen input coordinate is reversed, summed over all coordinate choices. This is a basic quantitative question in the analysis of Boolean functions: how much can a low-degree decision rule vary across the edges of the Boolean cube?

The result collected here is a uniform bound with an explicit coefficient. The OpenAI weighted-grading development supplies a complete coefficient-eight construction. Lagdive, Aglave and Damre sharpen its probability estimate and obtain the sufficient coefficient 3.83. The present fixed-source development formalizes the refined estimate, extracts the coefficient 3.762, and connects it to the full polynomial-threshold statement.

This mission organizes that completed result and its reusable supporting theorems. Its goal and both milestones already have accepted Lean proofs. It does not present the coefficient as optimal, and it makes no claim of exhaustive historical priority.

Setting

Let n,dn,dn,d be positive integers, and let ppp be a real polynomial in nnn variables with total degree at most ddd. Choose an input xxx uniformly from the sign cube {−1,1}n\{-1,1\}^n{−1,1}n. For a coordinate iii, write x⊕ix^{\oplus i}x⊕i for the same input with coordinate iii negated. The threshold convention is

f(x)={1,p(x)≥0,−1,p(x)<0.f(x)=\begin{cases}1,&p(x)\ge0,\\-1,&p(x)<0.\end{cases}f(x)={1,−1,​p(x)≥0,p(x)<0.​

In particular, a zero of the polynomial is assigned the positive sign. The average sensitivity is

AS⁡(f)=∑i=1nPr⁡{f(x)≠f(x⊕i)}.\operatorname{AS}(f)=\sum_{i=1}^{n}\Pr\{f(x)\ne f(x^{\oplus i})\}.AS(f)=i=1∑n​Pr{f(x)=f(x⊕i)}.

For the scalar supporting statements, let BnB_nBn​ have the symmetric binomial distribution with parameters nnn and 1/21/21/2. Its mean absolute deviation is

bn=E∣Bn−n/2∣=2−n−1∑j=0n(nj)∣2j−n∣.b_n=\mathbb E|B_n-n/2|=2^{-n-1}\sum_{j=0}^{n}\binom nj|2j-n|.bn​=E∣Bn​−n/2∣=2−n−1j=0∑n​(jn​)∣2j−n∣.

The accompanying definition module fixes this finite sum and the normalized central coefficient ck=4−k(2kk)c_k=4^{-k}\binom{2k}{k}ck​=4−k(k2k​). These definitions contain no estimates or unproved hypotheses.

Formalization targets

Goal — the coefficient 3.762 for arbitrary real polynomials

For every n,d≥1n,d\ge1n,d≥1 and every real polynomial of total degree at most ddd, prove

AS⁡(sign⁡p)≤1881500 dn.\operatorname{AS}(\operatorname{sign}p)\le\frac{1881}{500}\,d\sqrt n.AS(signp)≤5001881​dn​.

The goal is the published theorem AverageSensitivity.polynomial_bound_3762_general. It has no multilinearity hypothesis and no requirement that d≤nd\le nd≤n. The narrower range 1≤d≤n1\le d\le n1≤d≤n used by the Big O board is therefore included. The goal's fixed coefficient records this particular verified result; a future sharper coefficient would be a separate statement.

Milestone 1 — the refined finite one-sided coupling estimate

Let a finite set carry nonnegative probability weights www, and let real functions U,VU,VU,V have identical weighted distributions. Let mmm be any real centre and let a≥0a\ge0a≥0. If V−U≤aV-U\le aV−U≤a on the support of the weights, prove

E(U−V)2≤4aE∣U−m∣+a2.\mathbb E(U-V)^2\le4a\mathbb E|U-m|+a^2.E(U−V)2≤4aE∣U−m∣+a2.

This is the finite form of the first estimate in Lemma 2 of Lagdive, Aglave and Damre. The centre is arbitrary; independence, exchangeability and a two-sided displacement bound are not hypotheses. Its published formalization is already proved.

Milestone 2 — exact extraction of the universal coefficient

For positive integers n,dn,dn,d and a real number AAA, prove the scalar implication

A≤n,A≤8dbn+2d2⟹A≤1881500dn.A\le n,\qquad A\le8db_n+2d^2\quad\Longrightarrow\quad A\le\frac{1881}{500}d\sqrt n.A≤n,A≤8dbn​+2d2⟹A≤5001881​dn​.

This is AverageSensitivity.extract_constant. Its statement is independent of the polynomial and matrix constructions. It records the coefficient extraction proved in this development, rather than attributing 3.762 to the earlier paper.

Significance and current status

The result gives one coefficient that works simultaneously for every positive dimension and degree. Such uniformity distinguishes it from estimates that hold only for a fixed degree or only as the dimension tends to infinity. It also preserves the stated convention at polynomial zeros, so the class of threshold functions is unchanged at the boundary.

The formal contribution is a complete connection from the polynomial and the actual finite cube to the numerical bound. The final theorem does not assume the existence of a grading, an energy bound, a coupling estimate or a small-dimension certificate. Those mathematical components are discharged inside the proof chain. The two supporting milestones are independently importable results, and the live dependency graph records both as actual prerequisites of the goal's accepted reduction.

All three theorem nodes are currently Proved. The closed repository proof was rebuilt with Lean 4.33.1 and the platform's Mathlib revision, and an independent Linux build also passed. The final theorem's axiom dependencies are exactly propext, Classical.choice and Quot.sound. These checks establish the formal result under the displayed definitions; they do not establish optimality of the coefficient or independent human peer review.

Difficulty

A one-sided bound on the difference of two variables does not by itself bound the difference in the opposite direction. The equal-distribution condition is therefore essential to the coupling milestone. Omitting it would change the problem into a false assertion. In the polynomial application, the relevant distributions also have to come from the actual block masses of the constructed grading; treating those masses or the grading properties as free assumptions would omit the central analytic work.

The constant extraction must cover all admissible dimension-degree pairs. A calculation for finitely many dimensions cannot establish the universal statement, while an asymptotic first-moment estimate can leave uncontrolled small dimensions or degree-dependent errors. The formal target includes both the infinite range and every exceptional finite case. Numerical optimization and floating-point experiments are not premises of the accepted result.

Formalization scope

Cube vertices are functions Fin n → Bool, interpreted coordinatewise as signs. A coordinate flip is an explicit function update, and each probability is a finite cardinality divided by 2n2^n2n. The polynomial is a Mathlib MvPolynomial (Fin n) ℝ; the degree bound refers to its total degree. General polynomial inputs are included through a proved value-preserving, degree-nonincreasing multilinearization. Positive dimensions ensure the normalizing denominator is nonzero. Degree zero and dimension zero are outside the displayed goal's quantifiers.

The two definition references provide the original cube/threshold interface and the exact scalar moment interface. The coupling milestone uses finite weighted sums, so equality of distributions is stated for every real test function without additional measurability assumptions. The scalar milestone quantifies over an arbitrary real AAA satisfying its two explicit upper bounds. The main goal has no analogous auxiliary assumptions.

This is a Research Paper mission for a completed fixed-source development, with the main theorem and both milestones linked by their existing identities. It creates no duplicate theorem statements. Alternative proofs and subsequent sharper bounds can reuse these interfaces, but they are not claimed as completed by this mission. The construction and earlier probability refinement remain attributed to their original sources. Proof development and source preparation used OpenAI Codex.

Selected references

  • OpenAI, Average sensitivity of polynomial threshold functions, preprint and Lean source, 2026. Fixed Lean development.
  • Prathmesh Lagdive, Vaibhav Aglave and Suraj Damre, An elementary improvement of the average sensitivity bound for polynomial threshold functions, 2026, Lemma 2 and the dimension-degree estimate. Fixed manuscript source.
  • Anchen0823, Average sensitivity: a Lean proof with coefficient 3.762, source development, 2026. Verified source revision. Prove2Me accepted main submission: 0f539328-c783-4509-a78e-a86ac777468c.
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Control TheoryDynamic ProgrammingOperations Research·Captain: mikedeng1

Wait Time Based Pricing for Queues with Customer-Chosen Service Times: The Delay Differential Optimality Equations Have a Decreasing Concave SolutionResearch Paper

Motivation

Service systems such as public fast-charging stations for electric vehicles let each customer choose how long to be served. Lin, Shang and Sun (SSRN 3709573, 2020; later in Management Science, doi:10.1287/mnsc.2022.4474) study a firm that announces to every arriving customer the current wait time www (the work already in the queue) and a price rate ppp per unit of service time. The customer then decides whether to join and, if so, how long a service to buy. Queue pricing usually conditions on the queue length with random service times (Low 1974; Paschalidis and Tsitsiklis 2000; Kim and Randhawa 2018). Here the state is the wait time, and it moves deterministically between arrivals.

The firm maximizes long-run average revenue or social welfare. The optimality condition the paper derives is not an ordinary differential equation but a delay differential equation (DDE) that looks ahead: the value at www depends on the value at w+t(p)>ww + \mathtt t(p) > ww+t(p)>w. This mission formalizes the paper's existence theorem for that equation.

Setting

A model has a usage utility UUU, a waiting cost ccc, a Poisson arrival rate λ>0\lambda > 0λ>0 and a maximum service time C>0C > 0C>0, under Assumption 1 (p. 7):

  1. U(t)≥0U(t) \ge 0U(t)≥0, U(0)=0U(0) = 0U(0)=0, 0≤U′(t)≤U′(0)0 \le U'(t) \le U'(0)0≤U′(t)≤U′(0) and U′′(t)<0U''(t) < 0U′′(t)<0 on [0,C][0, C][0,C];
  2. d2dt2[U′(t)t]<0\frac{d^2}{dt^2}[U'(t)t] < 0dt2d2​[U′(t)t]<0 on [0,C][0, C][0,C];
  3. c(0)=0c(0) = 0c(0)=0, c′(w)>0c'(w) > 0c′(w)>0 and c′′(w)≥0c''(w) \ge 0c′′(w)≥0 for w≥0w \ge 0w≥0.

At price p∈[0,U′(0)]p \in [0, U'(0)]p∈[0,U′(0)] a joining customer chooses the service time t(p)=min⁡{(U′)−1(p),C}\mathtt t(p) = \min\{(U')^{-1}(p), C\}t(p)=min{(U′)−1(p),C} (5). They join when U(t(p))−p t(p)−c(w)≥0U(\mathtt t(p)) - p\,\mathtt t(p) - c(w) \ge 0U(t(p))−pt(p)−c(w)≥0. Three thresholds follow:

  • wˉ\bar wwˉ solves U(C)=c(wˉ)U(C) = c(\bar w)U(C)=c(wˉ); above it nobody joins.
  • Γ(w)\Gamma(w)Γ(w), for w∈[0,wˉ]w \in [0, \bar w]w∈[0,wˉ], is the highest price at which a customer still joins (Proposition 2).
  • w^\hat ww^ and L(w)L(w)L(w) (Proposition 1) describe when the marginal price U′(t)U'(t)U′(t) still attracts a customer.

The per-customer value is v(p)−αc(w)\mathbf v(p) - \alpha c(w)v(p)−αc(w), with v(p)=p t(p)\mathbf v(p) = p\,\mathtt t(p)v(p)=pt(p), α=0\alpha = 0α=0 for revenue and v(p)=U(t(p))\mathbf v(p) = U(\mathtt t(p))v(p)=U(t(p)), α=1\alpha = 1α=1 for welfare (Lemma 1).

The optimality equations (12)–(15) ask for a constant g\mathsf gg (the average rate) and a relative value function VVV with

g=−V′(w)+λmax⁡{max⁡p∈[0,Γ(w)][v(p)−αc(w)+V(w+t(p))−V(w)], 0},w∈(0,wˉ],\mathsf g = -V'(w) + \lambda \max\Big\{\max_{p \in [0, \Gamma(w)]} \big[\mathbf v(p) - \alpha c(w) + V(w + \mathtt t(p)) - V(w)\big],\ 0\Big\}, \quad w \in (0, \bar w],g=−V′(w)+λmax{p∈[0,Γ(w)]max​[v(p)−αc(w)+V(w+t(p))−V(w)], 0},w∈(0,wˉ], g=λmax⁡{max⁡p∈[0,Γ(0)][v(p)+V(t(p))−V(0)], 0},g=−V′(w) (w>wˉ),V(wˉ)=0.\mathsf g = \lambda \max\Big\{\max_{p \in [0, \Gamma(0)]} \big[\mathbf v(p) + V(\mathtt t(p)) - V(0)\big],\ 0\Big\}, \qquad \mathsf g = -V'(w) \ (w > \bar w), \qquad V(\bar w) = 0.g=λmax{p∈[0,Γ(0)]max​[v(p)+V(t(p))−V(0)], 0},g=−V′(w) (w>wˉ),V(wˉ)=0.

Algorithm 1 (p. 14) is a backward explicit-Euler shooting scheme. For a guess g≥0g \ge 0g≥0 and NNN grid cells on [0,wˉ][0, \bar w][0,wˉ], it starts from VNg(w)=−(w−wˉ)gV^g_N(w) = -(w - \bar w)gVNg​(w)=−(w−wˉ)g for w≥wˉw \ge \bar ww≥wˉ. It then builds a piecewise-linear VNgV^g_NVNg​ cell by cell from right to left. On the cell ending at xxx the slope is −g+KNg(x)-g + K^g_N(x)−g+KNg​(x), where the slope adjustment KNg(x)K^g_N(x)KNg​(x) is λ\lambdaλ times the positive part of the inner maximum at xxx. The shooting value is gN=min⁡{g≥0:g≥KNg(0)}g_N = \min\{g \ge 0 : g \ge K^g_N(0)\}gN​=min{g≥0:g≥KNg​(0)} (23). Finally gˉ=lim⁡jg2j\bar g = \lim_j g_{2^j}gˉ​=limj​g2j​ (24) and Vgˉ(w)=lim⁡jV2jgˉ(w)V^{\bar g}(w) = \lim_j V^{\bar g}_{2^j}(w)Vgˉ​(w)=limj​V2jgˉ​​(w) (Proposition 6).

Formalization targets

Goal: Theorem 1 (p. 17)

gˉ=lim⁡j→∞g2j exists,V2jgˉ(w)→Vgˉ(w) (w≥0),(gˉ,Vgˉ) solves (12)–(15),Vgˉ is nonincreasing and concave on [0,wˉ+C].\bar g = \lim_{j\to\infty} g_{2^j} \ \text{exists},\quad V^{\bar g}_{2^j}(w) \to V^{\bar g}(w)\ (w \ge 0),\quad (\bar g, V^{\bar g}) \text{ solves (12)–(15)},\quad V^{\bar g} \text{ is nonincreasing and concave on } [0, \bar w + C].gˉ​=j→∞lim​g2j​ exists,V2jgˉ​​(w)→Vgˉ​(w) (w≥0),(gˉ​,Vgˉ​) solves (12)–(15),Vgˉ​ is nonincreasing and concave on [0,wˉ+C].

Milestones

The milestones follow the paper's proof in order:

  • Thresholds and the value function (Propositions 1–3, pp. 8–11): uniqueness of w^\hat ww^ and wˉ\bar wwˉ, the characterization (8) of Γ\GammaΓ, Γ(0)=U′(0)\Gamma(0) = U'(0)Γ(0)=U′(0) with Γ\GammaΓ decreasing, and the bounds (V1)–(V2) on v\mathbf vv.
  • The finite-NNN scheme (Proposition 4, Lemmas 2, 3, 5): VNgV^g_NVNg​ is concave and KNgK^g_NKNg​ is nonincreasing; KKK increases when the grid is refined and decreases in ggg; and KNU′(0)≡0K^{U'(0)}_N \equiv 0KNU′(0)​≡0.
  • The limits (Proposition 5, Lemma 6, Proposition 6): g2jg_{2^j}g2j​ increases to gˉ≤U′(0)\bar g \le U'(0)gˉ​≤U′(0), the V2jgˉV^{\bar g}_{2^j}V2jgˉ​​ are uniformly gˉ\bar ggˉ​-Lipschitz, and they converge uniformly to a concave, nonincreasing, Lipschitz VgˉV^{\bar g}Vgˉ​.
  • The equations in the limit (Lemma 7, Propositions 7–8): K2jgˉ(0)→gˉK^{\bar g}_{2^j}(0) \to \bar gK2jgˉ​​(0)→gˉ​; the boundary condition (13); differentiability of VgˉV^{\bar g}Vgˉ​ on [0,wˉ][0, \bar w][0,wˉ] and the DDE (12).

Significance

Theorem 1 is the existence half of the paper's verification argument. Its Theorem 2 then shows that the constructed gˉ\bar ggˉ​ equals the optimal long-run average rate over all predictable price processes. Its Theorem 3 reads the structure of the optimal price and service-time policies off VgˉV^{\bar g}Vgˉ​. Without a solution of (12)–(15) neither result has an object to talk about. The construction also gives a convergent numerical method (Algorithm 1) for a class of look-ahead DDEs that standard ODE theory does not cover.

The proofs are written out in the paper's Appendix B, except Lemma 12, an internal step of Proposition 8 whose proof the authors leave out. None of it is machine-checked. A complete formalization would check every step of the shooting argument and supply the omitted lemma. It would also yield a reusable framework: Euler-type schemes for delay equations whose delay points forward, monotone in the grid and in a scalar parameter.

Difficulty

The obvious approach, Cauchy–Lipschitz, fails: (12) is not an initial-value problem. V′(w)V'(w)V′(w) depends on VVV on [w,w+C][w, w + C][w,w+C], so the equation must be integrated backwards from wˉ\bar wwˉ, and then the value g\mathsf gg is unknown. The shooting scheme fixes ggg, integrates backwards, and tunes ggg so that the boundary condition (13) at w=0w = 0w=0 holds in the limit. For fixed ggg the approximations need not converge as N→∞N \to \inftyN→∞ (the slope at 000 can diverge), so ggg and NNN must be coupled through gNg_NgN​.

The hard step is Proposition 8. Each V2jgˉV^{\bar g}_{2^j}V2jgˉ​​ has kinks at every grid point, yet the limit has to be differentiable. One has to show that the left and right derivatives of the concave limit coincide and equal the right-hand side of (12), which requires passing a maximum over a www-dependent price set to the limit.

Formalization scope

All declarations live in the namespace WaitTimePricing.Existence, and only Mathlib is imported. Conventions:

  • U,c:R→RU, c : \mathbb R \to \mathbb RU,c:R→R are C3C^3C3 and C2C^2C2 on R\mathbb RR, a disclosed strengthening of "three/two times differentiable". Assumption 1's inequalities are imposed exactly on [0,C][0, C][0,C] and [0,∞)[0, \infty)[0,∞). λ>0\lambda > 0λ>0 and C>0C > 0C>0 are added; the paper uses them without stating them.
  • t(p)=sup⁡{t∈[0,C]:p≤U′(t)}\mathtt t(p) = \sup\{t \in [0, C] : p \le U'(t)\}t(p)=sup{t∈[0,C]:p≤U′(t)}, meaningful for p∈[0,U′(0)]p \in [0, U'(0)]p∈[0,U′(0)]. w^\hat ww^, L(w)L(w)L(w), wˉ\bar wwˉ and Γ(w)\Gamma(w)Γ(w) are defined by their characterizing sets, not by closed forms. Propositions 1–2 are theorems about these sets.
  • The objective is one of Lemma 1's two cases. The paper's remark that any v\mathbf vv satisfying (V1)–(V2) would do is not formalized, because it silently needs continuity of v\mathbf vv.
  • Every "max" in (12), (13), (19) and (22) is a real supremum over [0,Γ(w)][0, \Gamma(w)][0,Γ(w)]. For the continuous VVV used here this set is nonempty and bounded, and the supremum is attained.
  • V′V'V′ is never a default-valued derivative. (12) and (14) assert that VVV has the prescribed derivative, two-sided for w∈(0,wˉ]w \in (0, \bar w]w∈(0,wˉ] and w>wˉw > \bar ww>wˉ; Proposition 8 states the case w=0w = 0w=0 with a right derivative.
  • Algorithm 1 is a recursion over the passes of its loop, with N≥1N \ge 1N≥1. The initialization (16) is extended from [wˉ,wˉ+C][\bar w, \bar w + C][wˉ,wˉ+C] to [wˉ,∞)[\bar w, \infty)[wˉ,∞) so that (14) can hold as printed on (wˉ,∞)(\bar w, \infty)(wˉ,∞). Only values on [0,wˉ+C][0, \bar w + C][0,wˉ+C] enter the loop, so the construction is unchanged.
  • gˉ\bar ggˉ​ and VgˉV^{\bar g}Vgˉ​ are defined as limits that take a default value when the limit does not exist. Propositions 5–6 and the goal assert the convergence.
  • "Decreasing" is nonincreasing everywhere (including Γ\GammaΓ, Proposition 2(iii)), the reading the proofs establish.

Trivializations ruled out. The goal names the paper's gˉ\bar ggˉ​ and VgˉV^{\bar g}Vgˉ​ together with their convergence, not an arbitrary solution and not default values of undefined limits. It cannot be met at a kink through a default-valued derivative. Its inner maxima cannot vanish through an empty or unbounded set. Γ\GammaΓ and t\mathtt tt are not closed forms that would make (8) true by definition. The weaker statement "some (g,V)(\mathsf g, V)(g,V) solves (12)–(15)" is not the goal.

Contributions are welcome at every milestone. Reusable pieces include monotonicity of a max-operator under backward induction, Dini-type uniform convergence of monotone sequences of equi-Lipschitz concave functions, and the differentiability of a concave limit of piecewise-linear functions. Theorem 2 (optimality over predictable controls) and Theorem 3 (policy structure) are outside this mission. Theorem 3 appears to fail as printed when gˉ>U′(C)\bar g > U'(C)gˉ​>U′(C).

Selected references

  • C.-A. Lin, K. Shang, P. Sun, Wait Time Based Pricing for Queues with Customer-Chosen Service Times, SSRN 3709573, version of October 12, 2020. https://ssrn.com/abstract=3709573 (journal version: Management Science, https://doi.org/10.1287/mnsc.2022.4474)
  • D. W. Low, Optimal dynamic pricing policies for an M/M/s queue, Operations Research 22(3), 1974. https://doi.org/10.1287/opre.22.3.545
  • I. C. Paschalidis, J. N. Tsitsiklis, Congestion-dependent pricing of network services, IEEE/ACM Transactions on Networking 8(2), 2000. https://doi.org/10.1109/90.842140
  • J. Kim, R. S. Randhawa, The value of dynamic pricing in large queueing systems, Operations Research 66(2), 2018. https://doi.org/10.1287/opre.2017.1668
  • D. P. Bertsekas, Dynamic Programming and Optimal Control, 2nd ed., Athena Scientific, 2000. http://www.athenasc.com/dpbook.html
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Operations ResearchStochastic Systems·Captain: mikedeng1

Provably Good Region Partitioning for On-Time Last-Mile Delivery II: An ε-Equitable Partition Keeps Each Subregion's Delivery Time Within 4η/(1−η)² of OptimalResearch Paper

Motivation

A delivery company can assign each driver a permanent district instead of allowing every driver to serve the whole city. This makes dispatching simpler, but it raises a service question: if the districts receive almost equal shares of demand and travel workload, how different can their expected delivery times be? Carlsson, Liu, Salari and Yu study this question for a region partitioning policy in which one vehicle serves each district. Their Proposition 3 gives an explicit error bound for a partition whose shares are accurate within a tolerance ε. The proposition complements their exact equitability result, Theorem 6, by quantifying the effect of a partition that can only be computed approximately.

Setting

The service region R is a compact convex subset of the Euclidean plane, with depot x₀ ∈ R. Orders arrive at a rate λ and have locations distributed with density f on R. The density is nonnegative, Lipschitz on R, and normalized by ∫_R f(x) dx = 1. There are m ≥ 1 identical vehicles, each with speed v > 0 and capacity q ≥ 1. An order requires a mean on site service time s̄ ≥ 0. The positive constant β is the geometric constant in the paper's heavy traffic delivery time expression. A partition R₁, …, R_m covers R, with districts disjoint up to area zero; vehicle i serves R_i.

For a measurable district S, let p(S) = ∫_S f(x) dx be its share of demand. Its arrival rate is λ_S = λp(S), and its conditional density is f_S(x) = f(x)/p(S) when p(S) > 0. The paper uses two partition measures:

μ1(S)=∫Sf(x) dx,μ2(S)=∫S(sˉvq+2∥x−x0∥)f(x) dx.\mu_1(S)=\int_S\sqrt{f(x)}\,dx,\qquad \mu_2(S)=\int_S(\bar s vq+2\lVert x-x_0\rVert)f(x)\,dx.μ1​(S)=∫S​f(x)​dx,μ2​(S)=∫S​(sˉvq+2∥x−x0​∥)f(x)dx.

The first controls the leading travel term. The second combines service time and radial travel from the depot. A partition is ε equitable when, for every district i and each j ∈ {1,2}, the difference between μ_j(R_i) and μ_j(R)/m has absolute value at most ε.

For vehicle count k, arrival rate a, region S, and density g, write the workload factor as

W(k,a,S,g)=asˉk+2akvq∫S∥x−x0∥g(x) dx.W(k,a,S,g)=\frac{a\bar s}{k} +\frac{2a}{kvq}\int_S\lVert x-x_0\rVert g(x)\,dx.W(k,a,S,g)=kasˉ​+kvq2a​∫S​∥x−x0​∥g(x)dx.

The heavy traffic expression from the paper's Theorem 3 is

L(k,a,S,g)=β2a(1−1/q)2[∫Sg(x) dx]22k2v2(1−W(k,a,S,g))2.L(k,a,S,g)=\frac{\beta^2a(1-1/q)^2 \left[\int_S\sqrt{g(x)}\,dx\right]^2} {2k^2v^2(1-W(k,a,S,g))^2}.L(k,a,S,g)=2k2v2(1−W(k,a,S,g))2β2a(1−1/q)2[∫S​g(x)​dx]2​.

The comparison value is L* = L(m,λ,R,f). For district i, the value L_i = L(1,λ_{R_i},R_i,f_{R_i}) uses that district's own arrival rate, density, and workload factor.

Formalization targets

Proposition 3: approximate districts

For λ > 0 with W(m,λ,R,f) < 1, ε ≥ 0, and an ε equitable partition, define the corrected tolerance factor

η=εmin⁡{μ1(R)/m,  vqλ(1−λμ2(R)mvq)}.\eta=\frac{\varepsilon}{ \min\left\{\mu_1(R)/m,\; \frac{vq}{\lambda}\left(1-\frac{\lambda\mu_2(R)}{mvq}\right) \right\}}.η=min{μ1​(R)/m,λvq​(1−mvqλμ2​(R)​)}ε​.

When η < 1, the target is the two sided estimate

∣Li−L∗∣≤4η(1−η)2L∗for every i.\lvert L_i-L^*\rvert\le \frac{4\eta}{(1-\eta)^2}L^* \qquad\text{for every }i.∣Li​−L∗∣≤(1−η)24η​L∗for every i.

The first milestone rewrites each district's Theorem 3 expression using μ₁(R_i) and μ₂(R_i). The next two milestones give upper and lower comparisons with L*. The final algebraic milestone evaluates the larger of the two relative deviations. These are the displayed steps on the paper's e companion pages ec6 and ec12–ec13.

The printed Proposition 3 uses max in the denominator defining η. Its proof requires min: when the two entries are 1 and 100 and ε = 0.1, a district can have L_i/L* = (1.1/0.999)² ≈ 1.212, while the printed η = 0.001 permits a deviation of only about 0.004. The correction is recorded in the theorem statements and audit notes.

Significance

The bound makes partition accuracy interpretable as a service guarantee. Once both shares are close enough that η < 1, every district's leading delivery time lies in a controlled interval around the flexible policy's benchmark. It states a guarantee for each district, rather than just for a demand weighted average, so it addresses unequal service across the region.

The authors prove the displayed comparison in their accepted manuscript. This mission formalizes the comparison between explicit heavy traffic expressions; it does not claim a new queueing theorem or a machine checked proof of the stochastic model. The reusable output is a precise Lean interface for spatial demand integrals, workload, conditional district densities, and perturbation bounds involving both numerator and denominator errors. The theorem items are proof targets.

Difficulty

The denominator responds to the μ₂ error in the opposite direction from the numerator's response to the μ₁ error. Bounding their ratio requires both the district workload and the lower numerator estimate to stay in their proper sign ranges. Simply squaring the ε share inequalities is invalid until those signs are known. The condition η < 1 supplies the required room; it also rules out a zero probability district under the other hypotheses. The printed choice of max for η fails to control the error in whichever of the two scales is smaller.

Formalization scope

Lean uses EuclideanSpace ℝ (Fin 2), Lebesgue set integrals, and real valued leading terms. The density, region, depot, fleet parameters, and positive β are fixed while λ and ε vary. The source's compactness, convexity, Lipschitz density, normalization, positive vehicle count, speed, and capacity, and nonnegative mean service time are included in a single standing predicate. A partition has null measurable pieces, pairwise disjoint almost everywhere, and exact union R; shared district boundaries have area zero. The goal also states λ > 0, global workload < 1, ε ≥ 0, and η < 1, matching the stable regime and the proof's small ε condition. Capacity q = 1 remains admitted: both leading terms then vanish and the inequality still holds.

The stochastic renewal arrivals, routing policy, and queueing process are outside this development. Theorem 3 supplies the paper's leading expression, applied separately to the full region and each district. Thus L_i and L* here are leading expressions at one fixed λ, not the underlying expected delivery time functions. A fixed positive ε makes η grow near the heavy traffic boundary, so the page's parenthetical “in heavy traffic” is read through the leading expressions used by its proof. The district value is formed from λ_{R_i} and f_{R_i}; it is not defined from the global benchmark or from the right hand side of the first milestone.

A complete proof will need standard facts about set integrals and square roots, the normalization of a conditional density, and inequalities for positive real denominators. The setting definitions can support other region partition comparisons. Contributions establishing these identities and the upper and lower estimates are welcome.

Selected references

  • J. G. Carlsson, S. Liu, N. Salari, and H. Yu, Provably Good Region Partitioning for On-Time Last-Mile Delivery, accepted manuscript, SSRN 3915544; published in Operations Research 72(1), 91–109 (2024), DOI: 10.1287/opre.2021.0588. Proposition 3, printed p. 21; proofs on pp. ec6 and ec12–ec13.
  • D. J. Bertsimas and G. J. van Ryzin, Stochastic and Dynamic Vehicle Routing with General Demand and Interarrival Time Distributions, Advances in Applied Probability 25(4), 947–978 (1993), DOI: 10.2307/1427801. Source of the heavy traffic expression cited as Theorem 3 in the Carlsson et al. manuscript.
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Operations ResearchProbabilityStatistics·Captain: mikedeng1

Scores for Multivariate Distributions and Level Sets II: The Level Set Score (S′)^Γ Is Consistent for the α Level Set {f_Y ∗ w ≥ α}Research Paper

Motivation

A forecaster who issues a probability distribution for a multivariate quantity, such as the joint demand at several locations or the joint returns of several assets, is often judged not on the whole distribution but on a region it implies: the set of outcomes whose cumulative probability, or smoothed density, exceeds a threshold. Such level sets are the multivariate counterpart of quantiles, and they are used as risk regions and as summaries of joint distributions in management science (Abbas, Budescu and Gu 2010) and in density level set estimation (Cadre 2006). To compare competing level set forecasts against realized data, one needs a consistent scoring function: a loss l(A,y)l(A, y)l(A,y) of a candidate set AAA and an outcome yyy whose expectation under the true distribution is smallest at the true level set. For univariate quantiles the answer is classical (the quantile or pinball loss, Gneiting 2011); for general multivariate level sets, the paper notes, scores had not been studied beyond density level sets and univariate quantiles.

Meng, Taylor, Ben Taieb and Li (Operations Research, 2025) obtain such scores by decomposing their L2L^2L2 scoring rule for multivariate distributions into an integral, over the threshold α\alphaα, of scores for the level sets of a smoothed density. This mission formalizes that construction: Theorem 2 of the paper.

Setting

Write Rd\mathbb R^dRd for ddd-dimensional space with Lebesgue measure Ld\mathcal L^dLd and the componentwise order (z≥yz \ge yz≥y means zj≥yjz_j \ge y_jzj​≥yj​ for all jjj). The unknown distribution of the observation YYY is a probability measure PYP_YPY​ on Rd\mathbb R^dRd; the paper writes fYf_YfY​ for its generalized density. Fix a kernel w:Rd→Rw : \mathbb R^d \to \mathbb Rw:Rd→R and a nonnegative integrable weight hhh. The smoothed density is the convolution

(fY∗w)(z)=∫Rdw(z−s) dPY(s).(f_Y * w)(z) = \int_{\mathbb R^d} w(z - s)\, dP_Y(s).(fY​∗w)(z)=∫Rd​w(z−s)dPY​(s).

For w=u=1{⋅≥0}w = u = \mathbb 1\{\cdot \ge 0\}w=u=1{⋅≥0} (the Heaviside function) it is the multivariate CDF FY(z)=PY{s≤z}F_Y(z) = P_Y\{s \le z\}FY​(z)=PY​{s≤z}.

The α\alphaα level set of a function ggg is (display (9), p. 12)

L(g;α)={z∈Rd:g(z)≥α}.L(g;\alpha) = \{ z \in \mathbb R^d : g(z) \ge \alpha \}.L(g;α)={z∈Rd:g(z)≥α}.

A function l(A,y)l(A, y)l(A,y) of a Borel set A⊆RdA \subseteq \mathbb R^dA⊆Rd and a realization yyy is a consistent scoring function for L(fY∗w;α)L(f_Y * w; \alpha)L(fY​∗w;α) if EPY[l(A,∙)]\mathbb E_{P_Y}[l(A, \bullet)]EPY​​[l(A,∙)] is minimized at A=L(fY∗w;α)A = L(f_Y * w;\alpha)A=L(fY​∗w;α), and strictly consistent if that set is the only minimizer (p. 12). The level set score is (display (11), p. 13)

(S′)Γ(A,y;w,h,α)=∫Rd(α−w(z−y)) 1{z∈A} h(z) dz,(S')^\Gamma(A, y; w, h, \alpha) = \int_{\mathbb R^d} \bigl(\alpha - w(z - y)\bigr)\, \mathbb 1\{z \in A\}\, h(z)\, dz,(S′)Γ(A,y;w,h,α)=∫Rd​(α−w(z−y))1{z∈A}h(z)dz,

and the L2L^2L2 scoring rule of the paper is (display (3), p. 8)

S′(PX,y;w,h)=∫Rd(fX∗w)2(z) h(z) dz−2∫Rd(fX∗w)(z) w(z−y) h(z) dz.S'(P_X, y; w, h) = \int_{\mathbb R^d} (f_X * w)^2(z)\, h(z)\, dz - 2 \int_{\mathbb R^d} (f_X * w)(z)\, w(z - y)\, h(z)\, dz.S′(PX​,y;w,h)=∫Rd​(fX​∗w)2(z)h(z)dz−2∫Rd​(fX​∗w)(z)w(z−y)h(z)dz.

In Lean these are smooth, levelSet, scoreΓ, S', cdf and heaviside in the definition item MultivarScores.LevelSet.Setting.

Formalization targets

The paper's Theorem 2 (p. 13) reads:

Let Vd\mathcal V^dVd, hhh, and www satisfy Assumption 1 in the appendix, and www is nonnegative. Let α>0\alpha > 0α>0, and let A⊆RdA \subseteq \mathbb R^dA⊆Rd be an arbitrary Borel set. Suppose (S′)Γ(A,∙;w,h,α)(S')^\Gamma(A, \bullet; w, h, \alpha)(S′)Γ(A,∙;w,h,α) is finite Ld\mathcal L^dLd-a.e. and (S′)Γ(A,∙;w,h,α)fY(∙)(S')^\Gamma(A, \bullet; w, h, \alpha) f_Y(\bullet)(S′)Γ(A,∙;w,h,α)fY​(∙) is integrable. Then the following expression defines a consistent scoring function for the α\alphaα level set L(fY∗w;α)L(f_Y * w; \alpha)L(fY​∗w;α): (S′)Γ(A,y;w,h,α)=∫Rd(α−w(z−y)) 1{z∈A} h(z) dz(S')^\Gamma(A, y; w, h, \alpha) = \int_{\mathbb R^d} (\alpha - w(z - y))\, \mathbb 1\{z \in A\}\, h(z)\, dz(S′)Γ(A,y;w,h,α)=∫Rd​(α−w(z−y))1{z∈A}h(z)dz. (11) If hhh is nonzero Ld\mathcal L^dLd-a.e. and L(fY∗w;α)L(f_Y * w; \alpha)L(fY​∗w;α) equals the closure of {fY∗w>α}\{f_Y * w > \alpha\}{fY​∗w>α}, it is strictly consistent. Moreover, with A=L(fX∗w;α)A = L(f_X * w; \alpha)A=L(fX​∗w;α), the integral of (11) with respect to α\alphaα is precisely half of the L2L^2L2 score in (3), i.e., 12S′(PX,y;w,h)=∫0∞(S′)Γ(L(fX∗w;α),y;w,h,α) dα\tfrac12 S'(P_X, y; w, h) = \int_0^\infty (S')^\Gamma(L(f_X * w; \alpha), y; w, h, \alpha)\, d\alpha21​S′(PX​,y;w,h)=∫0∞​(S′)Γ(L(fX​∗w;α),y;w,h,α)dα.

Goal: consistency

For every Borel AAA and every α>0\alpha > 0α>0,

EPY[(S′)Γ(L(fY∗w;α),∙;w,h,α)]≤EPY[(S′)Γ(A,∙;w,h,α)].\mathbb E_{P_Y}\bigl[(S')^\Gamma(L(f_Y * w;\alpha), \bullet; w, h, \alpha)\bigr] \le \mathbb E_{P_Y}\bigl[(S')^\Gamma(A, \bullet; w, h, \alpha)\bigr].EPY​​[(S′)Γ(L(fY​∗w;α),∙;w,h,α)]≤EPY​​[(S′)Γ(A,∙;w,h,α)].

This is the part of Theorem 2 that holds exactly as printed, and it is the goal.

Strict consistency (milestone)

If moreover h≠0h \ne 0h=0 a.e., Ld{fY∗w=α}=0\mathcal L^d\{f_Y * w = \alpha\} = 0Ld{fY​∗w=α}=0, and Ld(A △ L(fY∗w;α))≠0\mathcal L^d(A \,\triangle\, L(f_Y * w;\alpha)) \ne 0Ld(A△L(fY​∗w;α))=0, the inequality is strict. The null-set condition replaces the printed closure condition (see Formalization scope).

Layer-cake decomposition (milestone)

12S′(PX,y;w,h)=∫0∞(S′)Γ(L(fX∗w;α),y;w,h,α) dα.\tfrac12 S'(P_X, y; w, h) = \int_0^\infty (S')^\Gamma\bigl(L(f_X * w;\alpha), y; w, h, \alpha\bigr)\, d\alpha.21​S′(PX​,y;w,h)=∫0∞​(S′)Γ(L(fX​∗w;α),y;w,h,α)dα.

The other milestones are the steps of the paper's proof (pp. 33–34): the per-realization difference Δ′′\Delta''Δ′′ (p. 33), the expected difference (19) (p. 34), and two companions: the CDF level set score (13) is consistent for L(FY;α)L(F_Y;\alpha)L(FY​;α) (p. 16), and in dimension one it equals the quantile score up to a term depending only on yyy (Remark 2, p. 17).

Significance

Theorem 2 supplies consistent scoring functions for a whole family of multivariate level sets at once, one for each kernel www: CDF level sets (from w=uw = uw=u), density level sets (from w=δ0w = \delta_0w=δ0​) and lower-partial-moment level sets. It thereby gives a way to rank and compare multivariate region forecasts, and in one dimension recovers the full class of quantile scores (Remark 2). The layer-cake identity explains the relation between a distribution score and its level set scores, generalizing the classical identity CRPS=2∫01(quantile score) dα\mathrm{CRPS} = 2\int_0^1(\text{quantile score})\,d\alphaCRPS=2∫01​(quantile score)dα (display (10)); the paper relates its CDF level set score to the Vorob'ev quantile scores of Fissler, Frongillo, Hlavinová and Rudloff (2021).

The result is proved in the paper's appendix (pp. 33–34). It has no machine-checked proof that this mission is aware of. Formalizing it fixes the exact integrability conditions under which the expectations exist (the paper states them loosely in Assumption 1), and it repairs the strict consistency clause, whose printed sufficient condition does not imply what the proof uses.

Difficulty

The core of consistency is a sign argument, but every quantity in it is an integral over Rd\mathbb R^dRd against hhh or against PYP_YPY​, and none of them is a priori finite: www need not be bounded or integrable, and (S′)Γ(A,y)(S')^\Gamma(A, y)(S′)Γ(A,y) must be integrable in yyy for the true level set as well as for the candidate AAA, although the paper assumes it only for AAA. Exchanging the yyy- and zzz-integrals therefore needs a product-integrability condition, not pointwise finiteness. The layer-cake milestone requires the layer cake formula for two different measures (h dzh\,dzhdz and w(z−y)h(z) dzw(z-y)h(z)\,dzw(z−y)h(z)dz), with powers 222 and 111, followed by an exchange that keeps the sign of the second term; a nonnegative (lower) integral cannot express the difference. The strict clause needs a measure-theoretic condition on the boundary {fY∗w=α}\{f_Y * w = \alpha\}{fY​∗w=α}; a topological condition on closures, as printed, is not enough.

Formalization scope

  • Rd\mathbb R^dRd is Fin d → ℝ with volume and the Pi order; ddd is any natural number. A distribution is a probability measure P : Measure (E d); every integral is a Bochner integral.
  • The kernel www is a measurable function. The paper allows a local Borel measure, so that w=δ0w = \delta_0w=δ0​ gives the density level set score (12); that case is not formalized.
  • Standing assumptions. w≥0w \ge 0w≥0 and α>0\alpha > 0α>0 (Theorem 2), h≥0h \ge 0h≥0 measurable and integrable (Assumption 1(a)), AAA Borel.
  • Integrability. Assumption 1 and Theorem 2's "(S′)Γ(A,∙)(S')^\Gamma(A,\bullet)(S′)Γ(A,∙) finite a.e. and (S′)Γ(A,∙)fY(S')^\Gamma(A,\bullet)f_Y(S′)Γ(A,∙)fY​ integrable" are pinned down as the single hypothesis that (s,z)↦w(z−s)h(z)(s, z) \mapsto w(z - s)h(z)(s,z)↦w(z−s)h(z) is integrable for PY⊗LdP_Y \otimes \mathcal L^dPY​⊗Ld. With w,h≥0w, h \ge 0w,h≥0 it covers every Borel set at once, including L(fY∗w;α)L(f_Y * w;\alpha)L(fY​∗w;α). The layer-cake milestone uses Assumption 1(b)/(c) for the given yyy and the almost-everywhere integrability of w(z−⋅)w(z - \cdot)w(z−⋅) under PXP_XPX​.
  • No class Vd\mathcal V^dVd. The consistency statement is pointwise in PYP_YPY​; its convexity is never used.
  • Strict consistency is stated under Ld{fY∗w=α}=0\mathcal L^d\{f_Y * w = \alpha\} = 0Ld{fY​∗w=α}=0 and h≠0h \ne 0h=0 a.e., and "only minimizer" is read modulo Ld\mathcal L^dLd-null sets. The printed condition "L(fY∗w;α)L(f_Y * w;\alpha)L(fY​∗w;α) equals the closure of {fY∗w>α}\{f_Y * w > \alpha\}{fY​∗w>α}" does not imply the null-set property the proof uses: for d=1d = 1d=1, PY=δ0P_Y = \delta_0PY​=δ0​, w=α+dist(⋅,C)w = \alpha + \mathrm{dist}(\cdot, C)w=α+dist(⋅,C) with CCC a fat Cantor set, the closure condition holds but R∖C\mathbb R \setminus CR∖C scores as well as LLL.
  • Level sets use ≥\ge≥, as in (9). The proof's partition by {fY∗w>α}\{f_Y * w > \alpha\}{fY​∗w>α} is a printed slip; the milestones use A∖LA \setminus LA∖L and L∖AL \setminus AL∖A.
  • Ruled out. Because a Bochner integral of a non-integrable function is 000, dropping the integrability hypotheses, letting AAA range over non-measurable sets, or fixing particular www or hhh would trivialize or change the statements; none of these is done.
  • Infrastructure: Mathlib's layer cake (MeasureTheory.lintegral_comp_eq_lintegral_meas_le_mul and relatives in Mathlib/MeasureTheory/Integral/Layercake.lean) and Fubini–Tonelli (integral_prod). A reusable lemma for ∫ ⁣ ⁣∫g(z)w(z−s)h(z) dz dP(s)=∫g(z)(fP∗w)(z)h(z) dz\int\!\!\int g(z) w(z - s) h(z)\,dz\,dP(s) = \int g(z)(f_P * w)(z)h(z)\,dz∫∫g(z)w(z−s)h(z)dzdP(s)=∫g(z)(fP​∗w)(z)h(z)dz is welcome; it also serves the companion mission on the L2L^2L2 scoring rules.

Selected references

  • X. Meng, J. W. Taylor, S. Ben Taieb, S. Li, Scores for Multivariate Distributions and Level Sets, Operations Research, 2025; preprint arXiv:2002.09578v6, 2023. https://arxiv.org/abs/2002.09578
  • T. Gneiting, A. E. Raftery, Strictly Proper Scoring Rules, Prediction, and Estimation, Journal of the American Statistical Association 102(477), 359–378, 2007. https://doi.org/10.1198/016214506000001437
  • T. Gneiting, Making and Evaluating Point Forecasts, Journal of the American Statistical Association 106(494), 746–762, 2011. https://doi.org/10.1198/jasa.2011.r10138
  • T. Fissler, R. Frongillo, J. Hlavinová, B. Rudloff, Forecast Evaluation of Quantiles, Prediction Intervals, and Other Set-Valued Functionals, Electronic Journal of Statistics 15(1), 1034–1084, 2021. https://doi.org/10.1214/21-EJS1808
  • A. E. Abbas, D. V. Budescu, Y. Gu, Assessing Joint Distributions with Isoprobability Contours, Management Science 56(6), 997–1011, 2010. https://doi.org/10.1287/mnsc.1100.1157
  • E. H. Lieb, M. Loss, Analysis, 2nd ed., Graduate Studies in Mathematics 14, AMS, 2001. https://doi.org/10.1090/gsm/014
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Functional AnalysisProbability·Captain: Lucas

Hamburger Moment Problem (Wikipedia) I: Characterization and Uniqueness of SolutionsTextbook

Motivation

A sequence of real numbers (m0,m1,m2,… )(m_0, m_1, m_2, \dots)(m0​,m1​,m2​,…) often arrives as a list of moments: averages E[Xn]\mathbb E[X^n]E[Xn] of powers of a random variable, traces ⟨Tne,e⟩\langle T^n e, e\rangle⟨Tne,e⟩ of powers of a self-adjoint operator, or coefficients of a continued fraction. The Hamburger moment problem, named after Hans Ludwig Hamburger (1920–21), asks when such a list really comes from a measure on the whole real line, and, when it does, whether the measure is determined by its moments. The question sits at the junction of probability (the method of moments, identification of limit laws), spectral theory of symmetric operators and Jacobi matrices, and the theory of orthogonal polynomials; standard monographs include Shohat–Tamarkin (1943) and Schmüdgen (2017).

Timeline (as summarized in the source article and its references):

  1. 1894 — Stieltjes treats the analogous problem on [0,+∞)[0,+\infty)[0,+∞) (the Stieltjes moment problem).
  2. 1920–21 — Hamburger extends the theory to the whole real line: solvability is equivalent to positivity of the Hankel kernel (mj+k)(m_{j+k})(mj+k​).
  3. 1920s — Carleman gives a growth condition on the moments guaranteeing uniqueness (Carleman's condition); the factorial growth bound ∣mn∣≤CDnn!|m_n| \le C D^n n!∣mn​∣≤CDnn! is a special case (Reed–Simon 1975, p. 205).
  4. Later — the operator-theoretic treatment through self-adjoint extensions of the shift operator and its spectral measure becomes standard (Reed–Simon 1975, p. 145).

Setting

Let m=(mn)n≥0m = (m_n)_{n \ge 0}m=(mn​)n≥0​ be a sequence of real numbers. A solution of the Hamburger moment problem for mmm is a positive Borel measure μ\muμ on R\mathbb RR such that every power xnx^nxn is μ\muμ-integrable and

mn=∫−∞∞xn dμ(x)(n=0,1,2,… ).m_n = \int_{-\infty}^{\infty} x^n \, d\mu(x) \qquad (n = 0, 1, 2, \dots).mn​=∫−∞∞​xndμ(x)(n=0,1,2,…).

The sequence mmm is a moment sequence if at least one solution exists.

The Hankel kernel of mmm is the infinite matrix A=(mj+k)j,k≥0A = (m_{j+k})_{j,k \ge 0}A=(mj+k​)j,k≥0​. It is positive definite (in the sense of the source) if

∑j,k≥0mj+k cjck‾  ≥  0\sum_{j,k \ge 0} m_{j+k}\, c_j \overline{c_k} \;\ge\; 0j,k≥0∑​mj+k​cj​ck​​≥0

for every finitary complex sequence (cj)j≥0(c_j)_{j \ge 0}(cj​)j≥0​, i.e. cj=0c_j = 0cj​=0 for all but finitely many jjj. Its finite sections are the (n+1)×(n+1)(n+1)\times(n+1)(n+1)×(n+1) Hankel matrices

Δn=(mi+j)0≤i,j≤n.\Delta_n = (m_{i+j})_{0 \le i,j \le n}.Δn​=(mi+j​)0≤i,j≤n​.

In the Lean development these objects are IsMomentMeasure m μ, IsMomentSequence m, hankelForm m c, HankelPosDef m and hankelMatrix m n, all in the namespace HamburgerMoment.

Formalization targets

Goal — Hamburger's characterization

m is a moment sequence  ⟺  ∑j,k≥0mj+kcjck‾≥0 for every finitary (cj)⊂C.m \text{ is a moment sequence} \iff \sum_{j,k \ge 0} m_{j+k} c_j \overline{c_k} \ge 0 \text{ for every finitary } (c_j) \subset \mathbb C.m is a moment sequence⟺j,k≥0∑​mj+k​cj​ck​​≥0 for every finitary (cj​)⊂C.

Milestones

  1. The identity ∑j,kmj+kcjck‾=∫∣∑jcjxj∣2 dμ(x)\sum_{j,k} m_{j+k} c_j \overline{c_k} = \int |\sum_j c_j x^j|^2 \, d\mu(x)∑j,k​mj+k​cj​ck​​=∫∣∑j​cj​xj∣2dμ(x) for any solution μ\muμ, and the resulting "only if" direction.
  2. The "if" direction: a positive definite Hankel kernel is the kernel of a moment sequence.
  3. The solution set is convex; hence a solvable problem has either a unique solution or infinitely many.
  4. Positivity of AAA gives det⁡Δn≥0\det \Delta_n \ge 0detΔn​≥0 for all nnn; if det⁡Δn=0\det \Delta_n = 0detΔn​=0 for some nnn, the solution is unique and finitely supported.
  5. Uniqueness under the growth bound ∣mn∣≤CDnn!|m_n| \le C D^n n!∣mn​∣≤CDnn!.
  6. Existence of moment sequences with more than one solution.
  7. The real-polynomial identity ∫p2 dμ=∑j,kajakmj+k≥0\int p^2 \, d\mu = \sum_{j,k} a_j a_k m_{j+k} \ge 0∫p2dμ=∑j,k​aj​ak​mj+k​≥0, and the characterization of moment sequences by positive semidefiniteness of all real Hankel matrices Δn\Delta_nΔn​.

Significance

The result. Hamburger's theorem turns an existence question about measures into a family of finite-dimensional positivity conditions that can be checked on the data. It is the basic tool behind the method of moments in probability (identifying a distribution from its moments, when the problem is determinate), behind the spectral theory of Jacobi matrices, and behind Gauss quadrature and orthogonal polynomials on the line. The uniqueness criteria decide when moments determine a law; the non-uniqueness examples (for instance the log-normal distribution) show that they do not always do so.

Formalizing it. All results here are classical and proved in the literature; to the best of the captain's knowledge none of them is currently available as a formal statement in Mathlib, which has neither moment problems nor Hankel kernels. The mission produces a reusable vocabulary (moment measures, Hankel forms and matrices) and machine-checked versions of the existence theorem, the uniqueness criteria and the non-uniqueness phenomenon.

Difficulty

The "only if" direction is a direct computation. The converse is the substance: from positivity of countably many finite quadratic forms one must produce a countably additive measure on a non-compact space with all moments matching. Compactness arguments on finite sections give measures whose low-order moments match, but mass can escape to infinity and higher moments need not converge; the source's route instead goes through the Hilbert space completion of finitary sequences, self-adjoint extensions of the (generally unbounded) shift operator and the spectral theorem for unbounded self-adjoint operators — machinery that is only partly present in Mathlib. An alternative route via positive linear functionals on polynomials (M. Riesz extension, Riesz–Markov–Kakutani) has to control the same escape of mass. The uniqueness criterion requires quasi-analyticity or Carleman-type estimates.

Formalization scope

  1. Sequences are m : ℕ → ℝ; measures are Measure ℝ on the Borel σ-algebra of R\mathbb RR. A solution must have every power xnx^nxn integrable, so in particular μ\muμ is finite with total mass m0m_0m0​.
  2. Finitary complex sequences are finitely supported functions ℕ →₀ ℂ, and the Hankel form is the finite double sum over the support. "≥0\ge 0≥0" is the order on C\mathbb CC (the value is a nonnegative real number), matching the source.
  3. Δn\Delta_nΔn​ is the real matrix indexed by Fin (n + 1); positive semidefiniteness is Mathlib's Matrix.PosSemidef.
  4. Uniqueness statements quantify over all solutions; finite support means the solution vanishes outside a finite set.

Needed infrastructure and welcome contributions: polynomial integrability under finite moments, positive linear functionals on R[x]\mathbb R[x]R[x], a Riesz–Markov or spectral-measure construction on R\mathbb RR, Vandermonde arguments for finitely supported measures, and Carleman / quasi-analyticity estimates. The definitions of moment measures and Hankel kernels are reusable for the Stieltjes and Hausdorff moment problems.

Selected references

  • Wikipedia, Hamburger moment problem, revision oldid=1356180072, https://en.wikipedia.org/w/index.php?title=Hamburger_moment_problem&oldid=1356180072
  • H. Hamburger, Über eine Erweiterung des Stieltjesschen Momentenproblems, Math. Ann. 81 (1920), 235–319; 82 (1921), 120–164, 168–187.
  • M. Reed, B. Simon, Methods of Modern Mathematical Physics II: Fourier Analysis, Self-Adjointness, Academic Press, 1975, pp. 145, 205.
  • T. S. Chihara, An Introduction to Orthogonal Polynomials, Gordon and Breach, 1978, pp. 56, 73.
  • K. Schmüdgen, The Moment Problem, Graduate Texts in Mathematics 277, Springer, 2017. https://doi.org/10.1007/978-3-319-64546-9
  • J. A. Shohat, J. D. Tamarkin, The Problem of Moments, AMS, 1943.
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Mathematical Physics·Captain: Lucas

BCS Theory: the universal gap ratio Δ(0) = (π/e^γ) k_B T_cTextbook

Motivation

The BCS theory of Bardeen, Cooper and Schrieffer (1957) is the microscopic theory of conventional superconductivity in metals; its authors received the 1972 Nobel Prize in Physics. Its most quoted quantitative predictions are universal numbers: in the weak-coupling limit the zero-temperature energy gap and the transition temperature are related by Δ(0)=(π/eγ) kBTc≈1.764 kBTc\Delta(0) = (\pi/e^{\gamma})\,k_BT_c \approx 1.764\,k_BT_cΔ(0)=(π/eγ)kB​Tc​≈1.764kB​Tc​, the gap closes as Δ(T)/Δ(0)≈1.741−T/Tc\Delta(T)/\Delta(0)\approx 1.74\sqrt{1-T/T_c}Δ(T)/Δ(0)≈1.741−T/Tc​​, and the specific heat jumps by (Ces−Cen)/Cen≈1.43(C_{es}-C_{en})/C_{en}\approx 1.43(Ces​−Cen​)/Cen​≈1.43 at TcT_cTc​. These numbers are what experiments compare against, and they follow from a single scalar integral equation, the BCS gap equation. This mission formalizes that mathematical core, following the section Erfolge der BCS-Theorie of the German Wikipedia article BCS-Theorie.

Timeline (as summarized in the source):

  • 1950 — isotope effect observed (Lock et al.; Maxwell; Serin et al.): TcT_cTc​ depends on the ionic mass MMM.
  • 1956 — Cooper shows that an arbitrarily weak attraction binds two electrons above a filled Fermi sea.
  • 1957 — Bardeen, Cooper and Schrieffer publish Theory of Superconductivity, including the gap equation and its consequences.

Setting

Fix the Boltzmann constant kB>0k_B>0kB​>0, the Debye energy ℏωD>0\hbar\omega_D>0ℏωD​>0 (called hbarOmegaD in Lean) and the dimensionless coupling λ=V0 Z(EF)>0\lambda = V_0\,Z(E_F)>0λ=V0​Z(EF​)>0 (called coupling), where V0V_0V0​ is the attractive pairing potential and Z(EF)Z(E_F)Z(EF​) is half the electronic density of states at the Fermi energy. With the quasiparticle energy E(η,Δ)=η2+Δ2E(\eta,\Delta)=\sqrt{\eta^2+\Delta^2}E(η,Δ)=η2+Δ2​ define

I0(ℏωD,Δ)=∫0ℏωDdηη2+Δ2,I(kB,ℏωD,Δ,T)=∫0ℏωDdηη2+Δ2tanh⁡η2+Δ22kBT.I_0(\hbar\omega_D,\Delta)=\int_0^{\hbar\omega_D}\frac{d\eta}{\sqrt{\eta^2+\Delta^2}},\qquad I(k_B,\hbar\omega_D,\Delta,T)=\int_0^{\hbar\omega_D}\frac{d\eta}{\sqrt{\eta^2+\Delta^2}}\tanh\frac{\sqrt{\eta^2+\Delta^2}}{2k_BT}.I0​(ℏωD​,Δ)=∫0ℏωD​​η2+Δ2​dη​,I(kB​,ℏωD​,Δ,T)=∫0ℏωD​​η2+Δ2​dη​tanh2kB​Tη2+Δ2​​.

The zero-temperature gap Δ(0)\Delta(0)Δ(0) is the positive solution of 1/λ=I0(ℏωD,Δ)1/\lambda = I_0(\hbar\omega_D,\Delta)1/λ=I0​(ℏωD​,Δ); the critical temperature TcT_cTc​ is the positive solution of 1/λ=I(kB,ℏωD,0,T)1/\lambda = I(k_B,\hbar\omega_D,0,T)1/λ=I(kB​,ℏωD​,0,T); and for 0<T<Tc0<T<T_c0<T<Tc​ the gap Δ(T)\Delta(T)Δ(T) is the positive solution of 1/λ=I(kB,ℏωD,Δ,T)1/\lambda = I(k_B,\hbar\omega_D,\Delta,T)1/λ=I(kB​,ℏωD​,Δ,T). The Fermi–Dirac function is f(E,T)=1/(eE/kBT+1)f(E,T) = 1/(e^{E/k_BT}+1)f(E,T)=1/(eE/kB​T+1), and 1−2f(E,T)=tanh⁡(E/2kBT)1-2f(E,T) = \tanh(E/2k_BT)1−2f(E,T)=tanh(E/2kB​T).

Formalization targets

Goal: the universal gap ratio

lim⁡λ→0+Δ(0)kBTc=πeγ=1.764…\lim_{\lambda\to0^+}\frac{\Delta(0)}{k_BT_c}=\frac{\pi}{e^{\gamma}}=1.764\ldotsλ→0+lim​kB​Tc​Δ(0)​=eγπ​=1.764…

with γ\gammaγ the Euler–Mascheroni constant. The source writes Δ(T=0)=2ℏωDe−1/V0Z(EF)=πeγkBTc\Delta(T=0)=2\hbar\omega_D e^{-1/V_0Z(E_F)}=\frac{\pi}{e^\gamma}k_BT_cΔ(T=0)=2ℏωD​e−1/V0​Z(EF​)=eγπ​kB​Tc​; both equalities are weak-coupling asymptotics, so the goal is stated as a limit λ→0+\lambda\to0^+λ→0+ at fixed kBk_BkB​, ℏωD\hbar\omega_DℏωD​.

Milestones

  1. I0(ℏωD,Δ)=arsinh⁡(ℏωD/Δ)I_0(\hbar\omega_D,\Delta) = \operatorname{arsinh}(\hbar\omega_D/\Delta)I0​(ℏωD​,Δ)=arsinh(ℏωD​/Δ).
  2. Δ(0)=ℏωD/sinh⁡(1/λ)\Delta(0)=\hbar\omega_D/\sinh(1/\lambda)Δ(0)=ℏωD​/sinh(1/λ), the unique positive solution of the T=0T=0T=0 gap equation.
  3. Δ(0)∼2ℏωDe−1/λ\Delta(0)\sim 2\hbar\omega_D e^{-1/\lambda}Δ(0)∼2ℏωD​e−1/λ as λ→0+\lambda\to0^+λ→0+.
  4. The Fermi–Dirac and tanh⁡\tanhtanh forms of the finite-temperature gap equation agree.
  5. The TcT_cTc​ equation has exactly one positive solution.
  6. kBTc∼2eγπℏωDe−1/λk_BT_c\sim\frac{2e^\gamma}{\pi}\hbar\omega_D e^{-1/\lambda}kB​Tc​∼π2eγ​ℏωD​e−1/λ (the source's 1,141{,}141,14).
  7. Isotope effect: with ℏωD=C/M\hbar\omega_D = C/\sqrt MℏωD​=C/M​, Tc∝M−1/2T_c\propto M^{-1/2}Tc​∝M−1/2.
  8. Δ(T)\Delta(T)Δ(T) exists uniquely for 0<T<Tc0<T<T_c0<T<Tc​, and the gap equation has no positive solution for T≥TcT\ge T_cT≥Tc​.
  9. Near TcT_cTc​: Δ(T)2/(1−T/Tc)\Delta(T)^2/(1-T/T_c)Δ(T)2/(1−T/Tc​) has a limit L(λ)L(\lambda)L(λ) as T→Tc−T\to T_c^-T→Tc−​, and L(λ)/Δ(0)2→8e2γ/(7ζ(3))=1.73672L(\lambda)/\Delta(0)^2\to 8e^{2\gamma}/(7\zeta(3)) = 1.7367^2L(λ)/Δ(0)2→8e2γ/(7ζ(3))=1.73672 as λ→0+\lambda\to0^+λ→0+.
  10. Specific-heat jump: the left derivative D(λ)D(\lambda)D(λ) of Δ(T)2\Delta(T)^2Δ(T)2 at TcT_cTc​ exists, and −D(λ)/(2π23kB2Tc)→12/(7ζ(3))=1.426…-D(\lambda)/(\tfrac{2\pi^2}{3}k_B^2T_c)\to 12/(7\zeta(3)) = 1.426\ldots−D(λ)/(32π2​kB2​Tc​)→12/(7ζ(3))=1.426….

Significance

The universal ratios are the standard quantitative test that separates weak-coupling (BCS-like) superconductors from strong-coupling ones; deviations from 1.7641.7641.764 and 1.431.431.43 are used to diagnose strong electron–phonon coupling. Mathematically, each statement is an assertion about a parameter-dependent integral equation and its asymptotics as λ→0+\lambda\to0^+λ→0+, with the Euler–Mascheroni constant and ζ(3)\zeta(3)ζ(3) arising from the asymptotics of ∫0Xtanh⁡(x)/x dx\int_0^X\tanh(x)/x\,dx∫0X​tanh(x)/xdx and from a Sommerfeld-type expansion near TcT_cTc​. These results are classical in the physics literature; the mission aims at a machine-checked derivation of the textbook constants from the gap equation, together with reusable lemmas on monotone parameter-dependent integrals.

Difficulty

The T=0T=0T=0 statements reduce to an explicit antiderivative. The finite-temperature statements do not: TcT_cTc​ and Δ(T)\Delta(T)Δ(T) are defined only implicitly, so the asymptotics require a uniform expansion ∫0Xtanh⁡(x)/x dx=log⁡X+log⁡(4eγ/π)+o(1)\int_0^X\tanh(x)/x\,dx=\log X+\log(4e^\gamma/\pi)+o(1)∫0X​tanh(x)/xdx=logX+log(4eγ/π)+o(1). The near-TcT_cTc​ and specific-heat statements additionally concern the behaviour of Δ(T)2\Delta(T)^2Δ(T)2 at the boundary point TcT_cTc​, where Δ\DeltaΔ itself is not differentiable, and the evaluation of the resulting coefficient in the limit ℏωD/kBTc→∞\hbar\omega_D/k_BT_c\to\inftyℏωD​/kB​Tc​→∞.

Formalization scope

  • All quantities are real numbers. Δ(0)\Delta(0)Δ(0), TcT_cTc​ and Δ(T)\Delta(T)Δ(T) are defined as real suprema (sSup) of the corresponding positive solution sets, so they equal 000 when no positive solution exists; existence and uniqueness are separate milestones. In particular Δ(T)=0\Delta(T)=0Δ(T)=0 for T≥TcT\ge T_cT≥Tc​.
  • The zero-temperature gap is a separate definition: at T=0T=0T=0 the finite-temperature integrand is not used.
  • The coupling enters only through λ=V0Z(EF)\lambda = V_0Z(E_F)λ=V0​Z(EF​); asymptotic claims are limits λ→0+\lambda\to0^+λ→0+ at fixed kB,ℏωD>0k_B,\hbar\omega_D>0kB​,ℏωD​>0, with the exact constants 2eγ/π2e^\gamma/\pi2eγ/π, 8e2γ/(7ζ(3))8e^{2\gamma}/(7\zeta(3))8e2γ/(7ζ(3)) and 12/(7ζ(3))12/(7\zeta(3))12/(7ζ(3)) in place of the rounded 1,141{,}141,14, 1,7421{,}74^21,742 and 1,431{,}431,43. ζ(3)\zeta(3)ζ(3) is written as the real part of riemannZeta 3.
  • The specific heat is not modeled thermodynamically; the jump milestone formalizes the source's closed-form expression in terms of −dΔ2/dT-d\Delta^2/dT−dΔ2/dT at TcT_cTc​.
  • Needed infrastructure: monotonicity and continuity of parameter-dependent interval integrals, the integral identity for arsinh⁡\operatorname{arsinh}arsinh, asymptotics of ∫0Xtanh⁡x/x dx\int_0^X\tanh x/x\,dx∫0X​tanhx/xdx, and Mathlib's Euler–Mascheroni constant and ζ(3)\zeta(3)ζ(3).

Selected references

  • J. Bardeen, L. N. Cooper, J. R. Schrieffer, Theory of Superconductivity, Phys. Rev. 108, 1175 (1957). https://doi.org/10.1103/PhysRev.108.1175
  • L. N. Cooper, Bound Electron Pairs in a Degenerate Fermi Gas, Phys. Rev. 104, 1189 (1956). https://doi.org/10.1103/PhysRev.104.1189
  • Wikipedia (de), BCS-Theorie, section Erfolge der BCS-Theorie (source used for all statements). https://de.wikipedia.org/wiki/BCS-Theorie
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Mathematical Physics·Captain: Lucas

Titius–Bode Law I: The −25%/+50% Coverage Band of Doubling Distance RulesTextbook

Motivation

The Titius–Bode law is an empirical rule, published in the eighteenth century by J. D. Titius and J. E. Bode, for the semi-major axes of the planets: in units in which the Earth's semi-major axis is 101010, the planets lie near 4+x4+x4+x with x=0,3,6,12,24,48,96,…x = 0, 3, 6, 12, 24, 48, 96, \dotsx=0,3,6,12,24,48,96,…. It anticipated the positions of Uranus (1781) and Ceres (1801), failed for Neptune (1846), and has since become a standard example of how a numerical pattern can fit data without a physical mechanism. Dermott's law (S. F. Dermott, 1968) is the analogous power law T(n)=T(0) CnT(n) = T(0)\,C^nT(n)=T(0)Cn for the orbital periods of the major satellites of Jupiter, Saturn and Uranus.

Much of the debate about such rules is quantitative rather than physical. The Wikipedia article on the law records, in a footnote to its data table, the observation that because consecutive predicted distances roughly double, an arbitrary planet may be found within −25%-25\%−25% to +50%+50\%+50% of one of the predicted positions. In other words, the agreement of any single body with the rule at that level carries no information. This mission formalizes that observation and the elementary arithmetic of the law as stated in the source.

Timeline (as recorded in the source). Gregory (1702, 1715) and Wolff (1723–24) give the sequence 4,7,10,16,52,1004, 7, 10, 16, 52, 1004,7,10,16,52,100; Titius (1766) and Bode (1772) publish the rule; Uranus (1781) and Ceres (1801) fit it; Neptune (1846) does not; Blagg (1913) and Richardson (1945) replace the ratio 222 by about 1.731.731.73; Dermott (1968) proposes the period law for satellite systems; Nieto (1970, 1972) reviews the subject.

Setting

For a formal exponent n∈{−∞,0,1,2,… }n \in \{-\infty, 0, 1, 2, \dots\}n∈{−∞,0,1,2,…} put 2−∞=02^{-\infty} = 02−∞=0. The Titius–Bode distance in astronomical units is

a(n)=0.4+0.3⋅2n,n=−∞,0,1,2,…,a(n) = 0.4 + 0.3 \cdot 2^{n}, \qquad n = -\infty, 0, 1, 2, \dots,a(n)=0.4+0.3⋅2n,n=−∞,0,1,2,…,

so a(−∞)=0.4a(-\infty) = 0.4a(−∞)=0.4, a(0)=0.7a(0) = 0.7a(0)=0.7, a(1)=1.0a(1) = 1.0a(1)=1.0, a(2)=1.6,…a(2) = 1.6, \dotsa(2)=1.6,…. The same numbers appear in three other guises in the source: the original form 4+x4 + x4+x (Earth =10=10=10), the form 4+3⋅2n4 + 3 \cdot 2^n4+3⋅2n (Earth =10=10=10), and the canonical form an=0.4+0.3⋅2na_n = 0.4 + 0.3 \cdot 2^nan​=0.4+0.3⋅2n for n=0,1,2,…n = 0, 1, 2, \dotsn=0,1,2,…. The relative deviation of an observed value ddd from a predicted value ppp is (d−p)/p(d - p)/p(d−p)/p, which the source reports as a percentage.

Dermott's law models the period of the nnn-th satellite as T(n)=T(0) CnT(n) = T(0)\,C^nT(n)=T(0)Cn. Kepler's third law makes the semi-major axis proportional to the 2/32/32/3 power of the period, a=K T2/3a = K\,T^{2/3}a=KT2/3.

Formalization targets

Goal: the coverage band

∀d≥0.3:∃ n∈{−∞,0,1,2,… },−14  ≤  d−a(n)a(n)  ≤  12.\forall d \ge 0.3:\quad \exists\, n \in \{-\infty,0,1,2,\dots\},\qquad -\tfrac14 \;\le\; \frac{d - a(n)}{a(n)} \;\le\; \tfrac12 .∀d≥0.3:∃n∈{−∞,0,1,2,…},−41​≤a(n)d−a(n)​≤21​.

Every distance of at least 0.30.30.3 au lies within −25%-25\%−25% to +50%+50\%+50% of some Titius–Bode position. The lower limit 0.3=34⋅0.40.3 = \tfrac34 \cdot 0.40.3=43​⋅0.4 is exactly where the statement begins to hold: below it no predicted position is close enough. The source says "an arbitrary planet"; the formal statement makes the range explicit.

Supporting milestones

  1. The four representations of the rule (original, Earth =10=10=10, au, canonical) agree.
  2. The recursion an+1=2an−0.4a_{n+1} = 2a_n - 0.4an+1​=2an​−0.4 holds for the canonical form; started from a0=0.55a_0 = 0.55a0​=0.55, as printed in the source, it produces the canonical sequence shifted by one index.
  3. The predicted distances in the data table: 0.4,0.7,1.0,1.6,2.8,5.2,10.0,19.6,38.80.4, 0.7, 1.0, 1.6, 2.8, 5.2, 10.0, 19.6, 38.80.4,0.7,1.0,1.6,2.8,5.2,10.0,19.6,38.8 au, and 77.277.277.2 au for the next term.
  4. Consecutive predicted distances less than double, with ratio tending to 222.
  5. The abstract principle behind the goal: for any unbounded sequence with pk+1≤2pkp_{k+1} \le 2p_kpk+1​≤2pk​, every d≥34p0d \ge \tfrac34 p_0d≥43​p0​ lies within −25%-25\%−25% to +50%+50\%+50% of some pkp_kpk​.
  6. The 2:32{:}32:3 resonance figures: semi-major axes of bodies with periods in ratio 2:32{:}32:3 differ by −23.69%-23.69\%−23.69% and +31.04%+31.04\%+31.04% relative to one another.
  7. Dermott's law gives geometric spacing of periods (ratio CCC) and, through Kepler's third law, of semi-major axes (ratio C2/3C^{2/3}C2/3).

Significance

The goal makes precise why a fit of a single body to the Titius–Bode rule within tens of percent is weak evidence: the predicted positions are spaced so that the whole half-line [0.3,∞)[0.3, \infty)[0.3,∞) is covered by such bands. The resonance milestone gives the corresponding figures for a 2:32{:}32:3 period commensurability, and the Dermott milestone connects period power laws to Titius–Bode-type distance laws, as the source asserts.

All results are elementary and none is open. The value of the mission is a checked, unambiguous record of the arithmetic claims in the source, including one place where the source's formulas disagree: the "recursive form" with a0=0.55a_0 = 0.55a0​=0.55 does not reproduce the canonical form index-for-index but is shifted by one (milestone 2). No machine-checked version of these statements is known to exist on the platform.

Difficulty

There is no deep obstacle. The covering argument needs care in two places: the first step of the rule (0.4→0.70.4 \to 0.70.4→0.7) is not a doubling, and the generic doubling lemma must locate the first term that exceeds ddd without assuming monotonicity. The resonance milestone requires certified numerical bounds on the irrational numbers (2/3)2/3(2/3)^{2/3}(2/3)2/3 and (3/2)2/3(3/2)^{2/3}(3/2)2/3 that are tight enough to fix the second decimal place of a percentage.

Formalization scope

Distances, periods and deviations are real numbers. The exponent set {−∞,0,1,2,… }\{-\infty, 0, 1, 2, \dots\}{−∞,0,1,2,…} is encoded as the natural numbers with a bottom element adjoined, and 2−∞2^{-\infty}2−∞ is defined to be 000. The relative deviation is the plain quotient (d−p)/p(d-p)/p(d−p)/p; every statement only evaluates it at positive ppp. Percent figures from the source (−23.69%-23.69\%−23.69%, +31.04%+31.04\%+31.04%) are stated as "within 0.0050.0050.005 percentage points", i.e. correct to the two decimals printed. Kepler's law enters only as the hypothesis a=K T2/3a = K\,T^{2/3}a=KT2/3 with K>0K > 0K>0; no orbital mechanics is formalized. The doubling lemma is stated for an arbitrary real sequence and is reusable for any Titius–Bode-type rule.

Trivializing encodings are ruled out: the goal is not stated for an empty or bounded range of ddd, the predicted set is the full image of the rule, and the deviation band is the one printed in the source.

Selected references

  • Wikipedia, Titius–Bode law, revision 1372822920. https://en.wikipedia.org/w/index.php?title=Titius%E2%80%93Bode_law&oldid=1372822920
  • Wikipedia, Dermott's law, revision 1315813288. https://en.wikipedia.org/w/index.php?title=Dermott%27s_law&oldid=1315813288
  • M. M. Nieto, Conclusions about the Titius–Bode Law of Planetary Distances, Astronomy and Astrophysics 8 (1970), 105–111.
  • S. F. Dermott, On the origin of commensurabilities in the solar system – II: The orbital period relation, MNRAS 141 (1968), 363–376. https://doi.org/10.1093/mnras/141.3.363
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Partial Differential Equations·Captain: mikedeng1

Local Exponential H² Stabilization of a 2 × 2 Quasilinear Hyperbolic System Using Backstepping 1: The 4 × 4 Goursat-Type Kernel System Has a Unique Continuous SolutionResearch Paper

Why kernel well-posedness matters

Boundary control of a transport equation acts at the edge of a spatial interval, while the state evolves throughout the interval. A backstepping transformation connects the original state to a simpler target state by integrating against kernels on a triangular region. The transformation is useful only when those kernels exist with the regularity and uniqueness needed to define a single feedback law. Coron, Vazquez, Krstic and Bastin use this construction for a two-component quasilinear hyperbolic system. Their Appendix A isolates a four-component linear kernel system and proves its well-posedness independently of the later stability arguments (Coron et al., Appendix A).

This mission concerns that appendix result. The paper states a generic system broad enough to include the kernel equations arising from its controller design. Its goal is a unique continuous solution on the closed triangle, assuming continuous coefficients and strictly positive transport speeds. The result supplies the existence and uniqueness premise for the paper's later linear and quasilinear stabilization results. It is a proved result in the source preprint; the work here is to state its analytic content precisely in Lean and leave its proof as a formalization target.

Setting

Let T={(x,ξ):0≤ξ≤x≤1}\mathcal T=\{(x,\xi):0\le\xi\le x\le1\}T={(x,ξ):0≤ξ≤x≤1}. There are four unknown real functions F1,…,F4F^1,\ldots,F^4F1,…,F4 on T\mathcal TT. Two positive, continuous functions ϵ1,ϵ2\epsilon_1,\epsilon_2ϵ1​,ϵ2​ describe the characteristic speeds. Four functions gjg_jgj​ supply forcing, and sixteen functions CjiC_{ji}Cji​ couple the unknown components. The functions gjg_jgj​ and CjiC_{ji}Cji​ are continuous on T\mathcal TT. Boundary functions hj,qjh_j,q_jhj​,qj​ are continuous on [0,1][0,1][0,1]. The paper's equations (A.1)–(A.4) have first-order directional derivatives of FjF^jFj on the left and gj+∑iCjiFig_j+\sum_i C_{ji}F^igj​+∑i​Cji​Fi on the right (Coron et al., p. 18).

The boundary data have two forms. Components F2F^2F2 and F3F^3F3 are prescribed on the diagonal ξ=x\xi=xξ=x: F2(x,x)=h2(x)F^2(x,x)=h_2(x)F2(x,x)=h2​(x) and F3(x,x)=h3(x)F^3(x,x)=h_3(x)F3(x,x)=h3​(x). Components F1F^1F1 and F4F^4F4 are prescribed on the lower edge ξ=0\xi=0ξ=0 with linear dependence on F2(x,0)F^2(x,0)F2(x,0) and F3(x,0)F^3(x,0)F3(x,0). For example, F1(x,0)=h1(x)+q1(x)F2(x,0)+q2(x)F3(x,0)F^1(x,0)=h_1(x)+q_1(x)F^2(x,0)+q_2(x)F^3(x,0)F1(x,0)=h1​(x)+q1​(x)F2(x,0)+q2​(x)F3(x,0). The fourth component uses q3,q4q_3,q_4q3​,q4​ in the same way. Those edge couplings are part of the problem, rather than optional side conditions.

For merely continuous FjF^jFj, a classical partial derivative need not exist. Accordingly, the mission uses the paper's characteristic integral equations (A.23) as the meaning of solution. The travel-time coordinates are ϕi(x)=∫0xϵi(z)−1 dz\phi_i(x)=\int_0^x\epsilon_i(z)^{-1}\,dzϕi​(x)=∫0x​ϵi​(z)−1dz for i=1,2i=1,2i=1,2, with ϕ3=ϕ1+ϕ2\phi_3=\phi_1+\phi_2ϕ3​=ϕ1​+ϕ2​. Each characteristic starts on the prescribed part of the boundary and ends at (x,ξ)(x,\xi)(x,ξ). The value of Fj(x,ξ)F^j(x,\xi)Fj(x,ξ) equals its starting boundary value plus the forcing and coupling integrals along that characteristic. A continuously differentiable solution of the differential equations and the boundary conditions satisfies this integral form (Coron et al., pp. 19–20).

Formalization targets

The goal is Theorem A.1: for every set of data with the continuity and positivity assumptions above, there is a continuous characteristic solution FFF on T\mathcal TT, and any two such solutions agree at every point of T\mathcal TT:

∃F∈C(T)4  CharSolution⁡(F),∀F,F′∈C(T)4,CharSolution⁡(F)∧CharSolution⁡(F′)⟹F=F′ on T.\exists F\in C(\mathcal T)^4\;\operatorname{CharSolution}(F),\qquad \forall F,F'\in C(\mathcal T)^4,\quad \operatorname{CharSolution}(F)\land\operatorname{CharSolution}(F')\Longrightarrow F=F'\text{ on }\mathcal T.∃F∈C(T)4CharSolution(F),∀F,F′∈C(T)4,CharSolution(F)∧CharSolution(F′)⟹F=F′ on T.

Four source results mark the path to that goal. Lemma A.3 keeps every characteristic in T\mathcal TT and records its continuity and coordinate inequalities. Lemma A.4 bounds the integral of the nnnth power of its first coordinate by Kϵxn+1/(n+1)K_\epsilon x^{n+1}/(n+1)Kϵ​xn+1/(n+1). Lemma A.5 bounds one application of the linear integral operator to an increment satisfying a factorial estimate. Proposition A.6 bounds the resulting infinite series by ϕˉexp⁡(CˉKϵx)\bar\phi\exp(\bar C K_\epsilon x)ϕˉ​exp(CˉKϵ​x) (Coron et al., pp. 19, 21–23). These are the mission's four milestones.

Significance

Theorem A.1 fixes a genuine mathematical issue behind the feedback construction: a kernel cannot be treated as an arbitrary coefficient of a controller when its defining boundary problem has not been solved. Existence gives a kernel for the transformation; uniqueness makes that kernel determined by the coefficient data. The theorem is stated for a generic coupled system, so the same result can support several kernels rather than just one equation in the control design (Coron et al., Appendix A).

Formalizing this known proof would add a reusable interface for characteristic coordinates, bounded coefficient functions on a triangle, and coupled Volterra-type integral operators. The present proposal contains statements, not completed proofs. The local prior-art search found no published Goursat kernel item with the same four-component system and boundary conventions. The broader paper's linear and quasilinear stability results are separate missions; this one records their analytic kernel prerequisite without importing their controller definitions.

Difficulty

The mixed boundaries make the usual one-direction transport picture insufficient. Two characteristic families enter from ξ=0\xi=0ξ=0, while two enter from the diagonal. Moreover, the lower-edge values of F1F^1F1 and F4F^4F4 depend on the other components at that edge. Thus a bound for one component cannot ignore the other three or assume all boundary values are given independently. A candidate continuous solution must also be shown to agree with the same integral equations at the corner and along both boundary segments. The explicit characteristics involve the inverse of ϕ3\phi_3ϕ3​, whose argument and range must be checked throughout T\mathcal TT (Coron et al., pp. 19–23).

Formalization scope

The Lean data bundle contains globally defined real functions, with continuity and positivity imposed only on [0,1][0,1][0,1] or T\mathcal TT. Such functions represent continuous data on those closed domains by extension; values outside the domains do not enter the statements. The four components use Fin 4, indexed 0,1,2,30,1,2,30,1,2,3 in Lean for the paper's 1,2,3,41,2,3,41,2,3,4. The two lower-edge couplings and the two diagonal values are all included in IsCharSolution. Equality in the uniqueness clause is restricted to T\mathcal TT, because the extensions outside it are unconstrained.

The coordinate inverses are Function.invFunOn on [0,1][0,1][0,1]; only arguments in their ranges have mathematical meaning here. Lemma A.3 includes the domain facts that keep the characteristics in range. Integrals are over finite characteristic intervals with continuous integrands, and the maxima in (A.35) are suprema of continuous images of compact sets, not suprema over all real inputs. Proposition A.6 asserts summability before using an infinite sum. Lemmas A.4 and A.5 include n=0n=0n=0, a valid base case needed by the source's induction. Lemma A.5 makes the continuity of the increment explicit so its integrals retain their intended values. Existence and uniqueness both remain in the goal; retaining only one would change Theorem A.1. Two formalizations would trivialize or falsify the goal and are ruled out: dropping the boundary conditions (A.5)–(A.7) from the solution notion makes uniqueness false, and reading the PDEs (A.1)–(A.4) classically for a merely continuous FFF would make existence false; the solution notion is the paper's characteristic integral form with all boundary conditions. Contributions to the characteristic and operator estimates, continuity of the constructed limit, and the uniqueness argument are within scope.

Selected references

  • J.-M. Coron, R. Vazquez, M. Krstic and G. Bastin, Local Exponential H² Stabilization of a 2 × 2 Quasilinear Hyperbolic System Using Backstepping, arXiv preprint arXiv:1208.6475v1, 2012, Appendix A, pp. 18–23. Preprint.
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Mathematical Physics·Captain: Lucas

Feynman 1948: The Path-Integral Wave Function Satisfies Schrödinger's EquationResearch Paper

Motivation

In 1948 R. P. Feynman published a third formulation of non-relativistic quantum mechanics, alongside Schrödinger's differential equation and Heisenberg's matrix algebra (Feynman 1948). The probability amplitude for a particle to follow a path x(t)x(t)x(t) is postulated to be exp⁡(iℏS[x])\exp\big(\tfrac{i}{\hbar}S[x]\big)exp(ℏi​S[x]), with SSS the classical action, and the amplitude to arrive at (x,t)(x,t)(x,t) is the sum of these contributions over all paths from the past. This is the path integral, now a standard tool across quantum field theory, statistical mechanics and probability.

The formulation is claimed to be mathematically equivalent to ordinary quantum mechanics. The key step of that claim is Section 6 of the paper, "The wave equation": the wave function defined by the path integral satisfies Schrödinger's equation. This mission formalizes that step for a particle in one dimension, as the paper does.

Timeline:

  • 1933/1945 — Dirac remarks on the role of the classical action in quantum mechanics, the starting point cited by Feynman.
  • 1948 — Feynman, Rev. Mod. Phys. 20, 367: path-integral postulates, definition of the wave function (Section 5), derivation of Schrödinger's equation (Section 6).
  • 1949 — Kac gives the rigorous imaginary-time (Wiener-measure) analogue, the Feynman–Kac formula.
  • 1964 — Nelson derives the real-time Feynman formula rigorously from the Trotter product formula; oscillatory-integral approaches follow later.

Setting

Fix ℏ>0\hbar>0ℏ>0, a mass m>0m>0m>0 and a potential V:R→RV:\mathbb R\to\mathbb RV:R→R. For a time step ε>0\varepsilon>0ε>0 the short-time action between positions yyy (time ttt) and xxx (time t+εt+\varepsilont+ε) is (Eq. 22)

S(x,y)=mε2(x−yε)2−εV(x),S(x,y)=\frac{m\varepsilon}{2}\Big(\frac{x-y}{\varepsilon}\Big)^2-\varepsilon V(x),S(x,y)=2mε​(εx−y​)2−εV(x),

and the normalizing factor is A(ε)=(2πℏεi/m)1/2A(\varepsilon)=(2\pi\hbar\varepsilon i/m)^{1/2}A(ε)=(2πℏεi/m)1/2 (Eq. 28, principal branch). The one-step path-integral evolution (Eqs. 18, 23) takes a wave function ψ:R→C\psi:\mathbb R\to\mathbb Cψ:R→C to

(Uεψ)(x)=1A(ε)∫Rexp⁡ ⁣(iℏS(x,y))ψ(y) dy.(U_\varepsilon\psi)(x)=\frac{1}{A(\varepsilon)}\int_{\mathbb R}\exp\!\Big(\frac{i}{\hbar}S(x,y)\Big)\psi(y)\,dy .(Uε​ψ)(x)=A(ε)1​∫R​exp(ℏi​S(x,y))ψ(y)dy.

Iterating UεU_\varepsilonUε​ and letting ε→0\varepsilon\to0ε→0 is the path integral (15) of Section 5. The Hamiltonian is Hψ=−ℏ22mψ′′+VψH\psi=-\frac{\hbar^2}{2m}\psi''+V\psiHψ=−2mℏ2​ψ′′+Vψ. The paper also uses the Gaussian moments of Eq. (26), which are oscillatory; footnote 13 defines them by replacing ℏ\hbarℏ with ℏ(1−iδ)\hbar(1-i\delta)ℏ(1−iδ) and letting δ→0+\delta\to0^+δ→0+:

Mn(δ)=∫Rξnexp⁡ ⁣(imξ22ℏ(1−iδ)ε)dξ.M_n(\delta)=\int_{\mathbb R}\xi^n\exp\!\Big(\frac{im\xi^2}{2\hbar(1-i\delta)\varepsilon}\Big)d\xi .Mn​(δ)=∫R​ξnexp(2ℏ(1−iδ)εimξ2​)dξ.

Formalization targets

Goal — Eq. (30)

For every Schwartz function ψ\psiψ and every x∈Rx\in\mathbb Rx∈R,

lim⁡ε→0+(Uεψ)(x)−ψ(x)ε=−iℏ(−ℏ22mψ′′(x)+V(x)ψ(x)),\lim_{\varepsilon\to0^+}\frac{(U_\varepsilon\psi)(x)-\psi(x)}{\varepsilon}=-\frac{i}{\hbar}\Big(-\frac{\hbar^2}{2m}\psi''(x)+V(x)\psi(x)\Big),ε→0+lim​ε(Uε​ψ)(x)−ψ(x)​=−ℏi​(−2mℏ2​ψ′′(x)+V(x)ψ(x)),

that is, −ℏi∂tψ=12m(ℏi∂x)2ψ+Vψ-\frac{\hbar}{i}\partial_t\psi=\frac{1}{2m}\big(\frac{\hbar}{i}\partial_x\big)^2\psi+V\psi−iℏ​∂t​ψ=2m1​(iℏ​∂x​)2ψ+Vψ for the path-integral evolution, which is Schrödinger's equation (30). This is the content of Feynman's statement that (18), valid to first order in ε\varepsilonε, yields (30).

Milestones

  1. Eq. (26), the three regularized Fresnel integrals: M0(δ)→AM_0(\delta)\to AM0​(δ)→A, M1(δ)=0M_1(\delta)=0M1​(δ)=0, M2(δ)→ℏεimAM_2(\delta)\to\frac{\hbar\varepsilon i}{m}AM2​(δ)→mℏεi​A.
  2. Eqs. (27)–(28), zero-order agreement: (Uεψ)(x)→ψ(x)(U_\varepsilon\psi)(x)\to\psi(x)(Uε​ψ)(x)→ψ(x); this is the condition that fixes AAA.
  3. Eq. (27) for the free particle: ((Uεψ)(x)−ψ(x))/ε→ℏi2mψ′′(x)\big((U_\varepsilon\psi)(x)-\psi(x)\big)/\varepsilon\to\frac{\hbar i}{2m}\psi''(x)((Uε​ψ)(x)−ψ(x))/ε→2mℏi​ψ′′(x) when V=0V=0V=0.
  4. Footnote 15: for the free particle (18) is exact, UεUδψ=Uε+δψU_\varepsilon U_\delta\psi=U_{\varepsilon+\delta}\psiUε​Uδ​ψ=Uε+δ​ψ.

Significance

The goal is the step that connects the path-integral postulates to the ordinary formulation: without it the formulation of Sections 3–5 is not known to reproduce any quantum mechanics. The Fresnel integrals of (26) and the short-time kernel appear throughout semiclassical analysis and in every derivation of path integrals from the Schrödinger equation.

The physics result is classical and its rigorous versions are known (via the Trotter product formula or oscillatory-integral estimates). The work here is the formalization: Mathlib has the complex Gaussian integral and Schwartz functions, but not Fresnel integrals, the free Schrödinger kernel, or the short-time asymptotics of oscillatory integrals. None of the targets is currently formalized on the platform.

Difficulty

Feynman's derivation expands ψ(x−ξ)\psi(x-\xi)ψ(x−ξ) in a Taylor series under the integral and integrates term by term against exp⁡(imξ2/2ℏε)\exp(im\xi^2/2\hbar\varepsilon)exp(imξ2/2ℏε). Those integrals are not absolutely convergent, and the higher moments do not even exist as improper Riemann integrals, so the term-by-term step is not justified as written. A proof has to control the Taylor remainder against an oscillatory kernel whose width is of order ℏε/m\sqrt{\hbar\varepsilon/m}ℏε/m​, uniformly as ε→0+\varepsilon\to0^+ε→0+, with a prefactor 1/A1/A1/A that blows up like ε−1/2\varepsilon^{-1/2}ε−1/2. The naive dominated-convergence argument does not apply, because the kernel has modulus ∣A∣−1|A|^{-1}∣A∣−1 everywhere and does not concentrate in absolute value.

Formalization scope

  • One space dimension, real potential VVV with no regularity assumptions (it enters only through V(x)V(x)V(x) at the fixed point, as in Eq. (23)).
  • Wave functions are Schwartz functions 𝓢(ℝ, ℂ), which formalizes the paper's "relatively smooth" ψ\psiψ that "falls off sufficiently for large xxx". For such ψ\psiψ the integral defining UεψU_\varepsilon\psiUε​ψ is absolutely convergent, so the Lebesgue (Bochner) integral is used.
  • ℏ>0\hbar>0ℏ>0, m>0m>0m>0 are hypotheses; limits in ε\varepsilonε and δ\deltaδ are one-sided, →0+\to0^+→0+.
  • AAA uses Mathlib's principal complex power z1/2z^{1/2}z1/2.
  • The Gaussian moments are regularized as in footnote 13 (ℏ→ℏ(1−iδ)\hbar\to\hbar(1-i\delta)ℏ→ℏ(1−iδ)), because the bare integrals are not Lebesgue integrable and the Bochner integral would silently return 000.
  • The goal is pointwise in xxx and concerns the generator of one step; it does not assert convergence of the full time-sliced path integral (a Trotter-type statement), which would be a natural follow-up mission.

Useful infrastructure: Fresnel integrals, Fourier representation of the free Schrödinger kernel on Schwartz space, and differentiation of oscillatory integrals with a parameter. All are reusable beyond this mission.

Selected references

  • R. P. Feynman, Space-Time Approach to Non-Relativistic Quantum Mechanics, Rev. Mod. Phys. 20, 367 (1948). https://doi.org/10.1103/RevModPhys.20.367
  • P. A. M. Dirac, On the Analogy Between Classical and Quantum Mechanics, Rev. Mod. Phys. 17, 195 (1945). https://doi.org/10.1103/RevModPhys.17.195
  • M. Kac, On distributions of certain Wiener functionals, Trans. Amer. Math. Soc. 65, 1 (1949).
  • E. Nelson, Feynman integrals and the Schrödinger equation, J. Math. Phys. 5, 332 (1964).
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Mathematical Physics·Captain: Lucas

Gambini–Pullin 2014, Appendix A: nonlocal weights make the Lorentz-violating model integral smallResearch Paper

Motivation

Gambini and Pullin (IJMPD 23 (2014) 1442023) study quantum fields living on the discrete quantum spacetimes of spherically symmetric loop quantum gravity. Discreteness makes the field equations lattice-like and hence breaks Lorentz invariance. Collins, Perez, Sudarsky, Urrutia and Vucetich (PRL 93 (2004) 191301) argued that in interacting theories such Planck-scale violations feed, through renormalized loop diagrams, into large low-energy violations: a difference of second derivatives of the self-energy that should vanish by Lorentz invariance stays bounded away from zero. Gambini and Pullin argue that two exponential weights — a Gaussian fuzziness factor from the spread of the ADM mass, and a Lorentz-invariant nonlocal interaction factor of the type found in string field theory — make this quantity arbitrarily small.

Because the full self-energy calculation is lengthy, the paper's Appendix A replaces it by a two-dimensional model integral in which rotations play the role of Lorentz transformations and a parameter σ\sigmaσ plays the role of lattice spacing. This mission formalizes the precise mathematical claims made about that model.

Setting

For real parameters σ≥0\sigma \ge 0σ≥0 define the denominator base and the model integrand

Dσ(x,y)=1+x2+y21+σy2,fσ(x,y)=x2−y2Dσ(x,y)2.D_\sigma(x,y) = 1 + x^2 + \frac{y^2}{1+\sigma y^2}, \qquad f_\sigma(x,y) = \frac{x^2-y^2}{D_\sigma(x,y)^2}.Dσ​(x,y)=1+x2+1+σy2y2​,fσ​(x,y)=Dσ​(x,y)2x2−y2​.

The paper's integral (A.1) is I=∫R2fσ(x,y) dx dyI = \int_{\mathbb R^2} f_\sigma(x,y)\,dx\,dyI=∫R2​fσ​(x,y)dxdy. For σ=0\sigma = 0σ=0 one has D0=1+x2+y2D_0 = 1 + x^2 + y^2D0​=1+x2+y2, which is rotation invariant.

(A.1) is only a formal expression: fσf_\sigmafσ​ is not Lebesgue integrable on R2\mathbb R^2R2 (for σ=0\sigma = 0σ=0 it decays like r−2r^{-2}r−2; for σ>0\sigma > 0σ>0 it grows like −y2-y^2−y2 along the yyy-axis). The mission therefore uses the disk-truncated integral

Iσdisk(R)=∫x2+y2≤R2fσ(x,y) dx dy,I^{\mathrm{disk}}_\sigma(R) = \int_{x^2+y^2 \le R^2} f_\sigma(x,y)\,dx\,dy,Iσdisk​(R)=∫x2+y2≤R2​fσ​(x,y)dxdy,

which regularizes (A.1) in a rotation-invariant way.

The weighted model integral (A.2) is, for weights α,β\alpha, \betaα,β,

I(α,β,σ)=∫R2e−αx2 e−β(x2+y2) fσ(x,y) dx dy.I(\alpha,\beta,\sigma) = \int_{\mathbb R^2} e^{-\alpha x^2}\, e^{-\beta(x^2+y^2)}\, f_\sigma(x,y)\,dx\,dy .I(α,β,σ)=∫R2​e−αx2e−β(x2+y2)fσ​(x,y)dxdy.

The first factor models the fuzziness (it acts on one direction only), and the second models the nonlocal interaction (rotation invariant here, Lorentz invariant in the physical case).

Formalization targets

Goal (Appendix A, sentence after (A.2))

"With suitable choices of α\alphaα and β\betaβ one can make the integral as small as desired":

∀σ>0, ∀ε>0, ∃α>0, ∃β>0:∣I(α,β,σ)∣<ε.\forall \sigma > 0,\ \forall \varepsilon > 0,\ \exists \alpha > 0,\ \exists \beta > 0:\quad |I(\alpha,\beta,\sigma)| < \varepsilon .∀σ>0, ∀ε>0, ∃α>0, ∃β>0:∣I(α,β,σ)∣<ε.

Milestones

  1. For σ=0\sigma = 0σ=0 the integral vanishes: I0disk(R)=0I^{\mathrm{disk}}_0(R) = 0I0disk​(R)=0 for every RRR.
  2. For σ>0\sigma > 0σ>0 it "does not vanish by a significant amount": Iσdisk(R)→−∞I^{\mathrm{disk}}_\sigma(R) \to -\inftyIσdisk​(R)→−∞ as R→∞R \to \inftyR→∞.
  3. (A.2) is well defined: the weighted integrand is integrable for α≥0\alpha \ge 0α≥0, β>0\beta > 0β>0, σ≥0\sigma \ge 0σ≥0.
  4. With only the rotation-invariant weight and σ=0\sigma = 0σ=0, (A.2) still vanishes: I(0,β,0)=0I(0,\beta,0) = 0I(0,β,0)=0 for β>0\beta > 0β>0.
  5. In the regime α∼β\alpha \sim \betaα∼β large: I(β,β,σ)→0I(\beta,\beta,\sigma) \to 0I(β,β,σ)→0 as β→∞\beta \to \inftyβ→∞, for each σ>0\sigma > 0σ>0.

Significance

In the paper this model is the only precisely stated mathematical content backing the claim that the two exponential weights restore approximate Lorentz invariance. Formalizing it pins down exactly which statements hold (and in what sense the formal integral (A.1) "vanishes" or "does not vanish"), separating the rigorous content of the toy model from the physical argument it illustrates. The results are elementary real analysis; no machine-checked proofs of them are known to exist.

Difficulty

The main difficulty is that the unweighted integral (A.1) diverges, so both "vanishes" and "does not vanish" need a regularization. The weighted statements need integrability and dominated-convergence estimates on R2\mathbb R^2R2 and a change of variables (swapping xxx and yyy) for the symmetry claims. The divergence to −∞-\infty−∞ in milestone 2 needs separate upper and lower estimates for the positive and negative parts of fσf_\sigmafσ​ on growing disks.

Formalization scope

All objects are real-valued functions on R×R\mathbb R \times \mathbb RR×R with Lebesgue (product) measure. I(α,β,σ)I(\alpha,\beta,\sigma)I(α,β,σ) is a Bochner integral over the whole plane; where the integrand is not integrable, the Lean integral is 000 by convention, which is why milestone 3 is included and all weighted statements assume β>0\beta > 0β>0. The disk is the closed Euclidean disk {x2+y2≤R2}\{x^2+y^2 \le R^2\}{x2+y2≤R2}, not a sup-norm ball. The parameter σ\sigmaσ is restricted to σ≥0\sigma \ge 0σ≥0 (or σ>0\sigma > 0σ>0) wherever it matters, so that 1+σy2>01+\sigma y^2 > 01+σy2>0. The sentence in the paper "more precisely one needs α∼β\alpha \sim \betaα∼β and both larger than σ\sigmaσ" is heuristic; only its sufficiency direction along α=β\alpha = \betaα=β is formalized (milestone 5). No necessity claim is formalized, because a large β\betaβ alone already makes III small.

Selected references

  • R. Gambini, J. Pullin, Emergence of stringlike physics from Lorentz invariance in loop quantum gravity, Int. J. Mod. Phys. D 23 (2014) 1442023. https://doi.org/10.1142/S0218271814420231
  • J. Collins, A. Perez, D. Sudarsky, L. Urrutia, H. Vucetich, Lorentz invariance and quantum gravity: an additional fine-tuning problem?, Phys. Rev. Lett. 93 (2004) 191301. https://doi.org/10.1103/PhysRevLett.93.191301
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Theoretical Computer Science·Captain: marwahaha

Average sensitivity of polynomial threshold functionsOpen Problem

Motivation

Average sensitivity measures how often a Boolean decision changes after one coordinate flip. For polynomial threshold rules, a degree-sensitive estimate limits the total influence of all coordinates. The source manuscript presents the surrounding research claim.

Setting

A polynomial threshold function evaluates a real multilinear polynomial p on the uniform cube {−1,1}ⁿ, then applies sign with sign(0)=1. Average sensitivity is the sum, over coordinates, of the fraction of cube vertices whose output changes under that flip.

Formalization target

For n≥1 and 1≤d≤n, prove

AS⁡(sign⁡p)≤8dn\operatorname{AS}(\operatorname{sign}p)\le8d\sqrt nAS(signp)≤8dn​

for every multilinear p of total degree at most d.

The selected formal target is OAI.LeanBlast.GotsmanLinial.gotsmanLinialStatement.

Significance and status

The constant is uniform in both dimension and degree. The formal target is the asymptotic Gotsman–Linial estimate with its explicit coefficient eight. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

A separate estimate for fixed degree would not establish the bound uniformly as d varies with n. Zeros of p on the cube must respect the specified tie convention.

Formalization scope

The cube is Fin n→Bool and coordinates are converted to ±1. Multilinearity is a support predicate on Mathlib multivariate polynomials, and the degree condition is explicit. General polynomial reduction to multilinear form is not an additional attached theorem.

Selected references

  • OpenAI, Average sensitivity of polynomial threshold functions, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Discrete Geometry·Captain: marwahaha

Finite cylinder approximation of ruled setsOpen Problem

Motivation

A continuously varying family of line segments suggests a low-cost cylinder cover, but a finite approximation must control both gaps and accumulated base area. The source manuscript presents the surrounding research claim.

Setting

A ruled set consists of segments (s,p+sv(p)) with p in a compact planar label set D and |s|≤L. The basic weighted projection cost is ∫_D(1+|v(p)|²)^(-1/2)dp. The source also defines physical rescalings, square intercept tiles and singular slope fields.

Formalization target

Prove the published FullMain conjunction. Its central finite-approximation clause gives

∑i∣Bi∣≤∫Ddp1+∣v(p)∣2+ε\sum_i |B_i|\le\int_D\frac{dp}{\sqrt{1+|v(p)|^2}}+\varepsiloni∑​∣Bi​∣≤∫D​1+∣v(p)∣2​dp​+ε

for every ε>0 under its C¹ hyperbolicity hypotheses. The package additionally contains physical-rescaling, logarithmic, product-cell, orthogonal-grid, smooth nilpotent and singular-tetrahedron assertions.

The selected formal target is OAI.RuledApproximation.fullMain.

Significance and status

The chosen goal supplies a package of finite-cover results with explicit regularity and base-shape requirements. The broad fourPaperMain reference also contains a C¹ nilpotent variant. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

Freezing directions can create gaps and a persistent area loss. The final family must be finite and cover every point while the area error is arbitrarily small.

Formalization scope

FullMain uses Euclidean planes and three-space. Some clauses require null-measure boundary or C² regularity; its NilpotentStatement requires smoothness and a square-zero derivative. The singular clause includes its stated p,γ ranges and strict tetrahedron cost below √2/2. These are the selected published clauses; the manuscript’s latest C¹ formulation is not silently substituted for them. Independent definition groups remain separate references.

Selected references

  • OpenAI, Finite cylinder approximation of ruled sets, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Combinatorics·Captain: marwahaha

The dyadic case of the Erdős similarity conjectureOpen Problem

Motivation

Finite patterns fit inside positive-measure sets after a sufficiently small affine change. The dyadic similarity problem asks whether one particular infinite pattern can be excluded even from compact sets of nearly full measure. The source manuscript presents the surrounding research claim.

Setting

The dyadic sequence is D={2⁻ⁿ:n≥1}. Its affine copies are x+sD with arbitrary x∈ℝ and nonzero signed scale s. The ambient measure is Lebesgue measure on the real line.

Formalization target

For every 0<η<1, construct a compact E⊆[0,1] with

∣E∣>1−η,∀x∈R  ∀s≠0  ∃n≥1,x+s2−n∉E.|E|>1-\eta,\qquad\forall x\in\mathbb R\;\forall s\ne0\;\exists n\ge1,\quad x+s2^{-n}\notin E.∣E∣>1−η,∀x∈R∀s=0∃n≥1,x+s2−n∈/E.

The same E must avoid every translation and both signs of dilation.

The selected formal target is OAI.Problem310.dyadic_affine_avoidance.

Significance and status

The result concerns the dyadic sequence specifically, with a stronger near-full-measure conclusion than merely finding one positive-measure avoiding set. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

Excluding a countable collection of copies does not handle the continuum of scales and centers. Finite initial segments cannot replace the entire sequence.

Formalization scope

The definition dyadicPoint accepts n=0, but the theorem explicitly chooses n≥1. Measure is ENNReal-valued and compares with ENNReal.ofReal(1−η). Compactness and interval containment are required conclusions. General infinite sets are outside this selected target.

Selected references

  • OpenAI, The dyadic case of the Erdős similarity conjecture, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Combinatorics·Captain: marwahaha

Asymptotically minimal maxima of real Littlewood polynomialsOpen Problem

Motivation

Choosing real signs in a polynomial controls how much its values can peak around the unit circle. The target seeks asymptotically optimal maximum modulus at every sufficiently large length. The source manuscript presents the surrounding research claim.

Setting

A real Littlewood polynomial has consecutive coefficients εₖ∈{−1,1}: P_N(z)=Σₖ₌₀ᴺ⁻¹ εₖzᵏ. The coefficient family may depend on both its length and the requested accuracy.

Formalization target

Prove

∀η>0  ∃N0≥1  ∀N≥N0  ∃ε,sup⁡∣z∣=1∣PN(z)∣≤(1+η)N.\forall\eta>0\;\exists N_0\ge1\;\forall N\ge N_0\;\exists\varepsilon,\quad\sup_{|z|=1}|P_N(z)|\le(1+\eta)\sqrt N.∀η>0∃N0​≥1∀N≥N0​∃ε,∣z∣=1sup​∣PN​(z)∣≤(1+η)N​.

All sufficiently large integer lengths are required, rather than a subsequence.

The selected formal target is OAI.AsymptoticallyMinimalLittlewood.main.

Significance and status

The selected target is the uniform maximum-modulus assertion. The companion finite-flatness target gives one sign family whose normalized modulus tends to one in every positive finite Lᵖ moment. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

Control at finitely many sample points does not directly give a bound on the full circle. Uniformity in the circle variable and coverage of all large lengths are separate obligations.

Formalization scope

Coefficients are real-valued Fin N functions explicitly constrained to ±1 and evaluated as complex polynomials. The companion theorem uses Haar probability on UnitAddCircle and a single family for every p>0. Both independent definition groups are referenced; finite-flatness is a related endpoint rather than a claimed prerequisite.

Selected references

  • OpenAI, Asymptotically minimal maxima of real Littlewood polynomials, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Captain: marwahaha

A strict inverse-first-power bound for univalent functionsOpen Problem

Motivation

Integral-means spectra record the worst derivative concentration among normalized conformal maps. A strict bound at exponent −1 tests a specific predicted value of that spectrum. The source manuscript presents the surrounding research claim.

Setting

For a normalized univalent disk map f, M(−1,f,r) is the average of |f′|⁻¹ on the circle of radius r. The bounded spectrum B_b uses the extended-real limsup growth exponent, then takes its supremum over maps with bounded image.

Formalization target

Prove that there exist real ε and C with 0<ε<1/4 such that

M(−1,f,r)≤C(1−r)−1/4+εM(-1,f,r)\le C(1-r)^{-1/4+\varepsilon}M(−1,f,r)≤C(1−r)−1/4+ε

for every normalized univalent f and 1/2≤r<1. Also prove B_b(−1)<1/4 and the failure of the defined Kraetzer prediction to equal B_b at every real exponent.

The selected formal target is OAI.StrictInverseFirstPower.main.

Significance and status

A strictly positive uniform ε is the content of the improvement. The target explicitly includes the spectrum consequence and the negation of the full predicted formula. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

An exponent arbitrarily close to 1/4 from above does not give a strict gap below 1/4. The same ε and C must precede the quantification over f and r.

Formalization scope

The circle estimate covers all normalized univalent maps, whereas the spectrum uses the bounded-image subclass. Complex derivatives, real interval integrals and EReal suprema are the supplied representations. The prediction is the specified piecewise quadratic/linear function.

Selected references

  • OpenAI, A strict inverse-first-power bound for univalent functions, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Captain: marwahaha

Brennan's conjecture and sharp inverse-square integral meansOpen Problem

Motivation

The size of the derivative of a conformal map can concentrate near a domain boundary. Brennan-type integrability and inverse-square integral means quantify how severe that concentration can be. The source manuscript presents the surrounding research claim.

Setting

A schlicht function is an injective holomorphic map f on the unit disk with f(0)=0 and f′(0)=1. M(f,t,r) is the circle average of |f′|ᵗ at radius r, and B(t) is the supremum of the associated extended-real boundary growth exponents.

Formalization target

Prove the four-part MainStatement, including

M(f,−2,r)≤Cε(1−r)−1−ε,B(−2)=1,M(f,-2,r)\le C_\varepsilon(1-r)^{-1-\varepsilon},\qquad B(-2)=1,M(f,−2,r)≤Cε​(1−r)−1−ε,B(−2)=1,

uniformly for schlicht f and 1/2 ≤ r < 1. For conformal bijections φ:W→𝔻 on the specified simply connected domains, prove area integrability of |φ′|ˢ for 4/3<s<4; for univalent disk maps prove integrability of |f′|ᵗ for −2<t<2/3.

The selected formal target is OAI.Brennan.main_theorem.

Significance and status

The goal packages the uniform circle bound, exact spectrum value and both area-integrability formulations. A separate endpoint target records sharp failure for the Koebe map and its inverse. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

A growth bound with a constant depending on f does not supply the stated uniform estimate. Boundary behavior must also support the precise open exponent intervals.

Formalization scope

Planar Lebesgue area, a left-hand limit r→1, and extended-real spectra are fixed. W must be open, connected, simply connected and have nontrivial spherical boundary. Main and sharp-endpoint definitions are independent published groups with repeated names, so references coexist without one aggregate import.

Selected references

  • OpenAI, Brennan's conjecture and sharp inverse-square integral means, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Partial Differential Equations·Captain: wurtle

The Subcritical Hénon–Lane–Emden ConjectureResearch Paper

Motivation: Liouville theorems for Lane–Emden systems

Liouville theorems say that certain nonlinear elliptic equations have no positive solutions on the whole space. Beyond their own interest, they are the key input in blow-up and rescaling arguments that give a priori bounds, existence results and singularity estimates for equations on bounded domains (Gidas–Spruck 1981; Polačik–Quittner–Souplet 2007). For the scalar equation −Δu=up-\Delta u=u^p−Δu=up, Gidas and Spruck proved nonexistence in the whole subcritical range. For the coupled Lane–Emden system −Δu=vp-\Delta u=v^p−Δu=vp, −Δv=uq-\Delta v=u^q−Δv=uq, the corresponding statement — no positive solutions below the critical hyperbola 1p+1+1q+1=n−2n\frac1{p+1}+\frac1{q+1}=\frac{n-2}{n}p+11​+q+11​=nn−2​ — is the Lane–Emden conjecture; before the source, it had been proved only in dimensions n≤4n\le4n≤4 and in partial ranges. The weighted Hénon–Lane–Emden version, with factors ∣x∣A|x|^A∣x∣A and ∣x∣B|x|^B∣x∣B, asks the same question for the weighted hyperbola.

Timeline

  • 1981 — Gidas and Spruck: scalar subcritical Liouville theorem and the blow-up method for a priori bounds (CPAM 1981; CPDE 1981).
  • 1993, 1996 — Mitidieri: a Rellich-type identity for systems and early nonexistence regions (CPDE 1993; DIE 1996).
  • 1996 — Serrin and Zou: the unweighted conjecture for n=3n=3n=3 under a growth condition (DIE 1996).
  • 2007 — Polačik, Quittner and Souplet remove the growth condition for n=3n=3n=3 (Duke 2007).
  • 2009 — Souplet proves the Lane–Emden conjecture for n=4n=4n=4 (Adv. Math. 2009); Chen and Li use integral systems and moving planes under integrability hypotheses (DCDS 2009).
  • 2010 — Bidaut-Véron and Giacomini identify the critical weighted hyperbola in the radial theory and prove radial existence on and above it (ADE 2010).
  • 2012 — Phan formulates the weighted question for A,B>−2A,B>-2A,B>−2 (Conjecture C) and proves bounded, low-dimensional and conditional cases (ADE 2012).
  • 2014 — Fazly and Ghoussoub: bounded and stable cases for nonnegative weights (DCDS 2014).
  • 2019 — Li and Zhang prove the Hénon–Lane–Emden conjecture in R3\mathbb R^3R3 (JDE 2019); Cheng and Huang give an energy-estimate criterion for the unweighted conjecture (DCDS 2019).
  • 2022 — H. Li: restricted exponent ranges in dimensions four and five (Adv. Nonlinear Stud. 2022).
  • 2025–2026 — K. Li, M. Li and Wei: a new unweighted region for p,q≥1p,q\ge1p,q≥1 when n≥5n\ge5n≥5 (preprint, 2025). Huang and Zou state the all-real-weight, origin-continuous assertion as Conjecture B (J. London Math. Soc. 2026). Xu and Luo treat radial higher-order systems (JDE 2026).
  • 2026 — An OpenAI preprint, The Subcritical Hénon–Lane–Emden Conjecture (OpenAI Math Release, September 24, 2026), claims the full subcritical nonexistence theorem for every n≥2n\ge2n≥2 and all real weights. It has not been peer reviewed, and the claim has not been formally verified.

Setting

Fix an integer n≥2n\ge2n≥2, exponents p,q>0p,q>0p,q>0 and real weights A,BA,BA,B. The Hénon–Lane–Emden system is

−Δu=∣x∣A vp,−Δv=∣x∣B uqin Rn∖{0},-\Delta u=|x|^A\,v^p,\qquad -\Delta v=|x|^B\,u^q\qquad\text{in }\mathbb R^n\setminus\{0\},−Δu=∣x∣Avp,−Δv=∣x∣Buqin Rn∖{0},

where Δ=∑i∂i2\Delta=\sum_i\partial_i^2Δ=∑i​∂i2​ is the Laplacian. A solution in the sense of the source is a pair u,v∈C2(Rn∖{0})∩C(Rn)u,v\in C^2(\mathbb R^n\setminus\{0\})\cap C(\mathbb R^n)u,v∈C2(Rn∖{0})∩C(Rn) with u(x)>0u(x)>0u(x)>0 and v(x)>0v(x)>0v(x)>0 for every x∈Rnx\in\mathbb R^nx∈Rn, including the origin, satisfying both equations at every x≠0x\neq0x=0. The exponents are subcritical if

n+Ap+1+n+Bq+1>n−2.\frac{n+A}{p+1}+\frac{n+B}{q+1}>n-2 .p+1n+A​+q+1n+B​>n−2.

In Lean, Space n = EuclideanSpace ℝ (Fin n), IsSolution n p q A B u v packages continuity, ContDiffOn ℝ 2 off the origin, strict positivity everywhere and the two equations with Mathlib's Laplacian and real powers, and Subcritical is the displayed inequality.

Formalization targets

Goal: subcritical nonexistence (Theorem 1.1)

n≥2, p,q>0, A,B∈R, n+Ap+1+n+Bq+1>n−2 ⟹ ∄ (u,v) solving the system as above.n\ge2,\ p,q>0,\ A,B\in\mathbb R,\ \frac{n+A}{p+1}+\frac{n+B}{q+1}>n-2\ \Longrightarrow\ \nexists\,(u,v)\ \text{solving the system as above}.n≥2, p,q>0, A,B∈R, p+1n+A​+q+1n+B​>n−2 ⟹ ∄(u,v) solving the system as above.

This is exactly Theorem 1.1 of the source. Taking A=B=0A=B=0A=B=0 gives the unweighted Lane–Emden conjecture (Corollary 1.2) for n≥3n\ge3n≥3. The goal is published on the platform with status Open: no machine-checked proof exists yet.

Significance

The result itself. If the source's proof is correct, the theorem gives a positive answer to Huang and Zou's Conjecture B and, with A=B=0A=B=0A=B=0, to the Lane–Emden conjecture in every dimension. It needs no radial symmetry, boundedness, integrability, finite energy, stability or growth condition at infinity. Combined with the radial existence theorem of Bidaut-Véron and Giacomini, it also settles Phan's Conjecture C for n≥3n\ge3n≥3 and A,B>−2A,B>-2A,B>−2, including existence on the critical hyperbola (Corollary 6.2). Through the blow-up method, Liouville theorems of this type give a priori bounds and singularity and decay estimates for Lane–Emden-type systems on bounded domains.

Formalizing it. The statement is elementary: classical derivatives, the Euclidean Laplacian and real powers. The proof uses potential estimates, a localized virial (Rellich–Pohozaev type) identity, a geometric interval inequality and a dilation argument. All of these are within reach of Mathlib's analysis library, which makes the theorem a realistic test of large-scale PDE formalization.

Difficulty

The weighted statement does not follow from the unweighted one at the same exponents. For example, n=5n=5n=5, p=q=4p=q=4p=q=4, A=B=3A=B=3A=B=3 is weighted-subcritical, while 1p+1+1q+1=25<35\frac1{p+1}+\frac1{q+1}=\frac25<\frac35p+11​+q+11​=52​<53​ is unweighted-supercritical. Weighted subcriticality also does not give the unweighted input in Phan's transfer argument. Translations do not preserve the weighted equation, so moving-plane and translation-based compactness arguments are unavailable. The level sets {∣x∣Buq>t}\{|x|^Bu^q>t\}{∣x∣Buq>t} have endpoint values that vary with ∣x∣|x|∣x∣, which breaks the unweighted interval comparison. Finally, since no energy, decay or stability bound is assumed, the localized energy has to be bounded from the subcritical gap alone.

Formalization scope

  • The domain is EuclideanSpace ℝ (Fin n) with n≥2n\ge2n≥2, and p,q,A,Bp,q,A,Bp,q,A,B are real with p,q>0p,q>0p,q>0. Weights are Real.rpow ‖x‖ A, used only at x≠0x\neq0x=0, so the junk value of rpow at 000 never enters. The nonlinearities Real.rpow (v x) p are evaluated at strictly positive arguments.
  • Regularity is Continuous on all of Rn\mathbb R^nRn and ContDiffOn ℝ 2 on {0}c\{0\}^c{0}c. Positivity is required at every point, including the origin, as in the source; differentiability at the origin is not assumed.
  • The conclusion is the nonexistence of any such pair. Every hypothesis is satisfiable (supercritical solutions exist), so the statement is not trivialized.
  • Infrastructure needed: Newtonian potentials and distributional extension across a point, Rellich–Pohozaev identities, polar integration and dilation arguments. These pieces would serve other Liouville-type theorems.

Selected references

  • B. Gidas and J. Spruck, Global and local behavior of positive solutions of nonlinear elliptic equations, Comm. Pure Appl. Math. 34 (1981), 525–598. https://doi.org/10.1002/cpa.3160340406
  • B. Gidas and J. Spruck, A priori bounds for positive solutions of nonlinear elliptic equations, Comm. PDE 6 (1981), 883–901. https://doi.org/10.1080/03605308108820196
  • E. Mitidieri, A Rellich type identity and applications, Comm. PDE 18 (1993), 125–151. https://doi.org/10.1080/03605309308820923
  • E. Mitidieri, Nonexistence of positive solutions of semilinear elliptic systems in RN\mathbb R^NRN, Differential Integral Equations 9 (1996), 465–479. https://doi.org/10.57262/die/1367969966
  • J. Serrin and H. Zou, Non-existence of positive solutions of Lane–Emden systems, Differential Integral Equations 9 (1996), 635–653. https://doi.org/10.57262/die/1367969879
  • P. Polačik, P. Quittner and P. Souplet, Duke Math. J. 139 (2007), 555–579. https://doi.org/10.1215/S0012-7094-07-13935-8
  • P. Souplet, The proof of the Lane–Emden conjecture in four space dimensions, Adv. Math. 221 (2009), 1409–1427. https://doi.org/10.1016/j.aim.2009.02.014
  • W. Chen and C. Li, An integral system and the Lane–Emden conjecture, Discrete Contin. Dyn. Syst. 24 (2009), 1167–1184. https://doi.org/10.3934/dcds.2009.24.1167
  • M.-F. Bidaut-Véron and H. Giacomini, A new dynamical approach of Emden–Fowler equations and systems, Adv. Differential Equations 15 (2010), 1033–1082. https://doi.org/10.57262/ade/1355854434
  • Q. H. Phan, Adv. Differential Equations 17 (2012), 605–634. https://doi.org/10.57262/ade/1355702970
  • M. Fazly and N. Ghoussoub, On the Hénon–Lane–Emden conjecture, Discrete Contin. Dyn. Syst. 34 (2014), 2513–2533. https://doi.org/10.3934/dcds.2014.34.2513
  • K. Li and Z. Zhang, Proof of the Hénon–Lane–Emden conjecture in R3\mathbb R^3R3, J. Differential Equations 266 (2019), 202–226. https://doi.org/10.1016/j.jde.2018.07.036
  • Z. Cheng and G. Huang, A Liouville theorem for the subcritical Lane–Emden system, Discrete Contin. Dyn. Syst. 39 (2019), 1359–1377. https://doi.org/10.3934/dcds.2019058
  • H. Li, Adv. Nonlinear Stud. 22 (2022), 517–533. https://doi.org/10.1515/ans-2022-0027
  • L.-H. Huang and W. Zou, J. London Math. Soc. 113 (2026), e70412. https://doi.org/10.1112/jlms.70412
  • Y. Xu and H. Luo, Liouville type theorems for higher order elliptic systems, J. Differential Equations 453 (2026), 113823. https://doi.org/10.1016/j.jde.2025.113823
  • OpenAI, The Subcritical Hénon–Lane–Emden Conjecture, OpenAI Math Release preprint, September 24, 2026 (Theorem 1.1, p. 2). https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/The-Subcritical-Henon-Lane-Emden-Conjecture-September-24-2026/paper.pdf
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Functional Analysis·Captain: wurtle

Exact asymptotic moduli in a Daugavet subspace of L1Research Paper

Motivation

A norm is uniformly convex when midpoints of far-apart unit vectors are pushed strictly inside the unit ball. In infinite-dimensional Banach spaces the useful notions are asymptotic: one asks for a gain only in directions taken from a subspace of finite codimension, chosen after the center is fixed. Two such notions are compared here. Asymptotic uniform convexity (AUC) asks for growth of ∥x+ty∥\|x+ty\|∥x+ty∥ in every far-out unit direction yyy; asymptotic midpoint uniform convexity (AMUC) asks only that the average of ∥x+ty∥\|x+ty\|∥x+ty∥ and ∥x−ty∥\|x-ty\|∥x−ty∥ grows. These properties control nonlinear embeddings (for instance of countably branching diamond graphs) and are standard tools in the asymptotic geometry of Banach spaces.

Dilworth, Kutzarova, Randrianarivony, Revalski and Zhivkov (2016) asked whether AMUC and AUC are equivalent up to renorming. Baudier (2026) answered no, using subspaces of L1L^1L1 whose unit ball is compact in measure and the Daugavet-property example of Kadets and Werner. This mission asks for the exact values of both moduli in that setting.

Timeline

  • 1980. Bourgain and Rosenthal construct a subspace of L1L^1L1 whose unit ball is relatively compact in measure but which fails the Radon–Nikodym property (doi:10.1007/BF02762868).
  • 1983. Brézis and Lieb prove their splitting identity for pointwise convergent sequences in LpL^pLp (doi:10.1090/S0002-9939-1983-0699419-3).
  • 2000. Kadets, Shvidkoy, Sirotkin and Werner give the slice characterization of the Daugavet property (arXiv:math/9709216); Shvydkoy gives its weak-open form (doi:10.1006/jfan.2000.3626).
  • 2004. Kadets and Werner refine the Bourgain–Rosenthal construction to obtain a space with the Schur and Daugavet properties (doi:10.1090/S0002-9939-03-07278-2).
  • 2016. Dilworth et al. introduce AMUC and ask whether it is equivalent to AUC up to renorming (doi:10.1016/j.jmaa.2015.11.061).
  • 2026. Baudier proves AMUC for measure-compact subspaces of L1L^1L1 and deduces a negative answer via the Kadets–Werner space (arXiv:2609.21283).

The source of this mission is an OpenAI preprint dated September 27, 2026, which computes both moduli exactly.

Setting

All spaces are real. For a Banach space XXX with norm NNN, let cof⁡(X)\operatorname{cof}(X)cof(X) be its closed linear subspaces of finite codimension. For N(x)=1N(x)=1N(x)=1 and t>0t>0t>0,

HN(x,t)=sup⁡F∈cof⁡(X) inf⁡y∈FN(y)≥1(N(x+ty)+N(x−ty)2−1),DN(x,t)=sup⁡F∈cof⁡(X) inf⁡y∈FN(y)=1(N(x+ty)−1).H_N(x,t)=\sup_{F\in\operatorname{cof}(X)}\ \inf_{\substack{y\in F\\ N(y)\ge1}}\Bigl(\frac{N(x+ty)+N(x-ty)}2-1\Bigr),\qquad D_N(x,t)=\sup_{F\in\operatorname{cof}(X)}\ \inf_{\substack{y\in F\\ N(y)=1}}\bigl(N(x+ty)-1\bigr).HN​(x,t)=F∈cof(X)sup​ y∈FN(y)≥1​inf​(2N(x+ty)+N(x−ty)​−1),DN​(x,t)=F∈cof(X)sup​ y∈FN(y)=1​inf​(N(x+ty)−1).

The averaged midpoint modulus δ^N(t)\widehat\delta_N(t)δN​(t) and the one-sided modulus δ‾N(t)\overline\delta_N(t)δN​(t) are the infima of HN(x,t)H_N(x,t)HN​(x,t) and DN(x,t)D_N(x,t)DN​(x,t) over unit xxx. NNN is AUC if δ‾N(t)>0\overline\delta_N(t)>0δN​(t)>0 for all t>0t>0t>0. A norm NNN is equivalent to ∥⋅∥\|\cdot\|∥⋅∥ if a∥x∥≤N(x)≤b∥x∥a\|x\|\le N(x)\le b\|x\|a∥x∥≤N(x)≤b∥x∥ with a,b>0a,b>0a,b>0.

A space has the Daugavet property if ∥I+T∥=1+∥T∥\|I+T\|=1+\|T\|∥I+T∥=1+∥T∥ for every rank-one bounded operator TTT. On a probability space (Ω,P)(\Omega,\mathbb P)(Ω,P), convergence in measure is given by the metric

d(f,g)=inf⁡{a>0: P(∣f−g∣>a)<a}.d(f,g)=\inf\{a>0:\ \mathbb P(|f-g|>a)<a\}.d(f,g)=inf{a>0: P(∣f−g∣>a)<a}.

A set is totally bounded in measure if for each ε>0\varepsilon>0ε>0 it is covered by finitely many ddd-balls of radius ε\varepsilonε.

Formalization targets

Goal: Theorem 1.1

Let EEE be an infinite-dimensional closed subspace of L1(Ω,P)L^1(\Omega,\mathbb P)L1(Ω,P), P\mathbb PP a probability measure, whose unit ball is totally bounded in measure and whose norm has the Daugavet property. Then for every unit x∈Ex\in Ex∈E and t>0t>0t>0

HE(x,t)=max⁡{t/2, t−1},DE(x,t)=max⁡{0, t−2},H_E(x,t)=\max\{t/2,\ t-1\},\qquad D_E(x,t)=\max\{0,\ t-2\},HE​(x,t)=max{t/2, t−1},DE​(x,t)=max{0, t−2},

so δ^E(t)=max⁡{t/2,t−1}\widehat\delta_E(t)=\max\{t/2,t-1\}δE​(t)=max{t/2,t−1} and δ‾E(t)=max⁡{0,t−2}\overline\delta_E(t)=\max\{0,t-2\}δE​(t)=max{0,t−2}, and EEE admits no equivalent AUC norm. Lean: OAI.ExactModuli.exact_main (open on the platform).

Milestone: Theorem 6.1 (Kadets–Werner construction)

On ([0,1]N,λN)([0,1]^{\mathbb N},\lambda^{\mathbb N})([0,1]N,λN) there is an infinite-dimensional closed subspace E⊆L1E\subseteq L^1E⊆L1 whose unit ball is totally bounded in measure and which has the Daugavet slice property. Lean: OAI.ExactModuli.kadets_werner_existence. The proposal also carries OAI.ExactModuli.exact_example, the combination of the two theorems for this space.

Significance

The formulas show how far apart the two moduli can be: the averaged modulus grows linearly from 000, while the one-sided modulus vanishes on the whole interval (0,2](0,2](0,2]. They refine Baudier's qualitative AMUC statement and linear lower bound into exact curves at every unit center, and the renorming clause shows that no equivalent norm can repair the one-sided modulus. Together with Theorem 6.1, they give a concrete space realizing the separation.

The results are proved in an OpenAI preprint; they have not been peer reviewed, and no machine-checked proof exists. The Daugavet slice characterization, Bourgain's lemma on slices and weak neighborhoods (Lemma 3.2), and the construction itself are reusable pieces of Banach space theory that a formalization would supply.

Difficulty

The lower bound for HEH_EHE​ must hold uniformly over all directions in some finite-codimensional subspace, while the hypothesis only says that the unit ball is compact in a weak metric. A compactness argument along subsequences (Baudier's route via Brézis–Lieb) gives positivity but not the exact constant. The upper bounds need directions in a prescribed finite-codimensional subspace that are almost at distance 222 from xxx; the Daugavet property supplies such vectors only in weak neighborhoods, and they must then be corrected into the subspace. The renorming clause must handle an arbitrary equivalent norm, for which neither formula is available.

Formalization scope

  • Cofinite F is a closed submodule with finite-dimensional quotient. H, D, averagedModulus, oneSidedModulus follow the displayed sup/inf order; H ranges over N(y)≥1N(y)\ge1N(y)≥1, D over N(y)=1N(y)=1N(y)=1.
  • EquivalentNorm N is a Seminorm with two-sided comparison constants a,b>0a,b>0a,b>0; AUC N is positivity of oneSidedModulus N t for every t>0t>0t>0.
  • Daugavet X quantifies over rank-one operators written as ell.smulRight v.
  • measureDistance is the metric ddd on Lp ℝ 1 μ; MeasurePrecompactBall μ E requires finite ε\varepsilonε-nets (centers in L1L^1L1) of the unit ball of EEE; μ is a probability measure.
  • kwMeasure is the product of Lebesgue measures on N→[0,1]\mathbb N\to[0,1]N→[0,1].
  • The moduli are real-valued sSup/sInf; for infinite-dimensional EEE the relevant sets are nonempty and bounded, so the junk values are not used.

A full development needs the Daugavet slice characterization (Lemma 3.1), Bourgain's lemma (Lemma 3.2), the weak-neighborhood diameter-two property (Lemma 3.3), L1L^1L1 truncation estimates, and the Kadets–Werner iteration (Lemmas 6.2–6.3). Formalizations of these lemmas are welcome.

Selected references

  • OpenAI, Exact asymptotic moduli in a Daugavet subspace of L1L^1L1, preprint, September 27, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Exact-asymptotic-moduli-in-a-Daugavet-subspace-of-L1-September-27-2026/manuscript.pdf
  • F. P. Baudier, The Kadets–Werner modification of Bourgain–Rosenthal space is asymptotically midpoint uniformly convex, preprint, 2026. https://arxiv.org/abs/2609.21283
  • S. J. Dilworth, D. Kutzarova, N. L. Randrianarivony, J. P. Revalski, N. V. Zhivkov, Lenses and asymptotic midpoint uniform convexity, J. Math. Anal. Appl., 2016. https://doi.org/10.1016/j.jmaa.2015.11.061
  • V. Kadets, D. Werner, A Banach space with the Schur and the Daugavet property, Proc. Amer. Math. Soc., 2004. https://doi.org/10.1090/S0002-9939-03-07278-2
  • J. Bourgain, H. P. Rosenthal, Martingales valued in certain subspaces of L1L^1L1, Israel J. Math., 1980. https://doi.org/10.1007/BF02762868
  • V. M. Kadets, R. V. Shvidkoy, G. G. Sirotkin, D. Werner, Banach spaces with the Daugavet property, Trans. Amer. Math. Soc., 2000. https://arxiv.org/abs/math/9709216
  • R. V. Shvydkoy, Geometric aspects of the Daugavet property, J. Funct. Anal., 2000. https://doi.org/10.1006/jfan.2000.3626
  • H. Brézis, E. Lieb, A relation between pointwise convergence of functions and convergence of functionals, Proc. Amer. Math. Soc., 1983. https://doi.org/10.1090/S0002-9939-1983-0699419-3
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Functional Analysis·Captain: wurtle

Midpoint lenses in segment spacesResearch Paper

Motivation

In a uniformly convex space, if xxx is nearly as long as RRR and both x+yx+yx+y and x−yx-yx−y have length at most RRR, then the displacement yyy must be short. The set of such displacements,

L(x,R)={y: ∥x+y∥≤R, ∥x−y∥≤R},\mathcal L(x,R)=\{y:\ \|x+y\|\le R,\ \|x-y\|\le R\},L(x,R)={y: ∥x+y∥≤R, ∥x−y∥≤R},

is a symmetric lens. In infinite dimensions the right question is asymptotic: is yyy short after discarding finitely many directions? Dilworth, Kutzarova, Randrianarivony, Revalski and Zhivkov (2016) characterized asymptotic midpoint uniform convexity (AMUC) through the measure of noncompactness of such lenses. AMUC is the property that, together with asymptotic uniform convexity (AUC), governs which countably branching graphs embed into a Banach space with bounded distortion.

This mission asks for an explicit lens estimate in two James-type tree spaces, with a bound depending only on the squared-radius deficit R2−∥x∥2R^2-\|x\|^2R2−∥x∥2 of the center and holding for every displacement simultaneously after one finite set of coordinates is removed.

Timeline

  • 1974. James introduces the square-sum norm over disjoint segments of a tree (doi:10.1090/S0002-9904-1974-13580-9).
  • 1985. Ghoussoub and Maurey study GδG_\deltaGδ​-embeddings in Hilbert space (doi:10.1016/0022-1236(85)90039-4); the coordinate predual B∞B_\inftyB∞​ used here is the Ghoussoub–Maurey–Schachermayer construction as presented by Banakh (2000).
  • 2001. Girardi proves AUC of the canonical predual and of the full dual of the binary James tree space (doi:10.4064/sm147-2-2).
  • 2016. Dilworth et al. introduce AMUC and characterize it by lenses (doi:10.1016/j.jmaa.2015.11.061).
  • 2017. Baudier, Causey, Dilworth, Kutzarova, Randrianarivony, Schlumprecht and Zhang show that an equivalent AMUC norm prevents uniform embeddings of countably branching diamonds (arXiv:1612.01984).
  • 2021. Perreau asks whether the canonical predual of the countably branching James tree space is AMUC (Question 6 of arXiv:2104.10494).
  • 2026. Baudier shows that AMUC does not imply AUC renormability, via the Kadets–Werner modification of the Bourgain–Rosenthal space (arXiv:2609.21283).

The source of this mission is an OpenAI preprint dated September 27, 2026.

Setting

All scalars are real.

Finite-height forest. For h≥1h\ge1h≥1 let Th=N≤hT_h=\mathbb N^{\le h}Th​=N≤h be the tree of words of length at most hhh, ordered by extension (the root is the empty word). The forest F\mathcal FF is the disjoint union of one copy {h}×Th\{h\}\times T_h{h}×Th​ for each h≥1h\ge1h≥1. Write a⪯ba\preceq ba⪯b if aaa is an ancestor of bbb in the same component. A segment is a nonempty interval [a,b]={v:a⪯v⪯b}[a,b]=\{v: a\preceq v\preceq b\}[a,b]={v:a⪯v⪯b}. For finitely supported uuu put u(S)=∑v∈Su(v)u(S)=\sum_{v\in S}u(v)u(S)=∑v∈S​u(v) and

ρ(u)=sup⁡{(∑i=1mu(Si)2)1/2: S1,…,Sm pairwise disjoint segments}.\rho(u)=\sup\Bigl\{\Bigl(\sum_{i=1}^m u(S_i)^2\Bigr)^{1/2}:\ S_1,\dots,S_m\ \text{pairwise disjoint segments}\Bigr\}.ρ(u)=sup{(i=1∑m​u(Si​)2)1/2: S1​,…,Sm​ pairwise disjoint segments}.

Let JJJ be the completion of (c00(F),ρ)(c_{00}(\mathcal F),\rho)(c00​(F),ρ) and X=J∗X=J^*X=J∗ with the dual norm. Coordinate evaluation gives functionals ev∗∈Xe_v^*\in Xev∗​∈X.

Infinite tree. Let T∞=N<ωT_\infty=\mathbb N^{<\omega}T∞​=N<ω (all finite words, root included), J∞J_\inftyJ∞​ the completion for the same norm, and B∞=span⁡‾{ev∗}⊂J∞∗B_\infty=\overline{\operatorname{span}}\{e_v^*\}\subset J_\infty^*B∞​=span​{ev∗​}⊂J∞∗​, closed in the dual norm.

A finite set HHH of vertices is ancestral if it contains all ancestors of its elements. On either space,

PHx=∑v∈Hx(ev) ev∗,QHx=x−PHx.P_Hx=\sum_{v\in H}x(e_v)\,e_v^*,\qquad Q_Hx=x-P_Hx.PH​x=v∈H∑​x(ev​)ev∗​,QH​x=x−PH​x.

Formalization targets

Goal: Theorem 1.1

For Y∈{X, B∞}Y\in\{X,\ B_\infty\}Y∈{X, B∞​}, every finite ancestral HHH, every x,y∈Yx,y\in Yx,y∈Y with x=PHxx=P_Hxx=PH​x, and every R≥0R\ge0R≥0 with ∥x+y∥≤R\|x+y\|\le R∥x+y∥≤R and ∥x−y∥≤R\|x-y\|\le R∥x−y∥≤R,

∥QHy∥ ≤ 2R2−∥x∥2.\|Q_Hy\|\ \le\ 2\sqrt{R^2-\|x\|^2}.∥QH​y∥ ≤ 2R2−∥x∥2​.

The Lean statement OAI.SegmentLenses.midpoint_lens_main is the conjunction of the two cases. It is open on the platform. The displacement yyy may have a nonzero head PHyP_HyPH​y; only its tail is controlled.

Significance

The estimate is uniform over the lens: one finite head HHH controls every admissible displacement, which is exactly what is needed when a single center has infinitely many approximate midpoints. As a consequence (Corollary 7.1 of the source) both given norms are AMUC with δ^(t)≥(1+t2/4−1)/2\widehat\delta(t)\ge(\sqrt{1+t^2/4}-1)/2δ(t)≥(1+t2/4​−1)/2, while Proposition 9.1 shows that neither space admits an equivalent AUC norm. In particular the infinite-height case answers Perreau's question for the specified real norm on B∞B_\inftyB∞​, and the finite-height forest gives a reflexive space separating AMUC from AUC renormability. A companion preprint uses this theorem to force distortion D2≥1+k/4D^2\ge1+k/4D2≥1+k/4 for depth-kkk countably branching diamonds.

The result is proved only in the OpenAI preprint; it is not peer reviewed and has no machine-checked proof. Formalizing it would certify the cancellation analysis that drives the constant 222.

Difficulty

The natural attempt is to represent a nearly norming functional for the center as a convex combination of disjoint segment functionals and read off the tail. The obstacle is cancellation: two atoms leaving the head HHH through the same vertex can have segment sums of opposite sign, and a naive estimate loses all control. The bound must also hold for every displacement with the same HHH, so compactness arguments that choose HHH after yyy do not suffice, and an independent radial approach in the source gives only the weaker (2+6)R(R−∥x∥)(\sqrt2+\sqrt6)\sqrt{R(R-\|x\|)}(2​+6​)R(R−∥x∥)​.

Formalization scope

  • Vertices: ForestVertex is the subtype of pairs (h,w)(h,w)(h,w) with 1≤h1\le h1≤h and ∣w∣≤h|w|\le h∣w∣≤h; InfiniteVertex := List ℕ. Ancestry is equality of heights plus List.IsPrefix (resp. prefix only).
  • Segments: IsInterval ancestor S asserts S=[a,b]S=[a,b]S=[a,b] with a⪯ba\preceq ba⪯b, so segments are nonempty. A test family is a finite set of pairwise disjoint segments, and segmentSeminorm is the supremum of the Euclidean norms of the vectors of segment sums.
  • Spaces: X := StrongDual ℝ (UniformSpace.Completion (Test ForestVertex)); BInfinite is the closed span of the coordinate functionals inside the full dual of the infinite-tree completion, carrying the subspace (dual) norm.
  • head H x = ∑ v ∈ H, x(e_v) • e_v^* and tail H x = x - head H x; ancestrality is Ancestral.
  • Trivialization check: R≥0R\ge0R≥0 is required as in the source, and since ∥x∥≤R\|x\|\le R∥x∥≤R follows from the lens condition, the square root argument is never negative.

A full development needs the James segment norm, its completion and dual, contractivity of coordinate projections, the ℓ2\ell_2ℓ2​ decomposition of the tail over descendant cones (Lemma 2.2), and the atomic description of finite head balls (Section 4). This infrastructure is shared with the other missions in the same family. Formalizations of Lemma 2.1, Lemma 2.2, Corollary 7.1 and Proposition 9.1 are welcome as supporting results.

Selected references

  • OpenAI, Midpoint lenses in segment spaces, preprint, September 27, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Midpoint-lenses-in-segment-spaces-September-27-2026/manuscript.pdf
  • S. J. Dilworth, D. Kutzarova, N. L. Randrianarivony, J. P. Revalski, N. V. Zhivkov, Lenses and asymptotic midpoint uniform convexity, J. Math. Anal. Appl., 2016. https://doi.org/10.1016/j.jmaa.2015.11.061
  • R. C. James, A separable somewhat reflexive Banach space with nonseparable dual, Bull. Amer. Math. Soc., 1974. https://doi.org/10.1090/S0002-9904-1974-13580-9
  • M. Girardi, The dual of the James tree space is asymptotically uniformly convex, Studia Math., 2001. https://doi.org/10.4064/sm147-2-2
  • Y. Perreau, On the embeddability of countably branching bundle graphs into dual spaces, preprint, 2021. https://arxiv.org/abs/2104.10494
  • F. Baudier, R. Causey, S. Dilworth, D. Kutzarova, N. L. Randrianarivony, T. Schlumprecht, S. Zhang, On the geometry of the countably branching diamond graphs, J. Funct. Anal., 2017. https://arxiv.org/abs/1612.01984
  • F. P. Baudier, The Kadets–Werner modification of Bourgain–Rosenthal space is asymptotically midpoint uniformly convex, preprint, 2026. https://arxiv.org/abs/2609.21283
  • N. Ghoussoub, B. Maurey, GδG_\deltaGδ​-embeddings in Hilbert space, J. Funct. Anal., 1985. https://doi.org/10.1016/0022-1236(85)90039-4
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Functional Analysis·Captain: wurtle

Asymptotic midpoint uniform convexity and unbounded diamond distortion in a reflexive tree spaceResearch Paper

Motivation

Uniform convexity of a norm says that the midpoint of two far-apart points of the unit sphere lies strictly inside the ball. In infinite dimensions there is an asymptotic version: one only asks for a gain in directions that lie far out, that is, inside some closed subspace of finite codimension. Asymptotic uniform convexity and its relatives control the large-scale geometry of a Banach space, and in particular which infinite graphs can be embedded into the space with bounded distortion.

Two such properties are compared here. Asymptotic uniform convexity (AUC) demands a gain in every far-out direction separately; asymptotic midpoint uniform convexity (AMUC), introduced by Dilworth, Kutzarova, Randrianarivony, Revalski and Zhivkov (2016), only asks for a gain when a direction and its opposite are tested together. Every AUC norm is AMUC. The question is how far apart the two notions are, both up to renorming and in terms of metric embeddings of the countably branching diamond graphs DkD_kDk​.

Timeline

  • 1974. James introduces the square-sum norm over disjoint segments of a tree (the James tree space) (doi:10.1090/S0002-9904-1974-13580-9).
  • 2001. Girardi proves that the coordinate predual and the full dual of the binary James tree space are AUC (doi:10.4064/sm147-2-2).
  • 2004 and 2009. Lee and Naor obtain quantitative LpL_pLp​ distortion bounds for finite binary diamonds; Johnson and Schechtman relate diamond embeddings to super-reflexivity (doi:10.1007/s00039-004-0473-8, doi:10.1142/S1793525309000114).
  • 2016. Dilworth et al. define AMUC and construct an AMUC norm on ℓ2\ell_2ℓ2​ that is not AUC (doi:10.1016/j.jmaa.2015.11.061).
  • 2017. Baudier, Causey, Dilworth, Kutzarova, Randrianarivony, Schlumprecht and Zhang show that an equivalent AMUC norm prevents uniform embeddings of the countably branching diamonds, and that for reflexive spaces with unconditional asymptotic structure, failure of AUC renormability forces uniform diamond embeddings (arXiv:1612.01984).
  • 2018 and 2021. Swift extends the embedding construction to countably branching bundle graphs under the same hypotheses (arXiv:1710.00877); Perreau treats duals of separable spaces with weak-star unconditional asymptotic structure (arXiv:2104.10494).
  • 2025. Baudier and Lancien record, as Problem 39 of their monograph, whether the diamond implication holds for general reflexive spaces (arXiv:2512.00817).
  • 2026. Baudier shows that AMUC renormability does not imply AUC renormability, using the Kadets–Werner modification of the Bourgain–Rosenthal space, which is not reflexive (arXiv:2609.21283).

The source of this mission, an OpenAI preprint dated September 27, 2026, gives a reflexive example that separates the two notions and answers the reflexive diamond question negatively.

Setting

All spaces are real. For a Banach space YYY with norm NNN, let cof⁡(Y)\operatorname{cof}(Y)cof(Y) be the closed subspaces of finite codimension. For t>0t>0t>0,

δ‾N(t)=inf⁡N(x)=1 sup⁡F∈cof⁡(Y) inf⁡y∈F, N(y)=1(N(x+ty)−1),\overline\delta_N(t)=\inf_{N(x)=1}\ \sup_{F\in\operatorname{cof}(Y)}\ \inf_{y\in F,\ N(y)=1}\bigl(N(x+ty)-1\bigr),δN​(t)=N(x)=1inf​ F∈cof(Y)sup​ y∈F, N(y)=1inf​(N(x+ty)−1), δ^N(t)=inf⁡N(x)=1 sup⁡F∈cof⁡(Y) inf⁡y∈F, N(y)=1(N(x+ty)+N(x−ty)2−1).\widehat\delta_N(t)=\inf_{N(x)=1}\ \sup_{F\in\operatorname{cof}(Y)}\ \inf_{y\in F,\ N(y)=1}\Bigl(\tfrac{N(x+ty)+N(x-ty)}{2}-1\Bigr).δN​(t)=N(x)=1inf​ F∈cof(Y)sup​ y∈F, N(y)=1inf​(2N(x+ty)+N(x−ty)​−1).

NNN is AUC if δ‾N(t)>0\overline\delta_N(t)>0δN​(t)>0 for every t>0t>0t>0, and AMUC if δ^N(t)>0\widehat\delta_N(t)>0δN​(t)>0 for every t>0t>0t>0. A norm NNN is equivalent to ∥⋅∥\|\cdot\|∥⋅∥ if a∥x∥≤N(x)≤b∥x∥a\|x\|\le N(x)\le b\|x\|a∥x∥≤N(x)≤b∥x∥ for some 0<a≤b0<a\le b0<a≤b.

The forest. For h≥1h\ge1h≥1 let Th=N≤hT_h=\mathbb N^{\le h}Th​=N≤h be the rooted tree of words of length at most hhh, ordered by extension. The forest F\mathcal FF is the disjoint union of one copy of ThT_hTh​ for every h≥1h\ge1h≥1. A segment is an interval [a,b][a,b][a,b] of an ancestral chain. For a finitely supported u:F→Ru:\mathcal F\to\mathbb Ru:F→R,

ρ(u)=sup⁡{(∑i=1mu(Si)2)1/2:S1,…,Sm pairwise disjoint segments},u(S)=∑v∈Su(v).\rho(u)=\sup\Bigl\{\Bigl(\sum_{i=1}^m u(S_i)^2\Bigr)^{1/2} : S_1,\dots,S_m\ \text{pairwise disjoint segments}\Bigr\},\qquad u(S)=\sum_{v\in S}u(v).ρ(u)=sup{(i=1∑m​u(Si​)2)1/2:S1​,…,Sm​ pairwise disjoint segments},u(S)=v∈S∑​u(v).

Let JJJ be the completion and X=J∗X=J^*X=J∗ with the dual norm.

Diamonds. D0D_0D0​ is one edge; Dk+1D_{k+1}Dk+1​ replaces every edge of DkD_kDk​ by countably many internally disjoint two-edge paths. With the shortest-path metric dkd_kdk​, a map f:Dk→Xf:D_k\to Xf:Dk​→X has distortion at most CCC if some scale s>0s>0s>0 gives s dk(u,v)≤∥f(u)−f(v)∥≤Cs dk(u,v)s\,d_k(u,v)\le\|f(u)-f(v)\|\le Cs\,d_k(u,v)sdk​(u,v)≤∥f(u)−f(v)∥≤Csdk​(u,v) for all u,vu,vu,v.

Formalization targets

Goal: Theorem 1.1

X is infinite dimensional, separable and reflexive, and admits no equivalent AUC norm;X\ \text{is infinite dimensional, separable and reflexive, and admits no equivalent AUC norm;}X is infinite dimensional, separable and reflexive, and admits no equivalent AUC norm; δ^X(t) ≥ 1+t2/12−1(t>0);\widehat\delta_X(t)\ \ge\ \sqrt{1+t^2/12}-1\quad(t>0);δX​(t) ≥ 1+t2/12​−1(t>0); every embedding of Dk into X has distortion ≥ 1+k/12(k≥0).\text{every embedding of }D_k\text{ into }X\text{ has distortion}\ \ge\ \sqrt{1+k/12}\quad(k\ge0).every embedding of Dk​ into X has distortion ≥ 1+k/12​(k≥0).

The Lean statement OAI.ForestSpace.main_theorem is the conjunction of these six clauses. It is open on the platform.

Significance

The theorem separates AMUC from AUC renormability inside the reflexive class, which Baudier's 2026 example (non-reflexive) does not. Because AMUC is a property of the given norm while the diamond obstruction is invariant under renorming, the theorem also shows that, for general reflexive spaces, failure of AUC renormability does not force the countably branching diamonds to embed uniformly. This answers Problem 39 of Baudier–Lancien negatively and shows that the unconditional asymptotic structure hypothesis in the 2017 embedding theorem cannot simply be dropped. The quantitative modulus and distortion bounds are explicit, not merely positivity statements.

The result is proved in an OpenAI preprint; it has not been peer reviewed, and no machine-checked proof exists. A formal proof would certify the full construction, including reflexivity of J∗J^*J∗ for a non-locally-finite forest and the square-sum distortion recursion.

Difficulty

Two points are delicate. First, reflexivity: the classical James tree space is not reflexive, and here reflexivity comes from using trees of finite but unbounded height together with countable branching; the full dual J∗J^*J∗, not the coordinate completion, is the space. Second, the midpoint estimate: a segment test may cross from a finite ancestral set to its complement, and simply adding norming tests for the two parts produces uncontrolled positive cross terms. Non-renormability, by contrast, must be proved for every equivalent norm at once, so it cannot be read off from any computation with the given norm.

Formalization scope

  • The space is FullDual Vertex := StrongDual ℝ (J Vertex), where J V is the UniformSpace.Completion of TestVector V (finitely supported functions with norm rho). Vertex packs a height h≥1h\ge1h≥1 and a word in N∗\mathbb N^*N∗ of length ≤h\le h≤h; the order is equality of heights plus prefix order.
  • Segments are finite order-convex chains (IsSegment); the empty segment is allowed and contributes zero.
  • Reflexive is surjectivity of the canonical map NormedSpace.inclusionInDoubleDual, not an abstract isomorphism with the bidual.
  • EquivalentNorm E α β stores a Seminorm with explicit constants 0<α≤β0<\alpha\le\beta0<α≤β; the lower bound makes it a norm. The non-renormability clause quantifies over all such structures.
  • aucModulus and averageModulus take the inf/sup/inf order above, with sInf/sSup over real sets; for an infinite-dimensional space these sets are nonempty and bounded, so the Lean defaults are not triggered.
  • Diamond.diamond k iterates the edge replacement starting from one edge; distances are SimpleGraph.dist of the undirected graph, and EmbeddingBound is the scaled bi-Lipschitz condition above.

A complete development needs the James-type segment norm, its completion and dual, coordinate projections onto ancestral sets, and graph distances on the diamonds. The segment-norm and diamond infrastructure is shared with the other missions of this family. Contributions formalizing Lemma 2.1 (structure and reflexivity), Lemma 3.2 (bounded trees exclude AUC renorming), Lemma 4.1 (paired head–tail estimate) and Lemma 5.1 (lens lemma) are welcome.

Selected references

  • OpenAI, Asymptotic midpoint uniform convexity and unbounded diamond distortion in a reflexive tree space, preprint, September 27, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Asymptotic-midpoint-uniform-convexity-and-unbounded-diamond-distortion-in-a-reflexive-tree-space-September-27-2026/manuscript.pdf
  • S. J. Dilworth, D. Kutzarova, N. L. Randrianarivony, J. P. Revalski, N. V. Zhivkov, Lenses and asymptotic midpoint uniform convexity, J. Math. Anal. Appl., 2016. https://doi.org/10.1016/j.jmaa.2015.11.061
  • F. Baudier, R. Causey, S. Dilworth, D. Kutzarova, N. L. Randrianarivony, T. Schlumprecht, S. Zhang, On the geometry of the countably branching diamond graphs, J. Funct. Anal., 2017. https://arxiv.org/abs/1612.01984
  • F. P. Baudier, G. Lancien, Asymptotic and nonlinear geometries of Banach spaces and their interactions, Cours Spécialisés, SMF, 2026. https://arxiv.org/abs/2512.00817
  • F. P. Baudier, The Kadets–Werner modification of Bourgain–Rosenthal space is asymptotically midpoint uniformly convex, preprint, 2026. https://arxiv.org/abs/2609.21283
  • R. C. James, A separable somewhat reflexive Banach space with nonseparable dual, Bull. Amer. Math. Soc., 1974. https://doi.org/10.1090/S0002-9904-1974-13580-9
  • M. Girardi, The dual of the James tree space is asymptotically uniformly convex, Studia Math., 2001. https://doi.org/10.4064/sm147-2-2
  • A. Swift, A coding of bundle graphs and their embeddings into Banach spaces, Mathematika, 2018. https://arxiv.org/abs/1710.00877
  • Y. Perreau, On the embeddability of countably branching bundle graphs into dual spaces, preprint, 2021. https://arxiv.org/abs/2104.10494
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Functional Analysis·Captain: wurtle

A positive solution to Tingley’s problemResearch Paper

Motivation: isometries of unit spheres

The Mazur–Ulam theorem (1932) says that every surjective isometry between real normed spaces is affine. The whole space is not always available, though: often only distances between unit vectors are known. Tingley's problem (1987) asks whether the metric of the unit sphere alone already determines the linear structure, that is, whether every surjective isometry between the unit spheres of two real Banach spaces extends to a real-linear isometry of the spaces (Tingley 1987). The question has been studied for almost four decades, mostly class by class: for sequence spaces, LpL^pLp spaces, operator algebras and two-dimensional spaces. Nearly all known positive results depend on the structure of the particular spaces involved.

Timeline

  • 1932 — Mazur and Ulam: surjective isometries between real normed spaces are affine.
  • 1972 — Mankiewicz extends isometries between convex sets with nonempty interior. A unit sphere has empty interior, so this does not apply.
  • 1987 — Tingley poses the problem and shows that surjective isometries between spheres of finite-dimensional spaces preserve antipodal points (Tingley 1987).
  • 1994 — Wang treats spheres of C0(Ω)C_0(\Omega)C0​(Ω)-type spaces (Wang 1994).
  • 2003 — Ding handles ℓp(Γ)\ell^p(\Gamma)ℓp(Γ)-type spaces, p>1p>1p>1, p≠2p\ne 2p=2 (Ding 2003).
  • 2011 — Cheng and Dong formulate the Mazur–Ulam property (sphere isometries from a given space into an arbitrary target extend linearly) (Cheng–Dong 2011).
  • 2012 — Tan proves the Mazur–Ulam property for real Lp(μ)L^p(\mu)Lp(μ), 1<p<∞1<p<\infty1<p<∞, p≠2p\neq 2p=2 (Tan 2012).
  • 2014 — Tanaka: sphere isometries preserve maximal convex subsets of the sphere (Tanaka 2014).
  • 2018 — Fernández-Polo and Peralta (von Neumann algebras, JMAA 2018); Mori (preduals, JMAA 2018).
  • 2020 — Mori and Ozawa: Mazur–Ulam property for unital C∗C^*C∗-algebras and real von Neumann algebras (Studia Math. 2020).
  • 2022 — Banakh: every two-dimensional real Banach space has the Mazur–Ulam property (Banakh 2022).
  • 2025–2026 — Further class results: Schreier spaces (Fakhoury 2025); Haagerup noncommutative LpL_pLp​ and Schatten classes (Huang–Zhu, arXiv:2608.30131; arXiv:2607.11244).
  • 2026 — An OpenAI preprint, A positive solution to Tingley's problem (OpenAI Math Release, September 23, 2026), claims the general affirmative answer for all real Banach spaces. It has not been peer reviewed, and the claim has not been formally verified.

Setting

Let XXX and YYY be real Banach spaces, both nonzero. The unit sphere is SX={x∈X:∥x∥=1}S_X=\{x\in X:\|x\|=1\}SX​={x∈X:∥x∥=1} with the metric inherited from XXX. A map f:SX→SYf:S_X\to S_Yf:SX​→SY​ is an isometry if ∥f(x)−f(y)∥=∥x−y∥\|f(x)-f(y)\|=\|x-y\|∥f(x)−f(y)∥=∥x−y∥ for all x,y∈SXx,y\in S_Xx,y∈SX​, and it is surjective if every point of SYS_YSY​ is attained.

Any linear extension of fff is forced to be the radial extension

T(0)=0,T(x)=∥x∥ f ⁣(x∥x∥)(x≠0).T(0)=0,\qquad T(x)=\|x\|\,f\!\left(\frac{x}{\|x\|}\right)\quad(x\neq 0).T(0)=0,T(x)=∥x∥f(∥x∥x​)(x=0).

In Lean, UnitSphere X is the subtype {x:X∣∥x∥=1}\{x : X \mid \|x\|=1\}{x:X∣∥x∥=1} and normalize x hx is x/∥x∥x/\|x\|x/∥x∥ as an element of it.

Formalization targets

Goal: Tingley's problem (Theorem 1.1)

For nonzero real Banach spaces X,YX,YX,Y and every surjective isometry f:SX→SYf:S_X\to S_Yf:SX​→SY​ there is a surjective real-linear isometry T:X→YT:X\to YT:X→Y such that

T∣SX=f,T(0)=0,T(x)=∥x∥ f ⁣(x∥x∥) (x≠0),T|_{S_X}=f,\qquad T(0)=0,\qquad T(x)=\|x\|\,f\!\left(\tfrac{x}{\|x\|}\right)\ (x\neq0),T∣SX​​=f,T(0)=0,T(x)=∥x∥f(∥x∥x​) (x=0),

and TTT is the only real-linear map X→YX\to YX→Y that agrees with fff on SXS_XSX​. This is the full statement of Theorem 1.1 of the source. The goal is published on the platform with status Open: no machine-checked proof exists yet.

Significance

The result itself. An affirmative answer turns a forty-year class-by-class programme into a single theorem: the metric of the unit sphere of any real Banach space determines the space up to linear isometry. Every space then has the Mazur–Ulam property in the sense of Cheng and Dong, with no separability, reflexivity, smoothness or strict convexity assumptions. For complex Banach spaces viewed as real spaces the conclusion is real-linearity only; complex-linearity is not claimed.

Formalizing it. The claimed proof combines classical tools (supporting functionals, Banach-space ultrapowers, Darbo's fixed-point theorem with the Kuratowski measure of noncompactness, the Mazur–Ulam theorem) with new geometric estimates on aligned chords. A machine-checked proof would certify a result whose proof has not yet been refereed. The Mazur–Ulam theorem itself is already in Mathlib (IsometryEquiv.toRealLinearIsometryEquiv); ultrapowers of Banach spaces and Darbo's theorem are not.

Difficulty

The radial map TTT preserves norms and preserves distances between points of the same radius. What has to be shown is that it preserves distances between points on different spheres, ∥f(x)−qf(y)∥=∥x−qy∥\|f(x)-qf(y)\|=\|x-qy\|∥f(x)−qf(y)∥=∥x−qy∥ for 0<q<10<q<10<q<1, using only distances measured on a single sphere. Once this holds, TTT is a surjective isometry fixing 000 and Mazur–Ulam gives linearity. The obvious attempt (extend the isometry to a neighbourhood, or use convex-set extension theorems such as Mankiewicz's) fails because the sphere has empty interior. Structural arguments (smoothness, facial structure, explicit duals) cover only special classes of spaces. In general, the maximal defect sup⁡∣∥f(x)−qf(y)∥−∥x−qy∥∣\sup|\|f(x)-qf(y)\|-\|x-qy\||sup∣∥f(x)−qf(y)∥−∥x−qy∥∣ need not be attained, and no compactness is available in infinite dimensions.

Formalization scope

  • XXX and YYY are arbitrary types with NormedAddCommGroup, NormedSpace ℝ and CompleteSpace, and Nontrivial (the source's "nonzero"). Universe levels are independent, and no separability or dimension hypothesis is imposed.
  • The sphere is UnitSphere X := {x // ‖x‖ = 1} with the subtype metric; Isometry f and Function.Surjective f are the hypotheses.
  • The conclusion is an existential over X ≃ₗᵢ[ℝ] Y (a bijective real-linear isometry) with the five clauses: agreement on the sphere, T0=0T0=0T0=0, the radial formula, surjectivity, and uniqueness among all X →ₗ[ℝ] Y that agree with fff on the sphere. No hypothesis assumes any distance between different radii, so the statement is not trivialized.
  • Infrastructure a full development needs: Hahn–Banach supporting functionals, Banach-space ultrapowers (or another attainment device), the Kuratowski measure of noncompactness and Darbo's fixed-point theorem, together with Mathlib's Mazur–Ulam theorem. Ultrapowers and Darbo's theorem would be reusable well beyond this mission.

Selected references

  • D. Tingley, Isometries of the unit sphere, Geom. Dedicata 22 (1987), 371–378. https://doi.org/10.1007/BF00147942
  • S. Mazur and S. Ulam, Sur les transformations isométriques d'espaces vectoriels normés, C. R. Acad. Sci. Paris 194 (1932), 946–948.
  • P. Mankiewicz, On extension of isometries in normed linear spaces, Bull. Acad. Polon. Sci. Sér. Sci. Math. Astronom. Phys. 20 (1972).
  • R. S. Wang, Isometries between the unit spheres of C0(Ω)C_0(\Omega)C0​(Ω) type spaces, Acta Math. Sci. 14 (1994), 82–89. https://doi.org/10.1016/S0252-9602(18)30093-6
  • G. G. Ding, The isometric extension problem in the unit spheres of ℓp(Γ)\ell^p(\Gamma)ℓp(Γ) (p>1)(p>1)(p>1) type spaces, Sci. China Ser. A 46 (2003), 333–338. https://doi.org/10.1360/03ys9035
  • L. Cheng and Y. Dong, On a generalized Mazur–Ulam question, J. Math. Anal. Appl. 377 (2011), 464–470. https://doi.org/10.1016/j.jmaa.2010.11.025
  • D.-N. Tan, Extension of isometries on the unit sphere of LpL^pLp spaces, Acta Math. Sin. (Engl. Ser.) 28 (2012), 1197–1208. https://doi.org/10.1007/s10114-011-0302-6
  • R. Tanaka, A further property of spherical isometries, Bull. Aust. Math. Soc. 90 (2014), 304–310. https://doi.org/10.1017/S0004972714000185
  • F. J. Fernández-Polo and A. M. Peralta, On the extension of isometries between the unit spheres of von Neumann algebras, J. Math. Anal. Appl. 466 (2018), 127–143. https://doi.org/10.1016/j.jmaa.2018.05.062
  • M. Mori, Tingley's problem through the facial structure of operator algebras, J. Math. Anal. Appl. 466 (2018), 1281–1298. https://doi.org/10.1016/j.jmaa.2018.06.050
  • M. Mori and N. Ozawa, Mankiewicz's theorem and the Mazur–Ulam property for C∗C^*C∗-algebras, Studia Math. 250 (2020), 265–281. https://doi.org/10.4064/sm180727-14-11
  • T. Banakh, Every 2-dimensional Banach space has the Mazur–Ulam property, Linear Algebra Appl. 632 (2022), 268–280. https://doi.org/10.1016/j.laa.2021.09.020
  • G. Darbo, Punti uniti in trasformazioni a codominio non compatto, Rend. Sem. Mat. Univ. Padova 24 (1955), 84–92.
  • OpenAI, A positive solution to Tingley's problem, OpenAI Math Release preprint, September 23, 2026 (Theorem 1.1, p. 1). https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/A-positive-solution-to-Tingleys-problem-September-23-2026/paper.pdf
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Functional Analysis·Captain: wurtle

Backward intertwiners and a transitive commutantResearch Paper

Motivation

A closed subspace M\mathcal MM of a Hilbert space HHH is hyperinvariant for a bounded operator SSS if AM⊆MA\mathcal M\subseteq\mathcal MAM⊆M for every operator AAA commuting with SSS. The hyperinvariant subspace problem asks whether every bounded nonscalar operator on an infinite-dimensional separable complex Hilbert space has a nonzero proper closed hyperinvariant subspace. It is a strengthening of the invariant subspace problem, closely tied to the theory of transitive operator algebras: SSS has no such subspace exactly when its commutant {S}′\{S\}'{S}′ is transitive. A related classical question asks whether every unital transitive operator algebra is strongly dense in B(H)B(H)B(H); Arveson's density theorem gives a positive answer when the algebra contains a maximal abelian self-adjoint subalgebra.

Timeline

  • 1967. Arveson proves that a transitive algebra containing a maximal abelian self-adjoint subalgebra is strongly dense in B(H)B(H)B(H) (doi:10.1215/S0012-7094-67-03467-9).
  • 1972. Douglas and Pearcy relate hyperinvariant subspaces to transitive algebras (doi:10.1307/mmj/1029000793).
  • 1981–1982. Domar describes translation-invariant subspaces of weighted ℓp\ell^pℓp and LpL^pLp spaces (doi:10.7146/math.scand.a-11926); Grabiner studies unicellular shifts.
  • 1999. Atzmon and Sodin construct completely indecomposable bilateral weighted shifts with spectrum the unit circle, leaving open whether they have proper hyperinvariant subspaces (doi:10.1006/jfan.1999.3454).
  • 2005. Dykema observes that hyperinvariant subspaces of an operator in a von Neumann algebra have projections in that algebra (doi:10.1007/s00208-005-0669-8).
  • 2025–2026. A preprint of Kérchy and Pearcy claiming an equivalence between the invariant and hyperinvariant problems is withdrawn after a counterexample to its Theorem 3 (arXiv:2503.13005); Kérchy studies hyperinvariant subspaces of operators containing unilateral shifts (doi:10.1007/s11785-026-02038-9).

The source of this mission is an OpenAI preprint dated September 27, 2026. A companion OpenAI preprint of the same date reaches the same existence conclusion through invariant projections in an irrational-rotation factor, by a different construction.

Setting

Let HHH be a complex Hilbert space and B(H)B(H)B(H) its bounded operators. For S∈B(H)S\in B(H)S∈B(H):

  • the commutant is {S}′={A∈B(H):AS=SA}\{S\}'=\{A\in B(H):AS=SA\}{S}′={A∈B(H):AS=SA}, a unital subalgebra of B(H)B(H)B(H);
  • {S}′\{S\}'{S}′ is transitive if the only closed subspaces M\mathcal MM with AM⊆MA\mathcal M\subseteq\mathcal MAM⊆M for all A∈{S}′A\in\{S\}'A∈{S}′ are {0}\{0\}{0} and HHH;
  • SSS is norm-quasinilpotent if ∥Sn∥1/n→0\|S^n\|^{1/n}\to0∥Sn∥1/n→0;
  • the strong operator topology on B(H)B(H)B(H) is the topology of pointwise norm convergence: Aλ→AA_\lambda\to AAλ​→A iff Aλx→AxA_\lambda x\to AxAλ​x→Ax for every x∈Hx\in Hx∈H.

Formalization targets

Goal: Corollary 1.2

For every infinite-dimensional separable complex Hilbert space HHH there is S∈B(H)S\in B(H)S∈B(H) with

S≠0,lim⁡n→∞∥Sn∥1/n=0,{S}′ transitive,{S}′≠B(H),{S}′ strongly closed.S\neq0,\qquad \lim_{n\to\infty}\|S^n\|^{1/n}=0,\qquad \{S\}'\ \text{transitive},\qquad \{S\}'\neq B(H),\qquad \{S\}'\ \text{strongly closed}.S=0,n→∞lim​∥Sn∥1/n=0,{S}′ transitive,{S}′=B(H),{S}′ strongly closed.

The Lean statement OAI.BackwardIntertwiners.direct_algebra_corollary is open on the platform. The family statement OAI.Hyperinvariant.main_theorem asserts the same proposition and is included as a reference item.

Significance

Corollary 1.2 gives a negative answer to the hyperinvariant subspace problem on every separable infinite-dimensional Hilbert space, and its commutant is a proper, strongly closed, unital transitive algebra, so it also answers negatively whether every unital transitive operator algebra is strongly dense in B(H)B(H)B(H). The construction behind it (Theorem 1.1) is explicit: a weighted shift over the 2-adic odometer whose fibres have only coordinate-tail invariant subspaces, an explicit bound ∥Sn∥≤exp⁡(−10⌊(n+1)2/4⌋)\|S^n\|\le\exp(-10\lfloor(n+1)^2/4\rfloor)∥Sn∥≤exp(−10⌊(n+1)2/4⌋), and a bounded commuting operator moving those tails backward. The operator does have many ordinary invariant subspaces, so the invariant subspace problem itself is untouched.

The result is proved in an OpenAI preprint, which has not been peer reviewed. No machine-checked proof exists.

Difficulty

Weighted shifts have rich lattices of invariant subspaces, so one must first pin down the invariant subspaces of each fibre (a quadratic weighted-translation criterion in the style of Domar) and then find enough operators in the commutant to destroy every candidate. Multiplication operators and the shift alone leave every fixed tail L2(X;K≥h)L^2(X;K_{\ge h})L2(X;K≥h​) invariant. The essential step is a bounded operator commuting with SSS that moves tails backward across fibres; this requires opposite logarithmic drifts of the weights at the two ends of the bilateral sequence and one measurable normalization valid on the whole base. Arveson's theorem cannot be used, since the multiplier algebra has infinite multiplicity and is not maximal abelian.

Formalization scope

  • H is any type with [InnerProductSpace ℂ H] [CompleteSpace H] [SeparableSpace H] and ¬FiniteDimensional ℂ H; the claim is existential in T : H →L[ℂ] H.
  • commutant T is Subalgebra.centralizer ℂ {T}; TransitiveCommutant T quantifies over closed Submodules invariant under every A with A * T = T * A.
  • Quasinilpotence is Tendsto (fun n => ‖T ^ n‖ ^ (1 / n)) atTop (𝓝 0) (the n=0n=0n=0 term is irrelevant to the limit).
  • The strong operator topology is TopologicalSpace.induced from the pointwise (product) topology on functions H → H.

A complete development needs vector-valued L2L^2L2 spaces over the 2-adic integers with Haar measure, weighted shifts and their invariant subspaces, measurable fields of projections, and transport to an arbitrary separable Hilbert space by a unitary. Contributions formalizing Theorem 1.1 (the construction), Lemma 2.1 (weighted translation criterion), Proposition 4.3 (a bounded backward intertwiner) and Lemma 5.1 (strict descent) are welcome.

Selected references

  • OpenAI, Backward intertwiners and a transitive commutant, preprint, September 27, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Backward-intertwiners-and-a-transitive-commutant-September-27-2026/paper.pdf
  • OpenAI, Invariant-projection counterexamples for every irrational rotation, preprint, September 27, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Invariant-projection-counterexamples-for-every-irrational-rotation-September-27-2026/paper.pdf
  • W. B. Arveson, A density theorem for operator algebras, Duke Math. J., 1967. https://doi.org/10.1215/S0012-7094-67-03467-9
  • R. G. Douglas, C. Pearcy, Hyperinvariant subspaces and transitive algebras, Michigan Math. J., 1972. https://doi.org/10.1307/mmj/1029000793
  • Y. Domar, Translation invariant subspaces of weighted lpl^plp and LpL^pLp spaces, Math. Scand., 1981. https://doi.org/10.7146/math.scand.a-11926
  • A. Atzmon, M. Sodin, Completely indecomposable operators and a uniqueness theorem of Cartwright–Levinson type, J. Funct. Anal., 1999. https://doi.org/10.1006/jfan.1999.3454
  • K. Dykema, Hyperinvariant subspaces for some B-circular operators, Math. Ann., 2005. https://doi.org/10.1007/s00208-005-0669-8
  • L. Kérchy, C. Pearcy, Hyperinvariant subspaces of block-triangular operators on Hilbert space, withdrawn preprint, 2025. https://arxiv.org/abs/2503.13005
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Mathematical PhysicsProbability·Captain: wurtle

A radial continuum phase transition with algebraic decayResearch Paper

Motivation: continuum phase transitions with a power-law tail

Whether identical classical particles in R3\mathbb R^3R3, interacting only through a stable radial pair potential, can undergo a phase transition is a classical existence problem of rigorous statistical mechanics, highlighted in Simon's list of problems in mathematical physics (Simon 1984). A transition shows up as a singularity of the thermodynamic free energy. Earlier rigorous continuum transitions rely on extra structure — two species, many-body terms, hard cores, or interactions defined through a fixed partition into boxes — or on a mean-field limit in which the potential itself changes. A natural requirement for a satisfactory answer is a single fixed pair potential with a bounded core and an explicit integrable power-law tail.

Timeline

  • 1965 — Motzkin and Straus's weighted-graph maximization, later used for occupation bounds (Motzkin–Straus 1965).
  • 1966 — Lebowitz and Penrose: rigorous van der Waals–Maxwell theory in the Kac limit (Lebowitz–Penrose 1966).
  • 1970 — Ruelle's superstability framework (Ruelle 1970).
  • 1971 — Ruelle: transition for a symmetric two-species continuum system (Ruelle 1971).
  • 1973 — Gerardi, Marchioro, Olivieri and Presutti extend the Lebowitz–Penrose limit to superstable references (GMOP 1973).
  • 1984 — Simon lists the problem among fifteen problems in mathematical physics.
  • 1998–1999 — Lebowitz, Mazel and Presutti: liquid–vapor transition with attractive pair and repulsive four-body interactions (PRL 1998, J. Stat. Phys. 1999).
  • 2026 — He, Jauslin, Lebowitz and Peled: transition for a finite-range box-modified Kac pair interaction (CMP 2026); Dereudre and Renaud-Chan: density coexistence for saturated many-body interactions (arXiv:2602.11078).
  • 2026 — Two OpenAI preprints (OpenAI Math Release, September 24, 2026): a radial potential with divergent core and o(r−3)o(r^{-3})o(r−3) tail with a temperature singularity, and the present A radial continuum phase transition with algebraic decay, which claims a bounded continuous potential with ∣ϕ(r)∣≤Cr−3−1/32|\phi(r)|\le Cr^{-3-1/32}∣ϕ(r)∣≤Cr−3−1/32. Neither is peer reviewed, and the theorem is not formally verified.

Setting

Particles live in R3\mathbb R^3R3; a radial pair potential is a function ϕ:[0,∞)→R\phi:[0,\infty)\to\mathbb Rϕ:[0,∞)→R (in Lean, ℝ≥0 → ℝ) applied to pair distances. For the cube ΛL=[0,L]3\Lambda_L=[0,L]^3ΛL​=[0,L]3 and N≥0N\ge0N≥0,

Uϕ(x1,…,xN)=∑i<jϕ(∣xi−xj∣),ZL,N(β)=1N!∫ΛLNe−βUϕ dx,ZL,0=1.U^\phi(x_1,\dots,x_N)=\sum_{i<j}\phi(|x_i-x_j|),\qquad Z_{L,N}(\beta)=\frac1{N!}\int_{\Lambda_L^N}e^{-\beta U^\phi}\,dx,\qquad Z_{L,0}=1 .Uϕ(x1​,…,xN​)=i<j∑​ϕ(∣xi​−xj​∣),ZL,N​(β)=N!1​∫ΛLN​​e−βUϕdx,ZL,0​=1.

The potential is stable if Uϕ≥−BNU^\phi\ge -BNUϕ≥−BN for all configurations. The canonical free energy at density ρ\rhoρ is

f(β,ρ)=−lim⁡L→∞1βL3log⁡ZL,⌊ρL3⌋(β).f(\beta,\rho)=-\lim_{L\to\infty}\frac1{\beta L^3}\log Z_{L,\lfloor\rho L^3\rfloor}(\beta).f(β,ρ)=−L→∞lim​βL31​logZL,⌊ρL3⌋​(β).

The packing constant is p=lim⁡L→∞ML/L3p=\lim_{L\to\infty}M_L/L^3p=limL→∞​ML​/L3, where MLM_LML​ is the largest number of points in [0,L]3[0,L]^3[0,L]3 at mutual distance ≥1\ge1≥1; in Lean IsPackingDensity p asserts this limit. StrictTemperatureCorner f βc asserts finite left and right derivatives at βc\beta_cβc​ with the right one strictly smaller, and non-differentiability.

Formalization targets

Milestone: the corner at the central density

At the single density ρ=5p/3\rho=5p/3ρ=5p/3: there are a bounded continuous stable ϕ\phiϕ with ∣ϕ(r)∣≤Cr−3−1/32|\phi(r)|\le Cr^{-3-1/32}∣ϕ(r)∣≤Cr−3−1/32 for r≥1r\ge1r≥1 and βc∈[7/8,9/8]\beta_c\in[7/8,9/8]βc​∈[7/8,9/8] such that f(⋅,5p/3)f(\cdot,5p/3)f(⋅,5p/3) exists for all β>0\beta>0β>0 and

f−′(βc,5p/3)>f+′(βc,5p/3).f'_-(\beta_c,5p/3)>f'_+(\beta_c,5p/3).f−′​(βc​,5p/3)>f+′​(βc​,5p/3).

Goal: a common corner on a density interval

There are a bounded continuous ϕ\phiϕ, constants B,C>0B,C>0B,C>0 with

∑i<jϕ(∣xi−xj∣)≥−BN,∣ϕ(r)∣≤C r−3−1/32 (r≥1),\sum_{i<j}\phi(|x_i-x_j|)\ge -BN,\qquad |\phi(r)|\le C\,r^{-3-1/32}\ (r\ge1),i<j∑​ϕ(∣xi​−xj​∣)≥−BN,∣ϕ(r)∣≤Cr−3−1/32 (r≥1),

an open interval I=(5p/3−η, 5p/3+η)⊂(0,∞)I=(5p/3-\eta,\,5p/3+\eta)\subset(0,\infty)I=(5p/3−η,5p/3+η)⊂(0,∞) and one βc∈[7/8,9/8]\beta_c\in[7/8,9/8]βc​∈[7/8,9/8] such that for every ρ∈I\rho\in Iρ∈I the free energy f(β,ρ)f(\beta,\rho)f(β,ρ) exists and is finite for every β>0\beta>0β>0, and

f−′(βc,ρ)>f+′(βc,ρ).f'_-(\beta_c,\rho)>f'_+(\beta_c,\rho).f−′​(βc​,ρ)>f+′​(βc​,ρ).

This is Theorem 1.1 of the source. Both statements are published on the platform with status Open.

Significance

The result itself. The theorem gives a single-species, bounded, continuous radial pair potential with an explicit integrable power-law tail whose canonical free energy has a strict temperature corner at one critical inverse temperature for a whole interval of densities. The interaction is a genuine radial function of separations with all long-range terms kept; boxes appear only in the estimates. It does not treat Lennard–Jones-type potentials and does not identify the phases as conventional fluids. The companion preprint has a divergent core but only an o(r−3)o(r^{-3})o(r−3) tail; the fixed power margin 1/321/321/32 here needs a quantitative range estimate not present there.

Formalizing it. The statement fixes the model completely (free boundary conditions on [0,L]3[0,L]^3[0,L]3, Lebesgue measure without temperature normalization, 1/N!1/N!1/N!, ⌊ρL3⌋\lfloor\rho L^3\rfloor⌊ρL3⌋ particles), so a formal proof would settle exactly which version of the problem is solved. The infrastructure (thermodynamic limits, convex duality for pressures, Kac comparisons) is reusable for the companion mission.

Difficulty

The Lebowitz–Penrose theory produces non-convex mean-field free energies only in the limit where the attraction range tends to infinity, and that limiting object is not the free energy of any fixed potential. A single potential must therefore contain infinitely many attractions at growing ranges, and the required singularity must survive all of them. Density coexistence at fixed temperature does not by itself give a temperature corner at a fixed density: two supporting slopes with equal density coordinate and different energy coordinates are needed. A pointwise power bound constrains how strong the successive attractions may be relative to their ranges, which is why a quantitative comparison with an explicit error is required.

Formalization scope

  • Positions are EuclideanSpace ℝ (Fin 3); distances enter through nndist, so the potential is a function on ℝ≥0. Boundedness, continuity, stability with B>0B>0B>0, and decay with C>0C>0C>0 are separate conjuncts.
  • ppp is existentially quantified but pinned by IsPackingDensity p (a limit), and p>0p>0p>0 is required; packingNumber is a sSup over a bounded set of naturals.
  • IsCanonicalFreeEnergy φ ρ f asserts −log⁡Z/(βL3)→f(β)-\log Z/(\beta L^3)\to f(\beta)−logZ/(βL3)→f(β) for every β>0\beta>0β>0, so fff is determined on (0,∞)(0,\infty)(0,∞); one-sided derivatives use HasDerivWithinAt on Iic βc and Ici βc.
  • The goal requires the interval to lie in (0,∞)(0,\infty)(0,∞) and βc\beta_cβc​ to be independent of ρ\rhoρ.
  • Needed infrastructure: superstability and occupation moments, existence of thermodynamic limits and their convex duality, a Motzkin–Straus bound, quantitative Kac comparison, and subdifferential persistence arguments.

Selected references

  • B. Simon, Fifteen problems in mathematical physics, in Perspectives in Mathematics, Birkhäuser, 1984, 423–454. https://math.caltech.edu/SimonPapers/R27.pdf
  • T. S. Motzkin and E. G. Straus, Maxima for graphs and a new proof of a theorem of Turán, Canad. J. Math. 17 (1965), 533–540. https://doi.org/10.4153/CJM-1965-053-6
  • J. L. Lebowitz and O. Penrose, Rigorous treatment of the van der Waals–Maxwell theory of the liquid-vapor transition, J. Math. Phys. 7 (1966), 98–113. https://doi.org/10.1063/1.1704821
  • D. Ruelle, Superstable interactions in classical statistical mechanics, Comm. Math. Phys. 18 (1970), 127–159. https://doi.org/10.1007/BF01646091
  • D. Ruelle, Existence of a phase transition in a continuous classical system, Phys. Rev. Lett. 27 (1971), 1040–1041. https://doi.org/10.1103/PhysRevLett.27.1040
  • A. Gerardi, C. Marchioro, E. Olivieri and E. Presutti, Van der Waals–Maxwell theory, Lebowitz–Penrose limit and superstable interactions, Comm. Math. Phys. 29 (1973), 219–231. https://doi.org/10.1007/BF01645248
  • J. L. Lebowitz, A. E. Mazel and E. Presutti, Liquid–vapor phase transitions for systems with finite-range interactions, J. Stat. Phys. 94 (1999), 955–1025. https://doi.org/10.1023/A:1004591218510
  • Q. He, I. Jauslin, J. Lebowitz and R. Peled, Liquid-vapor transition in a model of a continuum particle system with finite-range modified Kac pair potential, Comm. Math. Phys. 407 (2026), 240. https://doi.org/10.1007/s00220-026-05735-w
  • D. Dereudre and C. Renaud-Chan, First-order phase transition for Gibbs point processes with saturated interactions, arXiv:2602.11078 (2026). https://arxiv.org/abs/2602.11078v1
  • R. T. Rockafellar and R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
  • OpenAI, A continuum temperature singularity for a radial pair potential, OpenAI Math Release preprint, September 24, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/A-continuum-temperature-singularity-for-a-radial-pair-potential-September-24-2026/paper.pdf
  • OpenAI, A radial continuum phase transition with algebraic decay, OpenAI Math Release preprint, September 24, 2026 (Theorem 1.1, p. 1). https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/A-radial-continuum-phase-transition-with-algebraic-decay-September-24-2026/paper.pdf
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