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Operations ResearchOptimizationProbability·Captain: mikedeng1

Sample-Driven Optimal Stopping: From the Secretary Problem to the i.i.d. Prophet Inequality III: The Explicit Lower Bound on the Competitive Ratio Is at Least α* Times pResearch Paper

Motivation

Optimal stopping with partial information sits between two classical problems. In the secretary problem a decision maker sees values in random order, knows nothing about how they are generated, and must stop on the best one; the optimal guarantee is 1/e1/e1/e. In the i.i.d. prophet inequality the values are independent draws from a known distribution, and the best guarantee, relative to the expected maximum, is the constant α∗≈0.745\alpha^*\approx 0.745α∗≈0.745: Hill and Kertz (1982) and Kertz (1986) showed that no stopping rule does better on every distribution, and Correa, Foncea, Hoeksma, Oosterwijk and Vredeveld (2017, doi:10.1145/3033274.3085137) gave a rule that achieves it. Practical settings, such as pricing from historical data, lie in between: the distribution is unknown, but samples of it are available.

Correa, Cristi, Epstein and Soto (arXiv:2011.06516v2) interpolate between the two problems with the ppp-sample-driven optimal stopping problem: each of NNN adversarial values is independently revealed in advance (a sample) with probability ppp, and the remaining values arrive online in random order. At p=0p=0p=0 this is the secretary problem; as p→1p\to1p→1 it approaches the i.i.d. prophet inequality. They show that the optimal competitive ratio α(p)\alpha(p)α(p) of the limit problem is the value of an infinite-dimensional linear program, and they construct an explicit threshold rule whose guarantee α~(p)\tilde\alpha(p)α~(p) is the root of a scalar equation.

Prior work on learning a distribution from samples obtained guarantees α∗−O(ε)\alpha^*-O(\varepsilon)α∗−O(ε) with O(n2/ε)O(n^2/\varepsilon)O(n2/ε) samples (Correa, Dütting, Fischer, Schewior, 2019) and with O(n/ε6)O(n/\varepsilon^6)O(n/ε6) samples (Rubinstein, Wang, Weinberg, 2020). Theorem 9 of the paper, the goal of this mission, gives such a guarantee with O(n/ε)O(n/\varepsilon)O(n/ε) samples.

Setting

Fix p∈(0,1)p\in(0,1)p∈(0,1). The guarantee of the explicit threshold rule is the number α~(p)∈(0,1)\tilde\alpha(p)\in(0,1)α~(p)∈(0,1) solving

ln⁡p+α~(1−p)2p=∑i=1∞ln⁡(1−α~+α~[(i+1)pi−ipi+1])i(i+1).(19)\ln p+\frac{\tilde\alpha(1-p)^2}{p}=\sum_{i=1}^{\infty}\frac{\ln\bigl(1-\tilde\alpha+\tilde\alpha[(i+1)p^i-ip^{i+1}]\bigr)}{i(i+1)}.\tag{19}lnp+pα~(1−p)2​=i=1∑∞​i(i+1)ln(1−α~+α~[(i+1)pi−ipi+1])​.(19)

Lemma 7 of the paper shows that (19) has exactly one root in (0,1)(0,1)(0,1). The i.i.d. prophet constant α∗∈(0,1)\alpha^*\in(0,1)α∗∈(0,1) is the solution of

∫01dyy(1−ln⁡y)+1/α∗−1=1.\int_0^1\frac{dy}{y(1-\ln y)+1/\alpha^*-1}=1 .∫01​y(1−lny)+1/α∗−1dy​=1.

The proof of Theorem 9 (Appendix B.9) works with three auxiliary functions of ppp, each depending on α∗\alpha^*α∗ as a parameter:

a(p)=∑i≥1ln⁡(1p−α∗(1−pi(1+i(1−p))))i(i+1)+α∗(2p−p2),b(p)=1p2∑i≥11i(i+1)(1p−α∗(1−pi(1+i(1−p)))),a(p)=\sum_{i\ge1}\frac{\ln\bigl(\tfrac1p-\alpha^*(1-p^i(1+i(1-p)))\bigr)}{i(i+1)}+\alpha^*(2p-p^2),\qquad b(p)=\frac1{p^2}\sum_{i\ge1}\frac{1}{i(i+1)\bigl(\tfrac1p-\alpha^*(1-p^i(1+i(1-p)))\bigr)},a(p)=i≥1∑​i(i+1)ln(p1​−α∗(1−pi(1+i(1−p))))​+α∗(2p−p2),b(p)=p21​i≥1∑​i(i+1)(p1​−α∗(1−pi(1+i(1−p))))1​, c(p)=∑i≥1pi−1−pi1pα∗−1+pi(1+i(1−p)).c(p)=\sum_{i\ge1}\frac{p^{i-1}-p^i}{\tfrac1{p\alpha^*}-1+p^i(1+i(1-p))}.c(p)=i≥1∑​pα∗1​−1+pi(1+i(1−p))pi−1−pi​.

Appendix B.7 also names the two sides of (19): f(p,α)=ln⁡p+α(1−p)2/pf(p,\alpha)=\ln p+\alpha(1-p)^2/pf(p,α)=lnp+α(1−p)2/p and g(p,α)=∑i≥1ln⁡(1+α(pi(1+i(1−p))−1))/(i(i+1))g(p,\alpha)=\sum_{i\ge1}\ln(1+\alpha(p^i(1+i(1-p))-1))/(i(i+1))g(p,α)=∑i≥1​ln(1+α(pi(1+i(1−p))−1))/(i(i+1)). In Lean, IsAlphaTilde p a and IsAlphaStar s are shared predicates in SampleDrivenOS.Limit; aB9 s p, bB9 s p, cB9 s p, fB7 p α, and gB7 p α are in SampleDrivenOS.Linear.

Formalization targets

Goal: Theorem 9 (p. 17)

for every p∈(0,1):α~(p) ≥ α∗p.\text{for every }p\in(0,1):\qquad \tilde\alpha(p)\ \ge\ \alpha^*p .for every p∈(0,1):α~(p) ≥ α∗p.

It is stated for every root α~\tilde\alphaα~ of (19) and every solution α∗\alpha^*α∗ of the integral equation; neither existence nor uniqueness is assumed.

Milestones (Appendix B.7 and B.9, in the order the proof uses them)

  1. B.7: f(p,⋅)f(p,\cdot)f(p,⋅) is strictly increasing on [0,1][0,1][0,1] and g(p,⋅)g(p,\cdot)g(p,⋅) non-increasing on [0,1)[0,1)[0,1).
  2. B.9: if (19) holds with "≤\le≤" at α∗p\alpha^*pα∗p in place of α~\tilde\alphaα~ (after the substitution α~=f(p)p\tilde\alpha=f(p)pα~=f(p)p), then α~(p)≥α∗p\tilde\alpha(p)\ge\alpha^*pα~(p)≥α∗p.
  3. B.9: that inequality is equivalent to α∗≤a(p)\alpha^*\le a(p)α∗≤a(p).
  4. B.9: aaa is differentiable on (0,1)(0,1)(0,1) with a′(p)=2α∗(1−p)−b(p)+c(p)a'(p)=2\alpha^*(1-p)-b(p)+c(p)a′(p)=2α∗(1−p)−b(p)+c(p), also in term-by-term form.
  5. B.9: b(p)≥1/pb(p)\ge 1/pb(p)≥1/p.
  6. B.9: c(p)≤1p∫01dy1/(pα∗)−1+y(1−pln⁡y)−α∗(1−p)c(p)\le\frac1p\int_0^1\frac{dy}{1/(p\alpha^*)-1+y(1-p\ln y)}-\alpha^*(1-p)c(p)≤p1​∫01​1/(pα∗)−1+y(1−plny)dy​−α∗(1−p).
  7. B.9: using the defining equation of α∗\alpha^*α∗,
1p∫01dy1pα∗−1+y(1−pln⁡y)≤1p−1−pp(1pα∗−1e)ln⁡1pα∗+pe1pα∗+pe−1.\frac1p\int_0^1\frac{dy}{\tfrac1{p\alpha^*}-1+y(1-p\ln y)}\le\frac1p-\frac{1-p}{p}\Bigl(\frac1{p\alpha^*}-\frac1e\Bigr)\ln\frac{\tfrac1{p\alpha^*}+\tfrac pe}{\tfrac1{p\alpha^*}+\tfrac pe-1}.p1​∫01​pα∗1​−1+y(1−plny)dy​≤p1​−p1−p​(pα∗1​−e1​)lnpα∗1​+ep​−1pα∗1​+ep​​.
  1. B.9: for all s∈[0.74,0.75]s\in[0.74,0.75]s∈[0.74,0.75] and p∈(0,1)p\in(0,1)p∈(0,1), (1ps−1e)ln⁡1/(ps)+p/e1/(ps)+p/e−1≥0.8\bigl(\frac1{ps}-\frac1e\bigr)\ln\frac{1/(ps)+p/e}{1/(ps)+p/e-1}\ge0.8(ps1​−e1​)ln1/(ps)+p/e−11/(ps)+p/e​≥0.8.
  2. B.9: if α∗∈[0.74,0.75]\alpha^*\in[0.74,0.75]α∗∈[0.74,0.75], then c(p)≤1p−α∗(1−p)(1+1p)c(p)\le\frac1p-\alpha^*(1-p)(1+\frac1p)c(p)≤p1​−α∗(1−p)(1+p1​).
  3. B.9: under the same hypothesis, ddpa(p)≤0\frac{d}{dp}a(p)\le0dpd​a(p)≤0 on (0,1)(0,1)(0,1).

Significance

The explicit rule's guarantee α~(p)\tilde\alpha(p)α~(p) is a lower bound on the optimal ratio α(p)\alpha(p)α(p), and Theorem 8 (a separate mission of this series) shows α~(p)→α∗\tilde\alpha(p)\to\alpha^*α~(p)→α∗ as p→1p\to1p→1. Theorem 9 makes that convergence quantitative and uniform: the guarantee is at least linear in ppp, so with p=1−εp=1-\varepsilonp=1−ε, an online set of size n=εNn=\varepsilon Nn=εN and O(n/ε)O(n/\varepsilon)O(n/ε) samples the rule earns α∗−O(ε)\alpha^*-O(\varepsilon)α∗−O(ε) of the expected maximum. This improves the sample complexity of the earlier learning-based results by a polynomial factor, in a model more general than theirs.

The theorem is proved in the paper; it has no machine-checked proof. The proof is elementary real analysis on explicit series and integrals, and one of its steps is a numerical check that the paper does not carry out in print. A formalization turns that numerical claim into a certified inequality and checks a chain of estimates in which one inequality sign is misprinted (see Formalization scope).

Difficulty

The statement is about two implicitly defined numbers. α~(p)\tilde\alpha(p)α~(p) has no closed form, and α∗\alpha^*α∗ is defined by an integral equation. Evaluating both numerically at finitely many ppp proves nothing for the remaining ppp, and the inequality is tight at p=1p=1p=1 (α~(1)=α∗\tilde\alpha(1)=\alpha^*α~(1)=α∗), so no uniform slack is available near p=1p=1p=1.

Concavity of α~\tilde\alphaα~ would give the result immediately, and the paper reports it numerically, but the authors were unable to prove it; the argument must avoid it. The remaining work handles infinite series whose terms depend on ppp through both pip^ipi and i(1−p)i(1-p)i(1−p): differentiating such a series term by term requires uniform control of the derivative series, comparing it with an integral needs a monotonicity argument, and one step needs a bound valid on an entire two-parameter region rather than at a point.

Formalization scope

  • Numbers, not processes. No probability, program or algorithm appears in Lean. Everything is a real-valued function on R\mathbb RR.
  • Predicates, not choice. α~(p)\tilde\alpha(p)α~(p) and α∗\alpha^*α∗ enter as IsAlphaTilde p a (with 0<a<10<a<10<a<1) and IsAlphaStar s (with 0<s<10<s<10<s<1). Statements quantify over every solution. Both exist, so the goal is not vacuous: existence of α~\tilde\alphaα~ is Lemma 7 (posed in the second mission of this series), and existence and uniqueness of α∗=1/β∗\alpha^*=1/\beta^*α∗=1/β∗ are posed as CorreaThreshold.Adaptive.beta_star_existsUnique (512ff915-7ec1-4d24-87b3-bc8adfee6bad).
  • Series. Every series is a Lean tsum over i : ℕ with the paper's index i≥1i\ge1i≥1 shifted to i + 1. For parameters in (0,1)(0,1)(0,1) all series are summable, so tsum is the true sum; summability is part of what solvers prove, never a hypothesis. Differentiability of aaa is likewise a conclusion (HasDerivAt), never assumed.
  • Total functions. Real.log 0 = 0 makes the integrands' values at y=0y=0y=0 equal their limits, so the interval integrals are the true integrals. Every division (1/p1/p1/p, 1/(ps)1/(ps)1/(ps)) is at a positive argument under the stated ranges, and every logarithm's argument is positive.
  • α∗≈0.745\alpha^*\approx0.745α∗≈0.745. The paper uses this approximation through the interval α∗∈[0.74,0.75]\alpha^*\in[0.74,0.75]α∗∈[0.74,0.75] of its numerical check. Milestones 9 and 10 carry that interval as a hypothesis; the goal does not. The lower bound α∗>0.745\alpha^*>0.745α∗>0.745 is posed as CorreaThreshold.Adaptive.inv_beta_star_gt (ce70487c-b155-4e47-9ce8-8348dc1b1645). The upper bound α∗≤0.75\alpha^*\le0.75α∗≤0.75 (numerically α∗≈0.74544\alpha^*\approx0.74544α∗≈0.74544) is posed nowhere and is welcome as a lemma.
  • A printed slip. The paper prints the conclusion of milestone 9 as "c(p)≥…c(p)\ge\dotsc(p)≥…". The surrounding argument requires and announces "≤\le≤", and the formal statement uses ≤\le≤.
  • Ruled-out trivializations. Fixing ppp, replacing α∗\alpha^*α∗ by the numeral 0.7450.7450.745 (a weaker statement, since 0.745<α∗0.745<\alpha^*0.745<α∗), stating aaa's monotonicity through deriv (which is 000 at non-differentiable points), or replacing α~\tilde\alphaα~ by a chosen value all change the theorem. None is used.
  • Reusable infrastructure. Welcome contributions include term-by-term differentiation of tsums under a dominating series, Riemann-sum comparisons for monotone integrands, a Chebyshev-type integral inequality for two decreasing functions, and certified interval arithmetic for a two-variable inequality such as milestone 8.

Selected references

  • J. Correa, A. Cristi, B. Epstein, J. A. Soto, Sample-Driven Optimal Stopping: From the Secretary Problem to the i.i.d. Prophet Inequality, arXiv:2011.06516v2, 2021 (journal version: Mathematics of Operations Research, 2024). https://arxiv.org/abs/2011.06516v2
  • J. Correa, P. Foncea, R. Hoeksma, T. Oosterwijk, T. Vredeveld, Posted Price Mechanisms for a Random Stream of Customers, ACM EC 2017; Mathematics of Operations Research 46(4), 2021. https://doi.org/10.1145/3033274.3085137
  • T. P. Hill, R. P. Kertz, Comparisons of stop rule and supremum expectations of i.i.d. random variables, Annals of Probability 10(2), 1982 (reference [26] of the paper). https://doi.org/10.1214/aop/1176993767
  • R. P. Kertz, Stop rule and supremum expectations of i.i.d. random variables: a complete comparison by conjugate duality, Journal of Multivariate Analysis 19, 1986 (reference [28] of the paper).
  • J. Correa, P. Dütting, F. Fischer, K. Schewior, Prophet Inequalities for I.I.D. Random Variables from an Unknown Distribution, ACM EC 2019. https://doi.org/10.1145/3328526.3329627
  • A. Rubinstein, J. Z. Wang, S. M. Weinberg, Optimal Single-Choice Prophet Inequalities from Samples, ITCS 2020. https://doi.org/10.4230/LIPIcs.ITCS.2020.60
13 thms2 active usersReviewed
Operations ResearchOptimizationProbability·Captain: mikedeng1

Sample-Driven Optimal Stopping: From the Secretary Problem to the i.i.d. Prophet Inequality II: The Optimal Competitive Ratio Tends to the i.i.d. Prophet Constant as p Tends to 1Research Paper

Motivation

Optimal stopping with samples sits between two classical problems. In the secretary problem a decision maker sees items in random order, knows nothing about their values, and must stop on one; the best guarantee is 1/e1/e1/e. In the i.i.d. prophet inequality the values are independent draws from a known distribution, and the best guarantee against the expected maximum is the constant α∗≈0.745\alpha^*\approx0.745α∗≈0.745: Hill and Kertz (1982) and Kertz (1986) showed that no stopping rule does better, and Correa, Foncea, Hoeksma, Oosterwijk and Vredeveld (2017) showed that it is achieved. Real decision makers usually have neither nothing nor everything: they have a history of past observations.

Correa, Cristi, Epstein and Soto (arXiv:2011.06516v2) model this as ppp-DOS (sample-driven optimal stopping): each of NNN items is independently placed in a history set with probability ppp, the decision maker sees the history first and then the remaining items online, and must stop on one online item. At p=0p=0p=0 this is the secretary problem; as p→1p\to1p→1 the history reveals the distribution and the problem approaches the i.i.d. prophet setting. This mission formalizes the paper's Theorem 8, which makes the second statement precise: the optimal guarantee tends to α∗\alpha^*α∗.

Timeline. Hill and Kertz (1982) compared stop-rule and supremum expectations for i.i.d. variables; Kertz (1986) completed the comparison, giving the worst-case constant ≈0.745\approx0.745≈0.745 through the integral equation used below; Correa et al. (2017) gave a matching algorithm. Kaplan, Naori and Raz (2020) studied the sample-driven model with a weaker bound for small ppp; Correa, Dütting, Fischer and Schewior (2019) and Rubinstein, Wang and Weinberg (2020) studied i.i.d. values with samples from an unknown distribution. The present paper (2020–2021) gives the exact limit program and Theorem 8.

Setting

Fix p∈(0,1)p\in(0,1)p∈(0,1). A stopping rule is a nonnegative function q(t,ℓ)q(t,\ell)q(t,ℓ) of a time t∈[p,1]t\in[p,1]t∈[p,1] and a rank ℓ≥1\ell\ge1ℓ≥1. For k≥1k\ge1k≥1 let

Fk(q)=∑ℓ=1k∫p1q(t,ℓ)∑j=ℓk(j−1ℓ−1)(1−t)j−ℓtℓ dt.F_k(q)=\sum_{\ell=1}^{k}\int_p^1 q(t,\ell)\sum_{j=\ell}^{k}\binom{j-1}{\ell-1}(1-t)^{j-\ell}t^{\ell}\,dt .Fk​(q)=ℓ=1∑k​∫p1​q(t,ℓ)j=ℓ∑k​(ℓ−1j−1​)(1−t)j−ℓtℓdt.

The limit program SDCLPp_pp​ maximizes α∈[0,1]\alpha\in[0,1]α∈[0,1] over pairs (q,α)(q,\alpha)(q,α) with

t q(t,ℓ)+∫pt∑s≥1q(τ,s) dτ≤1(t∈[p,1], ℓ≥1),α≤Fk(q)1−pk(k≥1).t\,q(t,\ell)+\int_p^t\sum_{s\ge1}q(\tau,s)\,d\tau\le1\quad(t\in[p,1],\ \ell\ge1),\qquad \alpha\le\frac{F_k(q)}{1-p^k}\quad(k\ge1).tq(t,ℓ)+∫pt​s≥1∑​q(τ,s)dτ≤1(t∈[p,1], ℓ≥1),α≤1−pkFk​(q)​(k≥1).

Its optimal value is α(p)\alpha(p)α(p). The paper obtains SDCLPp_pp​ as the limit N→∞N\to\inftyN→∞ of the linear programs that describe the best algorithm for ppp-DOS with adversarial values (§4.1–4.2); Theorem 8 is a statement about the program's value.

Two constants are defined by equations. α~(p)\tilde\alpha(p)α~(p) is the unique root in (0,1)(0,1)(0,1) of

ln⁡p+α~(1−p)2p=∑i=1∞ln⁡(1−α~+α~[(i+1)pi−ipi+1])i(i+1),(19)\ln p+\frac{\tilde\alpha(1-p)^2}{p}=\sum_{i=1}^{\infty}\frac{\ln\bigl(1-\tilde\alpha+\tilde\alpha[(i+1)p^i-ip^{i+1}]\bigr)}{i(i+1)},\qquad(19)lnp+pα~(1−p)2​=i=1∑∞​i(i+1)ln(1−α~+α~[(i+1)pi−ipi+1])​,(19)

and α∗\alpha^*α∗ is the solution of ∫01dyy(1−ln⁡y)+1/α∗−1=1\int_0^1\frac{dy}{y(1-\ln y)+1/\alpha^*-1}=1∫01​y(1−lny)+1/α∗−1dy​=1. A threshold rule (12) is given by times p=t1≤t2≤⋯≤1p=t_1\le t_2\le\cdots\le1p=t1​≤t2​≤⋯≤1 with Ti=∏j≤itjT_i=\prod_{j\le i}t_jTi​=∏j≤i​tj​: on [ti,ti+1)[t_i,t_{i+1})[ti​,ti+1​) it equals Ti/ti+1T_i/t^{i+1}Ti​/ti+1 for ranks ℓ≤i\ell\le iℓ≤i and 000 for larger ranks.

Formalization targets

Goal: Theorem 8

0≤α~(p)≤α(p)≤α∗(p∈(0,1)),lim⁡p→1−α~(p)=lim⁡p→1−α(p)=α∗.0\le\tilde\alpha(p)\le\alpha(p)\le\alpha^*\quad(p\in(0,1)),\qquad \lim_{p\to1^-}\tilde\alpha(p)=\lim_{p\to1^-}\alpha(p)=\alpha^*.0≤α~(p)≤α(p)≤α∗(p∈(0,1)),p→1−lim​α~(p)=p→1−lim​α(p)=α∗.

Milestones, in the order the proof uses them

  1. B.4: ∑ℓ=1j(j−1ℓ−1)(1−t)j−ℓtℓ=t\sum_{\ell=1}^{j}\binom{j-1}{\ell-1}(1-t)^{j-\ell}t^\ell=t∑ℓ=1j​(ℓ−1j−1​)(1−t)j−ℓtℓ=t.
  2. Lemma 4: a maximal α\alphaα satisfies α≥inf⁡k≥111−pk∑j≤k∫p1t q(t,j) dt\alpha\ge\inf_{k\ge1}\frac{1}{1-p^k}\sum_{j\le k}\int_p^1 t\,q(t,j)\,dtα≥infk≥1​1−pk1​∑j≤k​∫p1​tq(t,j)dt when qqq is non-increasing in ℓ\ellℓ.
  3. Lemma 5: for a threshold rule, the system "every term of that infimum equals α\alphaα" is equivalent to explicit equations (15)–(16).
  4. Lemma 6 (i), (ii): the times t1=pt_1=pt1​=p, t2=peα(1−p)2/pt_2=pe^{\alpha(1-p)^2/p}t2​=peα(1−p)2/p, (tk/tk+1)k−1=γk/γk−1(t_k/t_{k+1})^{k-1}=\gamma_k/\gamma_{k-1}(tk​/tk+1​)k−1=γk​/γk−1​ increase, and their limit is at most 111 exactly under condition (18).
  5. B.6: Ti/tii−1=pγi−1T_i/t_i^{i-1}=p\gamma_{i-1}Ti​/tii−1​=pγi−1​ and μk=p(1−α+αpk−2)/(k−2)\mu_k=p(1-\alpha+\alpha p^{k-2})/(k-2)μk​=p(1−α+αpk−2)/(k−2).
  6. Lemma 6 (iii): under (18) the threshold rule is feasible with value α\alphaα.
  7. Lemma 7: (19) has a unique root, continuous in ppp.
  8. B.8: the ratio h(p,η)h(p,\eta)h(p,η) of the two sides of (19) tends to ∫01dyy(1−ln⁡y)+1/η−1\int_0^1\frac{dy}{y(1-\ln y)+1/\eta-1}∫01​y(1−lny)+1/η−1dy​ as p→1p\to1p→1.

Significance

The result. Theorem 8 shows that sample access interpolates continuously between the secretary and prophet worlds and that, with almost full information, no more than the known-distribution guarantee α∗\alpha^*α∗ is lost or gained. The explicit rule behind α~(p)\tilde\alpha(p)α~(p) is a concrete threshold algorithm, and the companion Theorem 9 of the paper (α~(p)≥α∗p\tilde\alpha(p)\ge\alpha^*pα~(p)≥α∗p, a separate mission) turns it into sample-complexity bounds: O(n/ε)O(n/\varepsilon)O(n/ε) samples suffice for α∗−O(ε)\alpha^*-O(\varepsilon)α∗−O(ε).

Formalizing it. The result is proved on paper; no part of it is machine-checked. A formal proof contributes a verified treatment of an infinite-dimensional linear program over L1([p,1]×N)L^1([p,1]\times\mathbb N)L1([p,1]×N), of series defined through implicit equations, and of a Riemann-sum limit obtained by l'Hôpital's rule. One clause, α(p)≤α∗\alpha(p)\le\alpha^*α(p)≤α∗, is not proved in the paper: it is imported from the i.i.d. prophet inequality literature via the interpretation of α(p)\alpha(p)α(p) as a competitive ratio. A formal proof of that clause directly from SDCLPp_pp​ would be new.

Difficulty

The lower bound α~(p)≤α(p)\tilde\alpha(p)\le\alpha(p)α~(p)≤α(p) needs an explicit feasible point of an infinite program; checking feasibility of the threshold rule requires exact telescoping of series with products of the times tkt_ktk​, which are defined recursively through fractional powers. The limit α~(p)→α∗\tilde\alpha(p)\to\alpha^*α~(p)→α∗ is a 0/00/00/0 limit of infinite series whose terms change scale as p→1p\to1p→1: every individual term tends to zero, so termwise passage to the limit gives no information, and the integral in the defining equation of α∗\alpha^*α∗ appears only in an aggregate limit of the whole series. The upper bound α(p)≤α∗\alpha(p)\le\alpha^*α(p)≤α∗ cannot come from evaluating any single solution: it is a statement about every feasible qqq, and the paper obtains it only through an external argument.

Formalization scope

  • A stopping rule is q : ℝ → ℕ → ℝ; ranks are 1-based (values at rank 000 are never used), and constraints are imposed pointwise on [p,1][p,1][p,1] as printed. The integral of the series in (10) is a lower Lebesgue integral of an [0,∞][0,\infty][0,∞]-valued series, so it cannot collapse to a junk value; each q(⋅,ℓ)q(\cdot,\ell)q(⋅,ℓ) is required integrable on [p,1][p,1][p,1].
  • α(p)\alpha(p)α(p) is sSup of the set of feasible α\alphaα; it contains 000 and is bounded by 111, so it is the true supremum (checked in a sorry-free verification file). The program ranges over all feasible qqq, never only threshold rules.
  • (11) is quantified over k≥1k\ge1k≥1 only, so 1−pk≠01-p^k\neq01−pk=0.
  • Threshold rules use the half-open intervals [ti,ti+1)[t_i,t_{i+1})[ti​,ti+1​) of (7); (12) prints closed intervals, which overlap at the tit_iti​.
  • The series in (18), (19), (26) and μk\mu_kμk​ are written with the summation index shifted to start at 000; with p,α∈(0,1)p,\alpha\in(0,1)p,α∈(0,1) every logarithm's argument lies in [1−α,1][1-\alpha,1][1−α,1], so they converge absolutely and tsum is the true sum.
  • Lemma 6's recursion is tk+1=tk(γk−1/γk)1/(k−1)t_{k+1}=t_k(\gamma_{k-1}/\gamma_k)^{1/(k-1)}tk+1​=tk​(γk−1​/γk​)1/(k−1) for k≥2k\ge2k≥2, the unique positive solution of (17).
  • α~\tilde\alphaα~ and α∗\alpha^*α∗ are predicates (IsAlphaTilde, IsAlphaStar), not chosen functions; the goal holds for every root selection. Existence and uniqueness of α∗\alpha^*α∗ (with β=1/α∗\beta=1/\alpha^*β=1/α∗) is already posed as the open item CorreaThreshold.Adaptive.beta_star_existsUnique and is not posed again.
  • "p→1p\to1p→1" is the one-sided filter 𝓝[<] 1.
  • Lemma 6 (iii) carries hypothesis (18), which the paper states in the sentence after the lemma; without it the claim is false.

Trivializing formalizations are ruled out: replacing α(p)\alpha(p)α(p) by α~(p)\tilde\alpha(p)α~(p) or by the value of a truncated program, fixing ppp, restricting qqq to threshold rules in the definition of α(p)\alpha(p)α(p), or replacing α∗\alpha^*α∗ by 0.7450.7450.745 each changes the theorem and is not done.

A complete development needs: binomial identities, interval integrals of t−it^{-i}t−i and of piecewise-defined functions, real powers and logarithms of recursively defined sequences, summability of series in ℓ1\ell^1ℓ1, continuity of the root of a monotone family of equations, and limits of Riemann-type sums on (0,1](0,1](0,1]. The last two are reusable beyond this mission. Proofs of individual milestones are welcome independently of the goal.

Selected references

  • J. Correa, A. Cristi, B. Epstein, J. A. Soto, Sample-Driven Optimal Stopping: From the Secretary Problem to the i.i.d. Prophet Inequality, arXiv:2011.06516v2, 2021. https://arxiv.org/abs/2011.06516v2
  • T. P. Hill, R. P. Kertz, Comparisons of stop rule and supremum expectations of i.i.d. random variables, The Annals of Probability 10(2), 336–345, 1982 (reference [26] of the paper).
  • R. P. Kertz, Stop rule and supremum expectations of i.i.d. random variables: a complete comparison by conjugate duality, Journal of Multivariate Analysis 19, 88–112, 1986 (reference [28]).
  • J. Correa, P. Foncea, R. Hoeksma, T. Oosterwijk, T. Vredeveld, Posted price mechanisms for a random stream of customers, ACM EC 2017 (reference [17]).
  • H. Kaplan, D. Naori, D. Raz, Competitive analysis with a sample and the secretary problem, SODA 2020 (reference [27]).
  • J. Correa, P. Dütting, F. Fischer, K. Schewior, Prophet inequalities for i.i.d. random variables from an unknown distribution, ACM EC 2019 (reference [15]).
  • A. Rubinstein, J. Z. Wang, S. M. Weinberg, Optimal single-choice prophet inequalities from samples, ITCS 2020 (reference [40]).
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Algorithmic Game TheoryMechanism DesignOperations Research·Captain: mikedeng1

Mechanism Design under Approximate Incentive Compatibility 2: Under Local α-Power Envelopes, ε-IC Mechanisms Gain at Most Õ(ε^(α/(2α−1))) RevenueResearch Paper

Motivation

Classical mechanism design assumes that agents optimize exactly: a buyer facing a menu picks the option that maximizes his utility, however small the advantage over the next-best option. In many settings this is implausible. Agents may face cognitive or computational costs, or the designer may only be able to certify incentives approximately, as in algorithmic mechanism design where exact incentive compatibility is replaced by ε-incentive compatibility: no deviation gains more than ε\varepsilonε.

Balseiro, Besbes and Castro (arXiv:2103.03403v2; Operations Research, 2024) ask how much a revenue-maximizing seller can gain when the buyer is only an ε\varepsilonε-optimizer, in the most basic setting: one seller, one item, one buyer. Without the relaxation the answer is classical: by Myerson (1981) and Riley–Zeckhauser (1983) the optimal mechanism is a posted price. The rounding argument usually attributed to Nisan shows that the gain from the relaxation is O(ε1/2)O(\varepsilon^{1/2})O(ε1/2) for every distribution. This mission formalizes the paper's first main theorem, which shows that for regular instances the gain is much smaller and is determined by the local curvature of the revenue curve at the optimal price.

Setting

The buyer's value vvv has a density fff on S=[0,vˉ]S=[0,\bar v]S=[0,vˉ], with vˉ>0\bar v>0vˉ>0, f≥0f\ge 0f≥0, f=0f=0f=0 off SSS and ∫0vˉf=1\int_0^{\bar v}f=1∫0vˉ​f=1. Assumption 1 requires in addition that fff has bounded variation on SSS. Write F(v)=∫0vfF(v)=\int_0^v fF(v)=∫0v​f, Fˉ=1−F\bar F=1-FFˉ=1−F, the revenue function R(v)=vFˉ(v)R(v)=v\bar F(v)R(v)=vFˉ(v) (the revenue of a posted price vvv), and R˙(v)=Fˉ(v)−vf(v)\dot R(v)=\bar F(v)-vf(v)R˙(v)=Fˉ(v)−vf(v).

A mechanism m=(x,t)m=(x,t)m=(x,t) assigns to every report v∈Sv\in Sv∈S an allocation probability x(v)∈[0,1]x(v)\in[0,1]x(v)∈[0,1] and a payment t(v)∈Rt(v)\in\mathbb Rt(v)∈R. It is individually rational (IR) if vx(v)−t(v)≥0v x(v)-t(v)\ge 0vx(v)−t(v)≥0 for all v∈Sv\in Sv∈S, and ε-incentive compatible (ICε_\varepsilonε​) if

v x(v)−t(v) ≥ v x(v′)−t(v′)−ε∀v,v′∈S.v\,x(v)-t(v)\ \ge\ v\,x(v')-t(v')-\varepsilon\qquad\forall v,v'\in S .vx(v)−t(v) ≥ vx(v′)−t(v′)−ε∀v,v′∈S.

M(ε)\mathcal M(\varepsilon)M(ε) is the set of such mechanisms, Π(m)=∫0vˉt(v)f(v) dv\Pi(m)=\int_0^{\bar v}t(v)f(v)\,dvΠ(m)=∫0vˉ​t(v)f(v)dv the expected revenue, and Π⋆(M(ε))=sup⁡m∈M(ε)Π(m)\Pi^\star(\mathcal M(\varepsilon))=\sup_{m\in\mathcal M(\varepsilon)}\Pi(m)Π⋆(M(ε))=supm∈M(ε)​Π(m).

Definition 1 (local α-power envelopes). RRR has a unique maximizer p⋆∈(0,vˉ)p^\star\in(0,\bar v)p⋆∈(0,vˉ) on SSS, and there are α>1\alpha>1α>1, κL,κU>0\kappa_L,\kappa_U>0κL​,κU​>0 and a neighborhood Nℓ=(p⋆−ℓ,p⋆+ℓ)⊂(0,vˉ)\mathcal N_\ell=(p^\star-\ell,p^\star+\ell)\subset(0,\bar v)Nℓ​=(p⋆−ℓ,p⋆+ℓ)⊂(0,vˉ) with

κLα∣v−p⋆∣α≤(p⋆−v)R˙(v)≤κUα∣v−p⋆∣α∀v∈Nℓ.\kappa_L\alpha|v-p^\star|^\alpha\le(p^\star-v)\dot R(v)\le\kappa_U\alpha|v-p^\star|^\alpha\qquad\forall v\in\mathcal N_\ell .κL​α∣v−p⋆∣α≤(p⋆−v)R˙(v)≤κU​α∣v−p⋆∣α∀v∈Nℓ​.

For the uniform distribution on [0,1][0,1][0,1], p⋆=1/2p^\star=1/2p⋆=1/2 and α=2\alpha=2α=2.

Formalization targets

Goal: Theorem 1 (p. 16)

Under Assumption 1, local α\alphaα-power envelopes at p⋆p^\starp⋆ and inf⁡p∈S∖Nℓ∣R˙(p)∣>0\inf_{p\in S\setminus\mathcal N_\ell}|\dot R(p)|>0infp∈S∖Nℓ​​∣R˙(p)∣>0,

Π⋆(M(ε))−Π⋆(M(0))=O~(εα/(2α−1)),\Pi^\star(\mathcal M(\varepsilon))-\Pi^\star(\mathcal M(0))=\tilde O\big(\varepsilon^{\alpha/(2\alpha-1)}\big),Π⋆(M(ε))−Π⋆(M(0))=O~(εα/(2α−1)),

where O~\tilde OO~ allows a factor log⁡(1/ε)\log(1/\varepsilon)log(1/ε) and the constants depend on the instance but not on ε\varepsilonε.

Milestones

The paper's argument passes through the following stated results, in attack order:

  1. M(ε)⊆Mpath(ε)\mathcal M(\varepsilon)\subseteq\mathcal M_{\text{path}}(\varepsilon)M(ε)⊆Mpath​(ε) for the relaxation that keeps IR on [0,μ][0,\mu][0,μ] and IC only along a path v↦v⋆(v)v\mapsto v^\star(v)v↦v⋆(v) (p. 17);
  2. Lemma 1 (weak duality): Π(m)≤Φ1(λ)+Φ2(λ)\Pi(m)\le\Phi_1(\lambda)+\Phi_2(\lambda)Π(m)≤Φ1​(λ)+Φ2​(λ) for every m∈Mpath(ε)m\in\mathcal M_{\text{path}}(\varepsilon)m∈Mpath​(ε) and every dual-feasible λ\lambdaλ;
  3. Lemma 2: an explicit dual solution λ⋆(v)=ddv∑j≤kF(wj(v))\lambda^\star(v)=\frac{d}{dv}\sum_{j\le k}F(w^j(v))λ⋆(v)=dvd​∑j≤k​F(wj(v)) on the kkk-th step, where www inverts v⋆v^\starv⋆;
  4. Lemma 3: Φ1(λ⋆)≤CεK\Phi_1(\lambda^\star)\le C\varepsilon KΦ1​(λ⋆)≤CεK, KKK the number of steps;
  5. Lemma 4: ∫xvˉΔ≤R(x)+2(w(x)−x)\int_x^{\bar v}\Delta\le R(x)+2(w(x)-x)∫xvˉ​Δ≤R(x)+2(w(x)−x) when the dual virtual value Δ\DeltaΔ is nonnegative on [x,ν0][x,\nu_0][x,ν0​];
  6. Proposition 2: for the piecewise-linear path of eq. (9), K=O(log⁡(1/ε)/εβ)K=O(\log(1/\varepsilon)/\varepsilon^\beta)K=O(log(1/ε)/εβ);
  7. the sandwich vf−Fˉ−CLεβ≤Δ≤vf−Fˉ+CUεβvf-\bar F-C_L\varepsilon^\beta\le\Delta\le vf-\bar F+C_U\varepsilon^\betavf−Fˉ−CL​εβ≤Δ≤vf−Fˉ+CU​εβ a.e. on [p⋆,ν0][p^\star,\nu_0][p⋆,ν0​] (p. 48);
  8. Δ≤−R˙+Cεβ\Delta\le-\dot R+C\varepsilon^\betaΔ≤−R˙+Cεβ a.e. on [0,p⋆][0,p^\star][0,p⋆] (pp. 51–52).

Significance

Theorem 1 is an instance-dependent impossibility result: no ε\varepsilonε-IC mechanism can extract more than O~(εα/(2α−1))\tilde O(\varepsilon^{\alpha/(2\alpha-1)})O~(εα/(2α−1)) beyond the optimal posted price. Since α/(2α−1)>1/2\alpha/(2\alpha-1)>1/2α/(2α−1)>1/2 for every α>1\alpha>1α>1, it strictly improves the universal O(ε1/2)O(\varepsilon^{1/2})O(ε1/2) bound for these distributions; for α=2\alpha=2α=2 (a revenue curve with nonzero second derivative at p⋆p^\starp⋆) the rate is ε2/3\varepsilon^{2/3}ε2/3. Together with Theorem 3 of the same paper, a matching Ω(εα/(2α−1))\Omega(\varepsilon^{\alpha/(2\alpha-1)})Ω(εα/(2α−1)) lower bound by a randomized mechanism, it identifies the exact rate up to the logarithm. The authors conjecture that the logarithmic factor can be removed.

The result is proved in the paper; no machine-checked proof of it or of any of its lemmas exists. A formalization would check an appendix argument of several pages of explicit estimates, and would produce reusable components: a weak duality theorem for a mechanism-design program over a path of incentive constraints, an explicit solution of the functional equation λ(v)=f(v)+w˙(v)λ(w(v))\lambda(v)=f(v)+\dot w(v)\lambda(w(v))λ(v)=f(v)+w˙(v)λ(w(v)) by iterates of www, and estimates of iterated piecewise-linear maps.

Difficulty

The obvious approach is to bound the gain by perturbing the optimal posted price, which yields only the ε1/2\varepsilon^{1/2}ε1/2 rate of the rounding argument. Getting the exponent α/(2α−1)\alpha/(2\alpha-1)α/(2α−1) requires an upper bound that is tight to first order, i.e. a nearly optimal dual certificate for an infinite-dimensional program. The dual depends on the choice of path: the paper's analysis shows that a parallel shift w(x)=x+δw(x)=x+\deltaw(x)=x+δ cannot beat ε1/2\varepsilon^{1/2}ε1/2, so the path must approach the diagonal near p⋆p^\starp⋆ while keeping the number of steps KKK controlled. The estimates for Δ\DeltaΔ in milestones 7–8 require tracking λ⋆(w(v))\lambda^\star(w(v))λ⋆(w(v)) through K=O(log⁡(1/ε)/εβ)K=O(\log(1/\varepsilon)/\varepsilon^\beta)K=O(log(1/ε)/εβ) iterations of www, with a bounded-variation (possibly discontinuous) density. Measure-theoretic details absent from the paper also have to be supplied: changes of variables along a Lipschitz path, almost-everywhere differentiability of iterated compositions, and integrability of the dual variable.

Formalization scope

The Lean development lives in namespace ApproxIC.UpperBound. Every function of the value is a total function ℝ → ℝ and every condition quantifies over SSS only. Committed conventions:

  • FFF is the interval integral of fff; R˙\dot RR˙ is the explicit expression Fˉ(v)−vf(v)\bar F(v)-vf(v)Fˉ(v)−vf(v), not a derivative of RRR.
  • Mechanisms are required to be measurable (disclosed: Ev[t(v)]\mathbb E_v[t(v)]Ev​[t(v)] presumes it). Π⋆\Pi^\starΠ⋆ is an sSup of the revenue image, which is nonempty and bounded above by vˉ\bar vvˉ.
  • The goal is stated as ∀m∈M(ε), Π(m)−Π⋆(M(0))≤Cεα/(2α−1)log⁡(1/ε)\forall m\in\mathcal M(\varepsilon),\ \Pi(m)-\Pi^\star(\mathcal M(0))\le C\varepsilon^{\alpha/(2\alpha-1)}\log(1/\varepsilon)∀m∈M(ε), Π(m)−Π⋆(M(0))≤Cεα/(2α−1)log(1/ε) for all ε∈(0,ε0]\varepsilon\in(0,\varepsilon_0]ε∈(0,ε0​], with C,ε0C,\varepsilon_0C,ε0​ chosen after the instance and before ε\varepsilonε. The infimum hypothesis on ∣R˙∣|\dot R|∣R˙∣ ranges over S∖NℓS\setminus\mathcal N_\ellS∖Nℓ​.
  • Definition 1's constants are parameters of a predicate LocalPowerEnvelope.
  • Paths carry an added, disclosed assumption: www is Lipschitz on [0,ν0][0,\nu_0][0,ν0​] (eq. (9)'s www is). w˙\dot ww˙ is deriv w.
  • The thresholds are N\mathbb NN-indexed with index 000 equal to vˉ\bar vvˉ, so the paper's νk\nu_kνk​ is index k+1k+1k+1.
  • Lemma 1's printed sign (v−w(v))(v-w(v))(v−w(v)) in Φ2\Phi_2Φ2​ is read as (w(v)−v)(w(v)-v)(w(v)−v), as in its proof and in Lemma 4. Lemma 4's printed "Φ2(λ)=∫xvˉΔ\Phi_2(\lambda)=\int_x^{\bar v}\DeltaΦ2​(λ)=∫xvˉ​Δ" is read as ∫xvˉΔ+=∫xvˉΔ\int_x^{\bar v}\Delta^+=\int_x^{\bar v}\Delta∫xvˉ​Δ+=∫xvˉ​Δ. Lemmas 3 and 4 are stated for Lemma 2's explicit λ⋆\lambda^\starλ⋆.

The goal imports only the model file; paths, the dual and eq. (9) appear only in the milestones. A formalization in which O~\tilde OO~'s constants are chosen after ε\varepsilonε, Π⋆(M(0))\Pi^\star(\mathcal M(0))Π⋆(M(0)) is replaced by a constant, or the revenue integral is allowed to vanish on non-measurable mechanisms is not this theorem and is ruled out by the statement.

A complete development needs interval integrals and the fundamental theorem of calculus for absolutely continuous functions, change of variables along monotone Lipschitz maps, BoundedVariationOn, real powers and logarithms, and iterates Nat.iterate. The duality lemma and the functional-equation solution are reusable for other single-agent screening problems with relaxed incentive constraints. Contributions to any milestone, and alternative proofs of the goal that bypass the path construction, are welcome.

Selected references

  • S. R. Balseiro, O. Besbes, F. Castro, Mechanism Design under Approximate Incentive Compatibility, arXiv:2103.03403v2, 2022; Operations Research, 2024. https://arxiv.org/abs/2103.03403
  • R. B. Myerson, Optimal Auction Design, Mathematics of Operations Research 6(1), 1981. https://doi.org/10.1287/moor.6.1.58
  • J. Riley, R. Zeckhauser, Optimal Selling Strategies: When to Haggle, When to Hold Firm, Quarterly Journal of Economics 98(2), 1983. https://doi.org/10.2307/1885622
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Control TheoryEconomicsOperations Research·Captain: mikedeng1

Punish Underperformance with Suspension: Optimal Dynamic Contracts in the Presence of Switching Cost II: Condition 2, High Switching Cost, Not-Hiring Value Functions Meet the Optimality ConditionsResearch Paper

Motivation

Firms that outsource work to an agent whose effort they cannot observe often punish poor performance by suspending the relationship for a while, even though restarting costs money: a new set-up, re-training, re-mobilisation. Cao, Sun and Tian (Management Science, 2024) study this trade-off in a continuous-time principal–agent model with Poisson arrivals and a fixed switching cost paid every time work (re)starts. They characterise the optimal dynamic contract in three regimes: never hire the agent, hire and keep the agent working forever, or a control-band contract with suspension episodes of fixed length. The model extends the Poisson-arrival contracting framework of Sun and Tian (2018) by adding the switching cost.

The proof follows a guess-and-verify pattern. A stochastic verification theorem (Theorem 1 of the paper) turns any pair of functions satisfying a system of quasi-variational inequalities into an upper bound on the principal's value. Propositions 2–7 then supply such a pair in each parameter region. This mission covers one region: the agent is much more impatient than the principal (Condition 2) and the switching cost is high.

Setting

A principal earns revenue RRR per arrival of a Poisson process. Without the agent's effort the arrival rate is μ‾≥0\underline\mu\ge0μ​≥0; with effort it is μ>μ‾\mu>\underline\muμ>μ​, and effort costs the agent b>0b>0b>0 per unit of time. While the agent works, the principal's total cost rate is c≥bc\ge bc≥b. Each time work starts or restarts, the principal pays a switching cost K>0K>0K>0. The principal discounts at rate rrr and the agent at rate ρ\rhoρ, with 0<r≤ρ0<r\le\rho0<r≤ρ. Write Δμ=μ−μ‾\Delta\mu=\mu-\underline\muΔμ=μ−μ​. Assumption 1 is RΔμ>cR\Delta\mu>cRΔμ>c.

The derived constants are

β=bΔμ,wˉ=βμρ,v‾=μ‾Rr,Vˉ=Rμ−c−(ρ−r)wˉr,Kˉ2=Vˉ−v‾−wˉ.\beta=\frac{b}{\Delta\mu},\qquad \bar w=\frac{\beta\mu}{\rho},\qquad \underline v=\frac{\underline\mu R}{r},\qquad \bar V=\frac{R\mu-c-(\rho-r)\bar w}{r},\qquad \bar K_2=\bar V-\underline v-\bar w .β=Δμb​,wˉ=ρβμ​,v​=rμ​R​,Vˉ=rRμ−c−(ρ−r)wˉ​,Kˉ2​=Vˉ−v​−wˉ.

The variable w≥0w\ge0w≥0 is the agent's promised utility. The revenue threshold is

R^=[cb+(ρ−r)μΔμ(ρ−r−μ)⋅ρ−μρ]β.\hat R=\Big[\frac cb+\frac{(\rho-r)\mu}{\Delta\mu(\rho-r-\mu)}\cdot\frac{\rho-\mu}{\rho}\Big]\beta .R^=[bc​+Δμ(ρ−r−μ)(ρ−r)μ​⋅ρρ−μ​]β.

Condition 2 is: μ<ρ−r\mu<\rho-rμ<ρ−r and R≥R^R\ge\hat RR≥R^.

For a function fff on R+\mathbb R_+R+​ with left derivative f′f'f′, the working-state operator and the suspension-state operator are

(AIf)(w)=(μ+r)f(w)−μf(w+β)+ρ(wˉ−w)f′(w)−(μR−c)+(ρ−r)w,(\mathcal A_I f)(w)=(\mu+r)f(w)-\mu f(w+\beta)+\rho(\bar w-w)f'(w)-(\mu R-c)+(\rho-r)w,(AI​f)(w)=(μ+r)f(w)−μf(w+β)+ρ(wˉ−w)f′(w)−(μR−c)+(ρ−r)w, (A∅f)(w)=rf(w)−ρwf′(w)+(ρ−r)w−Rμ‾.(\mathcal A_\emptyset f)(w)=rf(w)-\rho wf'(w)+(\rho-r)w-R\underline\mu .(A∅​f)(w)=rf(w)−ρwf′(w)+(ρ−r)w−Rμ​.

The first is a delay-differential operator: it evaluates fff at w+βw+\betaw+β. A pair (VI,V∅)(V_I,V_\emptyset)(VI​,V∅​) satisfies the optimality condition (20)–(22) if

(AIVI)(w)≥0,(A∅V∅)(w)≥0,0≤VI(w)−V∅(w)≤K,VI(0)≥v‾, V∅(0)≥v‾.(\mathcal A_IV_I)(w)\ge0,\quad(\mathcal A_\emptyset V_\emptyset)(w)\ge0,\qquad 0\le V_I(w)-V_\emptyset(w)\le K,\qquad V_I(0)\ge\underline v,\ V_\emptyset(0)\ge\underline v .(AI​VI​)(w)≥0,(A∅​V∅​)(w)≥0,0≤VI​(w)−V∅​(w)≤K,VI​(0)≥v​, V∅​(0)≥v​.

Formalization targets

Goal: Proposition 4

Under Condition 2, let VIV_IVI​ be the line from v‾\underline vv​ at w=0w=0w=0 to Vˉ\bar VVˉ at w=wˉw=\bar ww=wˉ, and let VIV_IVI​ be constant Vˉ\bar VVˉ beyond wˉ\bar wwˉ (display (31)). Then

K>Vˉ−v‾ ⟹ (VI, V∅≡v‾) satisfies (20)–(22),K>\bar V-\underline v\ \Longrightarrow\ (V_I,\ V_\emptyset\equiv\underline v)\ \text{satisfies (20)–(22)},K>Vˉ−v​ ⟹ (VI​, V∅​≡v​) satisfies (20)–(22), Kˉ2<K≤Vˉ−v‾ ⟹ (VI, V∅) satisfies (20)–(22),\bar K_2<K\le\bar V-\underline v\ \Longrightarrow\ (V_I,\ V_\emptyset)\ \text{satisfies (20)–(22)},Kˉ2​<K≤Vˉ−v​ ⟹ (VI​, V∅​) satisfies (20)–(22),

where in the second case V∅V_\emptysetV∅​ is the line from v‾\underline vv​ to Vˉ−K\bar V-KVˉ−K on [0,wˉ][0,\bar w][0,wˉ], constant Vˉ−K\bar V-KVˉ−K beyond (display (32)).

Milestones

  1. Lemma EC.2(vi), second claim: if ρ>r+μ\rho>r+\muρ>r+μ, then Vˉ−ρ−rρ−r−μwˉ≥v‾\bar V-\frac{\rho-r}{\rho-r-\mu}\bar w\ge\underline vVˉ−ρ−r−μρ−r​wˉ≥v​ if and only if R≥R^R\ge\hat RR≥R^.
  2. Proposition 4, first part: the case K>Vˉ−v‾K>\bar V-\underline vK>Vˉ−v​.
  3. Proposition 4, second part: the case Kˉ2<K≤Vˉ−v‾\bar K_2<K\le\bar V-\underline vKˉ2​<K≤Vˉ−v​.

Significance

Through the paper's verification theorem, Proposition 4 yields the "not hiring" half of the main Theorem 2 in the Condition 2 regime. If K≥Kˉ2K\ge\bar K_2K≥Kˉ2​, the principal's value is at most v‾\underline vv​, so it is optimal never to engage the agent (Theorem 3). The threshold Kˉ2=Vˉ−v‾−wˉ\bar K_2=\bar V-\underline v-\bar wKˉ2​=Vˉ−v​−wˉ is the switching cost above which the value of hiring, net of the set-up cost and of the agent's promised rent, falls below the outside value. Together with the companion missions of this series (Condition 1 with high cost, Condition 2 with medium cost, and the low-cost control-band regime), this result completes the partition of the parameter space behind Theorem 2.

The result is proved in the paper and has no machine-checked proof yet. This mission states the analytic certificate of the guess-and-verify argument, not the contract-optimality theorem. The contribution it asks for is a formal proof that these explicit functions satisfy the quasi-variational inequalities, including the left-derivative behaviour at the kink w=wˉw=\bar ww=wˉ and the algebra that links Condition 2 to the sign of AIVI\mathcal A_IV_IAI​VI​.

Difficulty

The functions are piecewise linear, so the difficulty is not analytic depth but bookkeeping that is easy to get wrong:

  • The operator AI\mathcal A_IAI​ is non-local. It evaluates VIV_IVI​ at w+βw+\betaw+β, and which branch of (31) applies there depends on how wˉ\bar wwˉ compares with β\betaβ, which Condition 2 settles.
  • At the kink w=wˉw=\bar ww=wˉ the functions are not differentiable, so the left-derivative convention must be used explicitly.
  • The sign of AIVI\mathcal A_IV_IAI​VI​ on [0,wˉ][0,\bar w][0,wˉ] reduces to an inequality between Vˉ\bar VVˉ, v‾\underline vv​ and wˉ\bar wwˉ, and showing that this inequality is the revenue condition R≥R^R\ge\hat RR≥R^ requires unfolding (8)–(10) and (28).

The naive check, that AIVI\mathcal A_IV_IAI​VI​ vanishes or is positive because VIV_IVI​ is "close to" a solution of the delay equation, does not work: VIV_IVI​ is not a solution of (25), and the inequality is strict in general.

Formalization scope

All parameters are real numbers in one structure Params. Its predicate Standing collects the paper's standing assumptions: 0≤μ‾<μ0\le\underline\mu<\mu0≤μ​<μ, 0<b≤c0<b\le c0<b≤c, K>0K>0K>0, 0<r≤ρ0<r\le\rho0<r≤ρ and RΔμ>cR\Delta\mu>cRΔμ>c. Two of these are added to the page and disclosed: μ‾≥0\underline\mu\ge0μ​≥0, since it is an arrival rate, and b>0b>0b>0, since (31)–(32) divide by wˉ=βμ/ρ\bar w=\beta\mu/\rhowˉ=βμ/ρ.

Functions are ℝ → ℝ, and every condition is quantified over w≥0w\ge0w≥0 only. The derivative in AI\mathcal A_IAI​ and A∅\mathcal A_\emptysetA∅​ is the left derivative derivWithin f (Set.Iic w) w, as the paper prescribes on p. 15. Inequality (20) is required for w>0w>0w>0: on R+\mathbb R_+R+​ the left derivative at 000 does not exist. Inequalities (21) and (22) are required exactly as printed. "Satisfy the optimality condition (20)–(22)" means exactly these three conditions; the paper's Theorem 1 additionally asks for monotonicity and concavity, but Proposition 4 does not claim them and they are not added.

The threshold R^\hat RR^ is the printed formula. Its denominator ρ−r−μ\rho-r-\muρ−r−μ is positive under Condition 2, so Lean's convention x/0=0x/0=0x/0=0 never applies there.

None of the conditions is weakened: (21) keeps both bounds, (22) is kept, and the operators are not pre-simplified with the closed form of Vˉ\bar VVˉ. A formal proof therefore has to carry out the sign computation itself. The stochastic contract model (Poisson point processes, promise keeping, incentive compatibility), the verification Theorem 1 and the optimality Theorems 2–3 are not formalized.

Two hat symbols elsewhere in the paper are distinct objects from those used here: w^\hat{\mathrm w}w^ of Lemma 3 and the bold w^\hat{\mathbf w}w^ of Proposition 6. Neither appears in this mission. Proofs of the milestones, and proofs of the goal that use them, are welcome.

Selected references

  • P. Cao, P. Sun, F. Tian, Punish Underperformance with Suspension: Optimal Dynamic Contracts in the Presence of Switching Cost, Management Science, 2024. https://doi.org/10.1287/mnsc.2023.4845
  • P. Sun, F. Tian, Optimal Contract to Induce Continued Effort, Management Science 64(9), 4193–4217, 2018. https://doi.org/10.1287/mnsc.2017.2795
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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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Operations ResearchProbabilityStatistics·Captain: mikedeng1

Scores for Multivariate Distributions and Level Sets I: The L² Scoring Rules S and S′ Are Proper, With Divergence the h-Weighted L² Distance Between f_X ∗ w and f_Y ∗ wResearch Paper

Why scoring rules for multivariate distributions

A probabilistic forecast issues a whole distribution PXP_XPX​ for an uncertain quantity Y∈RdY\in\mathbb R^dY∈Rd rather than a single number: wind and wave heights at several sites, demand for several products, the joint returns of several assets. Forecasts of this kind are compared and estimated with a scoring rule S(PX,y)S(P_X,y)S(PX​,y), a number assigned to the forecast once the realization yyy is observed. A scoring rule is proper if a forecaster who knows the true distribution PYP_YPY​ minimizes the expected score by reporting it, and strictly proper if PYP_YPY​ is the only minimizer (Gneiting and Raftery 2007). Properness is what makes a score usable for model ranking and for M-estimation: an improper score rewards systematic misreporting.

For univariate distributions the continuous ranked probability score (CRPS) and the quadratic score are standard. In several dimensions the choices are thinner: the quadratic score needs a density and is sensitive to its spikes, and the energy score and the multivariate CRPS (MCRPS) were treated as separate constructions. Meng, Taylor, Ben Taieb and Li (arXiv:2002.09578v6, Operations Research, 2025) give one family, the L² scoring rules, which contains the quadratic score, the CRPS and the MCRPS as special cases and produces new ones, such as a score based on lower partial moments. Their Theorem 1 says these rules are proper. This mission formalizes that theorem.

Setting

Work on Rd\mathbb R^dRd with Lebesgue measure Ld\mathcal L^dLd and the componentwise order. A distribution is a probability measure PPP on Rd\mathbb R^dRd; the paper writes it through a generalized density fPf_PfP​ (a PDF, a PMF or a mixture), and every integral ∫g(s)fP(s) ds\int g(s)f_P(s)\,ds∫g(s)fP​(s)ds below is ∫g dP\int g\,dP∫gdP. The forecasts range over a class Vd\mathcal V^dVd of distributions.

Fix a kernel w:Rd→Rw:\mathbb R^d\to\mathbb Rw:Rd→R and a weight h≥0h\ge0h≥0 that is integrable. The smoothed density of PPP is the convolution

(fP∗w)(z)=∫Rdw(z−s) dP(s).(f_P*w)(z)=\int_{\mathbb R^d} w(z-s)\,dP(s).(fP​∗w)(z)=∫Rd​w(z−s)dP(s).

For the Heaviside kernel u(z)=1{z≥0}u(z)=\mathbb 1\{z\ge0\}u(z)=1{z≥0} it is the CDF FP(z)=P{s≤z}F_P(z)=P\{s\le z\}FP​(z)=P{s≤z}.

The two L² scoring rules are, for a forecast PXP_XPX​ and a realization yyy,

S(PX,y;w,h)=∫Rd((fX∗w)(z)−w(z−y))2h(z) dz(2)S(P_X,y;w,h)=\int_{\mathbb R^d}\big((f_X*w)(z)-w(z-y)\big)^2h(z)\,dz \qquad (2)S(PX​,y;w,h)=∫Rd​((fX​∗w)(z)−w(z−y))2h(z)dz(2) S′(PX,y;w,h)=∫Rd(fX∗w)2(z)h(z) dz−2∫Rd(fX∗w)(z) w(z−y) h(z) dz.(3)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. \qquad (3)S′(PX​,y;w,h)=∫Rd​(fX​∗w)2(z)h(z)dz−2∫Rd​(fX​∗w)(z)w(z−y)h(z)dz.(3)

The realization yyy is treated as a point mass, whose convolution with www is w(⋅−y)w(\cdot-y)w(⋅−y). The divergence of a score is EPY[S(PX,∙)]−EPY[S(PY,∙)]\mathbb E_{P_Y}[S(P_X,\bullet)]-\mathbb E_{P_Y}[S(P_Y,\bullet)]EPY​​[S(PX​,∙)]−EPY​​[S(PY​,∙)], and the paper's candidate is the weighted L² distance between smoothed densities,

∫Rd((fX∗w)(z)−(fY∗w)(z))2h(z) dz.(1)\int_{\mathbb R^d}\big((f_X*w)(z)-(f_Y*w)(z)\big)^2h(z)\,dz. \qquad (1)∫Rd​((fX​∗w)(z)−(fY​∗w)(z))2h(z)dz.(1)

Assumption 1 (p. 32) collects the integrability under which all these integrals are finite.

Formalization targets

Goal: Theorem 1 (p. 8)

Under Assumption 1, for all PX,PY∈VdP_X,P_Y\in\mathcal V^dPX​,PY​∈Vd,

EPY[S(PX,∙)]−EPY[S(PY,∙)]=EPY[S′(PX,∙)]−EPY[S′(PY,∙)]=∫(fX∗w−fY∗w)2h dz ≥0,\mathbb E_{P_Y}[S(P_X,\bullet)]-\mathbb E_{P_Y}[S(P_Y,\bullet)]=\mathbb E_{P_Y}[S'(P_X,\bullet)]-\mathbb E_{P_Y}[S'(P_Y,\bullet)]=\int\big(f_X*w-f_Y*w\big)^2h\,dz\ \ge 0,EPY​​[S(PX​,∙)]−EPY​​[S(PY​,∙)]=EPY​​[S′(PX​,∙)]−EPY​​[S′(PY​,∙)]=∫(fX​∗w−fY​∗w)2hdz ≥0,

so both rules are proper. If in addition h≠0h\ne0h=0 Ld\mathcal L^dLd-a.e. and fY∗wf_Y*wfY​∗w determines PYP_YPY​ within Vd\mathcal V^dVd, both are strictly proper. The goal fixes no kernel and no weight: it holds for every pair (w,h)(w,h)(w,h) meeting the assumption.

Milestones

  1. The relation between (2) and (3): S=S′+∫w2(z−y)h(z) dzS=S'+\int w^2(z-y)h(z)\,dzS=S′+∫w2(z−y)h(z)dz, a term that does not depend on the forecast (p. 8).
  2. The Fubini step of the proof: ∫ ⁣∫g(z)w(z−s)h(z) dz dPY(s)=∫g (fY∗w) h dz\int\!\int g(z)w(z-s)h(z)\,dz\,dP_Y(s)=\int g\,(f_Y*w)\,h\,dz∫∫g(z)w(z−s)h(z)dzdPY​(s)=∫g(fY​∗w)hdz (p. 32).
  3. The divergence display: the divergence of (2) equals (1) and is nonnegative (p. 32).
  4. The strict step: a vanishing divergence with h≠0h\ne0h=0 a.e. forces fX∗w=fY∗wf_X*w=f_Y*wfX​∗w=fY​∗w a.e. (p. 32).
  5. MCRPS (5) and MCRPS′ (6) are strictly proper for all distributions when h≠0h\ne0h=0 a.e. (p. 11).
  6. Lower partial moments of any order kkk determine the distribution (Appendix, p. 34).

Significance

Theorem 1 is the paper's justification for its whole family of scores. With w=uw=uw=u it shows that the MCRPS is proper; with www the kernel of lower partial moments it shows that a new LPM score is proper; and in Section 4 of the paper the same smoothed densities fY∗wf_Y*wfY​∗w define the level sets whose scoring functions are the subject of the companion mission (Mission II of this series). Strict properness reduces to one question about the kernel: whether fY∗wf_Y*wfY​∗w determines PYP_YPY​. Milestones 5 and 6 answer it for the CDF and for lower partial moments.

The result is proved in the paper (appendix, pp. 32 and 34). To our knowledge none of it is formalized: Mathlib has no scoring rules, and the platform has no proper scoring rule for distributions, no multivariate CRPS and no lower partial moment. The formalization adds the integrability bookkeeping the paper leaves implicit, a machine-checked uniqueness theorem for the multivariate CDF (Mathlib's ext_of_Iic covers linear orders only, i.e. d=1d=1d=1), and the same for lower partial moments.

Difficulty

The algebraic core of Theorem 1 is the expansion of a square, and the obvious argument is the paper's. The cost lies elsewhere. Every expectation is an iterated integral of a function of (s,z)(s,z)(s,z), and exchanging the order (Fubini) and splitting an integral of a difference require the integrability that Assumption 1 states only as "then (2) is well-defined and finite". The proof also uses ∫dPY=1\int dP_Y=1∫dPY​=1 when it integrates the yyy-free terms against PYP_YPY​.

For the companions the obstacle is measure-theoretic. An a.e. equality of multivariate CDFs must first be upgraded to equality everywhere, by right-continuity in each coordinate, and then measures that agree on lower orthants must be shown equal, a π-system argument in Rd\mathbb R^dRd. For lower partial moments the paper differentiates kkk times under the integral; a rigorous version has to control the finiteness of the lower-order moments.

Formalization scope

  • Rd\mathbb R^dRd is Fin d → ℝ with its product Lebesgue measure volume and the Pi order, so y≤zy\le zy≤z is componentwise and lower orthants are Set.Iic z. ddd is any natural number; at d=0d=0d=0 the strict clauses are vacuous, as in the paper.
  • Distributions are measures with IsProbabilityMeasure; the class Vd\mathcal V^dVd is a set of such measures. Its convexity (§2) is never used and is not imposed.
  • Standing assumptions. The kernel www is a measurable function. The paper also allows a local Borel measure, so that w=δ0w=\delta_0w=δ0​ gives the quadratic score (4); that case is not covered. hhh is measurable, nonnegative and integrable, not normalized to a density.
  • Assumption 1 made explicit. Its clauses (b) and (c) are formalized as integrability hypotheses, each labelled with its clause: (fY∗w)2h(f_Y*w)^2h(fY​∗w)2h and w(⋅−y)2hw(\cdot-y)^2hw(⋅−y)2h integrable; (s,z)↦w(z−s)2h(z)(s,z)\mapsto w(z-s)^2h(z)(s,z)↦w(z−s)2h(z) integrable for PY⊗LdP_Y\otimes\mathcal L^dPY​⊗Ld; (fX∗w) w(⋅−y) h(f_X*w)\,w(\cdot-y)\,h(fX​∗w)w(⋅−y)h integrable; and (s,z)↦(fX∗w)(z) w(z−s) h(z)(s,z)\mapsto(f_X*w)(z)\,w(z-s)\,h(z)(s,z)↦(fX​∗w)(z)w(z−s)h(z) integrable for PY⊗LdP_Y\otimes\mathcal L^dPY​⊗Ld. Clause (a) adds that fY∗wf_Y*wfY​∗w is well defined.
  • "fX∗w=fY∗wf_X*w=f_Y*wfX​∗w=fY​∗w" is an Ld\mathcal L^dLd-a.e. equality. "fY∗wf_Y*wfY​∗w uniquely characterizes any PY∈VdP_Y\in\mathcal V^dPY​∈Vd" is a property of the whole class Vd\mathcal V^dVd, not of the pair at hand. "hhh nonzero Ld\mathcal L^dLd-a.e." is used with the paper's quantifier. The theorem's printed "fy∗wf_{\mathbf y}*wfy​∗w" is read as fY∗wf_Y*wfY​∗w.
  • Lower partial moments are defined from the explicit kernel printed in (7), ∏j(zj−sj)k1{zj≥sj}/k!\prod_j (z_j-s_j)^k\mathbb 1\{z_j\ge s_j\}/k!∏j​(zj​−sj​)k1{zj​≥sj​}/k!, for k∈Nk\in\mathbb Nk∈N, not as a convolution power of uuu. Milestone 6 states equality of the LPMs implying PX=PYP_X=P_YPX​=PY​, the claim of its opening sentence.
  • Ruling out trivial readings. A Bochner integral of a non-integrable function is 000 in Lean, so every expectation in every statement carries the integrability that makes it the paper's integral. Without it, properness could hold because both sides are 000. The characterization hypothesis is never assumed for the pair (PX,PY)(P_X,P_Y)(PX​,PY​) alone.
  • Needed infrastructure: product-measure Fubini (integral_integral_swap), integrability of products and squares, and uniqueness of measures from a generating π-system. A general lemma "a multivariate CDF determines its measure" would be reusable well beyond this mission and is welcome as a separate contribution.

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/2002.09578v6
  • 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/10.1198/016214506000000437
  • T. Gneiting, R. Ranjan, Comparing Density Forecasts Using Threshold- and Quantile-Weighted Scoring Rules, Journal of Business & Economic Statistics 29(3), 411–422, 2011. https://doi.org/10.1198/jbes.2010.08110
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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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Functional Analysis·Captain: Lucas

Invariant Subspace ProblemOpen Problem

Motivation

The invariant subspace problem asks whether every bounded linear operator on an infinite-dimensional separable complex Hilbert space leaves some non-trivial closed subspace invariant. It is listed as a high-importance open problem in analysis in the Open Problem Garden (entry) and is widely regarded as one of the most famous open problems in functional analysis. Invariant subspaces are the infinite-dimensional replacement for eigenvectors: in finite dimensions every complex matrix has an eigenvector, and the structure theory of matrices (triangular and Jordan forms) is built from chains of invariant subspaces. Whether any such structure is available for an arbitrary bounded operator on Hilbert space is exactly what the problem asks.

Timeline

  • 1930s (von Neumann, unpublished). Compact operators on Hilbert space have non-trivial closed invariant subspaces.
  • 1954 (Aronszajn–Smith). The compact case on arbitrary Banach spaces (doi:10.2307/1969637).
  • 1966 (Bernstein–Robinson; Halmos). Polynomially compact operators on Hilbert space.
  • 1973 (Lomonosov). Every non-zero compact operator has a non-trivial closed hyperinvariant subspace; consequently every operator commuting with a non-zero compact operator has a non-trivial closed invariant subspace (doi:10.1007/BF01080698).
  • 1975 announced / 1987 published (Enflo). A bounded operator on a separable Banach space with no non-trivial closed invariant subspace (doi:10.1007/BF02392260).
  • 1985 (Read). Such an operator on the classical space ℓ1\ell^1ℓ1 (doi:10.1112/blms/17.4.305).
  • 2011 (Argyros–Haydon). An infinite-dimensional Banach space on which every operator is a scalar plus a compact operator, so that every operator on it has a non-trivial closed invariant subspace (arXiv:0903.3921).

The Hilbert-space question remains open.

Setting

Let K\mathbb{K}K be R\mathbb{R}R or C\mathbb{C}C, let EEE be a normed space over K\mathbb{K}K, and let T ⁣:E→ET\colon E\to ET:E→E be a bounded linear operator. A linear subspace S⊆ES\subseteq ES⊆E is invariant under TTT if T(S)⊆ST(S)\subseteq ST(S)⊆S. It is a non-trivial closed invariant subspace if moreover SSS is closed in the norm topology and {0}≠S≠E\{0\}\neq S\neq E{0}=S=E. A closed subspace SSS with {0}≠S≠E\{0\}\neq S\neq E{0}=S=E is a non-trivial closed hyperinvariant subspace of TTT if A(S)⊆SA(S)\subseteq SA(S)⊆S for every bounded operator AAA with AT=TAAT=TAAT=TA.

A Hilbert space HHH is a complete complex inner product space; it is separable if it has a countable dense subset. An operator KKK is compact if it maps bounded sets to relatively compact sets, and TTT is normal if T∗T=TT∗T^*T=TT^*T∗T=TT∗. In the Lean development these notions are IsInvariantSubspace, IsNontrivialClosedInvariantSubspace, HasNontrivialClosedInvariantSubspace and HasNontrivialClosedHyperinvariantSubspace (namespace InvariantSubspaceProblem), together with Mathlib's IsCompactOperator and IsStarNormal.

Formalization targets

Goal: the invariant subspace problem

∀ H separable, dim⁡H=∞, ∀ T∈B(H):∃ S⊆H closed, {0}≠S≠H, T(S)⊆S.\forall\, H \text{ separable, } \dim H=\infty,\ \forall\, T\in\mathcal{B}(H):\quad \exists\, S\subseteq H \text{ closed},\ \{0\}\neq S\neq H,\ T(S)\subseteq S .∀H separable, dimH=∞, ∀T∈B(H):∃S⊆H closed, {0}=S=H, T(S)⊆S.

The source poses a yes/no question; the goal states the affirmative answer, and a formal proof of its negation equally settles the problem.

Milestones (known results)

  1. Finite-dimensional case: every operator on a complex space of dimension ≥2\ge 2≥2 has a non-trivial invariant subspace.
  2. Non-separable case: every operator on a non-separable complex normed space has a non-trivial closed invariant subspace.
  3. Normal operators on a complex Hilbert space of dimension ≥2\ge 2≥2.
  4. Aronszajn–Smith: compact operators on infinite-dimensional real or complex Banach spaces.
  5. Lomonosov: non-zero compact operators have non-trivial closed hyperinvariant subspaces.
  6. Lomonosov: operators commuting with a non-zero compact operator.
  7. Enflo: a separable infinite-dimensional complex Banach space with an operator having no non-trivial closed invariant subspace.
  8. Read: such an operator on ℓ1\ell^1ℓ1.
  9. Argyros–Haydon: a separable infinite-dimensional real Banach space on which every operator is λI+K\lambda I+KλI+K with KKK compact.
  10. Argyros–Haydon: a separable infinite-dimensional real Banach space on which every operator has a non-trivial closed invariant subspace.

Significance

The result itself. A positive answer would give every bounded operator on Hilbert space a non-trivial piece of structure and would be the first step towards triangular-form type theorems for general operators. A negative answer would, after Enflo and Read, show that even the Hilbert-space geometry does not force invariant subspaces. Either answer resolves a question that has organised much of operator theory since the 1930s.

Formalizing it. The goal is open; no proof, formal or informal, is known. The milestones are proved results whose formal proofs would build reusable infrastructure absent from Mathlib: the Aronszajn–Smith and Lomonosov theorems (the latter through Schauder's fixed point theorem), invariant subspaces from the spectral theorem for normal operators, and the large explicit constructions of Enflo, Read and Argyros–Haydon. None of these results is formalized in Mathlib at the time of writing.

Difficulty

The obvious approach, taking the closed linear span of an orbit {x,Tx,T2x,… }\{x, Tx, T^2x,\dots\}{x,Tx,T2x,…}, fails exactly when every non-zero vector is cyclic, which is the situation that has to be ruled out; for separable spaces nothing prevents this a priori. Spectral methods fail because an operator can have a one-point spectrum and no eigenvectors (quasinilpotent operators). Methods that work on Hilbert space must use the inner-product structure in an essential way, since Enflo's and Read's examples show that the statement is false on some Banach spaces. Lomonosov's technique needs a non-zero compact operator in the commutant, which a general operator need not have.

Formalization scope

Hilbert spaces are Mathlib types H with [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]; separability is TopologicalSpace.SeparableSpace H and infinite dimension is ¬ FiniteDimensional ℂ H. Operators are continuous linear maps H →L[ℂ] H. Scalars are complex in the goal. Subspaces are Submodules, and closedness is required explicitly: without it the statement is trivially true in infinite dimensions (the algebraic span of an orbit is a proper invariant subspace), and a published platform statement that omits closedness should not be confused with this problem. Existential milestones quantify over spaces in Type.

Useful infrastructure includes: Schauder's fixed point theorem, Riesz theory of compact operators, the spectral theorem for normal operators, and ℓ1\ell^1ℓ1 machinery for Read's construction. Contributions of reusable lemmas, partial results (for instance further classes of operators known to have invariant subspaces), and proof sketches for the milestones are welcome.

Selected references

  • Open Problem Garden, Invariant subspace problem, posted by T. Chow, 2009. http://www.openproblemgarden.org/op/invariant_subspace_problem
  • N. Aronszajn, K. T. Smith, Invariant subspaces of completely continuous operators, Ann. of Math. 60 (1954) 345–350. https://doi.org/10.2307/1969637
  • V. I. Lomonosov, Invariant subspaces for the family of operators which commute with a completely continuous operator, Funct. Anal. Appl. 7 (1973) 213–214. https://doi.org/10.1007/BF01080698
  • P. Enflo, On the invariant subspace problem for Banach spaces, Acta Math. 158 (1987) 213–313. https://doi.org/10.1007/BF02392260
  • C. J. Read, A solution to the invariant subspace problem on the space ℓ1\ell_1ℓ1​, Bull. London Math. Soc. 17 (1985) 305–317. https://doi.org/10.1112/blms/17.4.305
  • S. A. Argyros, R. G. Haydon, A hereditarily indecomposable L∞\mathcal{L}_\inftyL∞​-space that solves the scalar-plus-compact problem, Acta Math. 206 (2011) 1–54. https://arxiv.org/abs/0903.3921
  • H. Radjavi, P. Rosenthal, The invariant subspace problem, Math. Intelligencer 4 (1982) 33–37.
  • B. S. Yadav, The present state and heritages of the invariant subspace problem, Milan J. Math. 73 (2005) 289–316.
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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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Mathematical PhysicsProbability·Captain: mikedeng1

Conformal Weldings of Random Surfaces: SLE and the Quantum Gravity Zipper 2: For κ < 4, Reverse SLE_κ Zipping Welds Boundary Arcs of Equal Quantum Length, ν_h[z₋,0] = ν_h[0,z₊]Research Paper

Why conformal welding by quantum length

Liouville quantum gravity (LQG) equips a planar domain with a random area measure μh\mu_hμh​ and a random boundary length measure νh\nu_hνh​. Both are built from an instance hhh of the Gaussian free field (GFF). The Schramm–Loewner evolution SLEκ\mathrm{SLE}_\kappaSLEκ​ is the conformally invariant random curve that describes interfaces in critical planar models. Sheffield's paper (arXiv:1012.4797, Ann. Probab. 44 (2016)) shows that the two are linked by a conformal welding. Zipping up a free boundary GFF by a reverse Loewner flow glues two boundary arcs of equal quantum length, and the glued seam is an SLEκ\mathrm{SLE}_\kappaSLEκ​ curve.

This "quantum zipper" is the starting point of the mating-of-trees programme (Duplantier–Miller–Sheffield, arXiv:1409.7055). It is also the mechanism behind the conjectured, and partly proved, scaling limits of random planar maps decorated by statistical-physics models.

Timeline:

  • 2005 — reverse Loewner flows are studied by Rohde and Schramm (RS05). They show that for κ<4\kappa<4κ<4 the SLE trace is simple and its complement is a Hölder domain.
  • 2000 — Jones and Smirnov show that boundaries of Hölder domains are conformally removable (JS00).
  • 2011 — Duplantier and Sheffield construct μh\mu_hμh​ and νh\nu_hνh​ as almost sure limits along dyadic scales and prove the KPZ relation (DS11a).
  • 2010–2016 — this paper (arXiv v1 2010, v2 2015, journal 2016) proves the welding theorem (Theorem 1.3) and the quantum-length zipper (Theorem 1.8).

Setting

H={z:Im⁡z>0}\mathbb H=\{z:\operatorname{Im}z>0\}H={z:Imz>0}, and the free boundary Green's function is G(y,z)=−log⁡∣y−z∣−log⁡∣y−zˉ∣G(y,z)=-\log|y-z|-\log|y-\bar z|G(y,z)=−log∣y−z∣−log∣y−zˉ∣. Fix κ∈(0,4)\kappa\in(0,4)κ∈(0,4) and put γ=κ\gamma=\sqrt\kappaγ=κ​ and Q=2/γ+γ/2Q=2/\gamma+\gamma/2Q=2/γ+γ/2.

  • Reverse Loewner flow. For a standard Brownian motion BBB, ft=gt−κBtf_t=g_t-\sqrt\kappa B_tft​=gt​−κ​Bt​, where ∂tgt(z)=−2/(gt(z)−κBt)\partial_tg_t(z)=-2/(g_t(z)-\sqrt\kappa B_t)∂t​gt​(z)=−2/(gt​(z)−κ​Bt​) and g0(z)=zg_0(z)=zg0​(z)=z. Then fTf_TfT​ maps H\mathbb HH onto H∖ηT\mathbb H\setminus\eta_TH∖ηT​, and ηT\eta_TηT​ is a simple curve.
  • The coupled field. Let ht(z)=2κlog⁡∣ft(z)∣+Qlog⁡∣ft′(z)∣\mathfrak h_t(z)=\frac2{\sqrt\kappa}\log|f_t(z)|+Q\log|f_t'(z)|ht​(z)=κ​2​log∣ft​(z)∣+Qlog∣ft′​(z)∣. With h~\tilde hh~ a free boundary GFF independent of BBB,
h=hT+h~∘fT,h=\mathfrak h_T+\tilde h\circ f_T ,h=hT​+h~∘fT​,

which by Theorem 1.2 has the law of 2κlog⁡∣⋅∣+h~\frac2{\sqrt\kappa}\log|\cdot|+\tilde hκ​2​log∣⋅∣+h~ modulo additive constants.

  • Quantum length. hε(x)h_\varepsilon(x)hε​(x) is the mean of hhh on the upper semicircle of radius ε\varepsilonε around x∈Rx\in\mathbb Rx∈R. Then
νh=lim⁡n→∞εnγ2/4eγhεn(x)/2 dx,εn=2−n,\nu_h=\lim_{n\to\infty}\varepsilon_n^{\gamma^2/4}e^{\gamma h_{\varepsilon_n}(x)/2}\,dx,\qquad \varepsilon_n=2^{-n},νh​=n→∞lim​εnγ2/4​eγhεn​​(x)/2dx,εn​=2−n,

as a vague limit. The area measure μh\mu_hμh​ is the analogous limit with circle averages and exponent γ2/2\gamma^2/2γ2/2.

  • Quantum wedges. An α\alphaα-quantum wedge is the doubly marked surface (H,h)(\mathbb H,h)(H,h) with h=h†+Q(−log⁡∣⋅∣)+A−log⁡∣⋅∣h=h^\dagger+Q(-\log|\cdot|)+A_{-\log|\cdot|}h=h†+Q(−log∣⋅∣)+A−log∣⋅∣​ (1.10). Here h†h^\daggerh† is the lateral part of the GFF and AAA is a two-sided drifted Brownian motion. A surface is identified with its canonical description, normalized by μh(B1(0))=1\mu_h(B_1(0))=1μh​(B1​(0))=1.

Formalization targets

Goal: Theorem 1.3

Almost surely, for every zzz on ηT\eta_TηT​ and the two real points z−<0<z+z_-<0<z_+z−​<0<z+​ that fTf_TfT​ maps to zzz,

νh([z−,0])=νh([0,z+]).\nu_h\big([z_-,0]\big)=\nu_h\big([0,z_+]\big).νh​([z−​,0])=νh​([0,z+​]).

The statement is scale free: it does not depend on the additive constant of hhh.

Milestones

  1. Theorem 4.5. Reverse SLEκ,ρ\mathrm{SLE}_{\kappa,\rho}SLEκ,ρ​ zipping preserves the law of h^0+h~\hat{\mathfrak h}_0+\tilde hh^​0​+h~, with h^t=ht+12κ∫Gt(y,⋅)ρ(dy)\hat{\mathfrak h}_t=\mathfrak h_t+\frac1{2\sqrt\kappa}\int G_t(y,\cdot)\rho(dy)h^​t​=ht​+2κ​1​∫Gt​(y,⋅)ρ(dy).
  2. Proposition 5.4. Under e(h0,ρ)Γe^{(h^0,\rho)}\Gammae(h0,ρ)Γ, the zipper is the modified SLE of Theorem 4.5.
  3. Proposition 1.6. Zooming in at a νh\nu_hνh​-typical boundary point gives a γ\gammaγ-quantum wedge.
  4. Proposition 1.7. The γ\gammaγ-wedge is stationary under shifting the origin by a fixed quantum length.
  5. Lemma 5.6. Sampling xxx from νh[−δ,0]\nu_h[-\delta,0]νh​[−δ,0] under Γ\GammaΓ turns the zipper into SLEκ,ρ\mathrm{SLE}_{\kappa,\rho}SLEκ,ρ​ with ρ=γ2δx−γ2σ0,1\rho=\gamma^2\delta_x-\gamma^2\sigma_{0,1}ρ=γ2δx​−γ2σ0,1​.
  6. Theorem 1.8, length clause. On a (γ−2/γ)(\gamma-2/\gamma)(γ−2/γ)-quantum wedge with an independent SLEγ2\mathrm{SLE}_{\gamma^2}SLEγ2​, the quantum lengths of the two sides of the curve agree.

Significance

Theorem 1.3 says that reverse SLE zipping is a welding by quantum length. Combined with the removability of SLEκ\mathrm{SLE}_\kappaSLEκ​ for κ<4\kappa<4κ<4, it gives Theorem 1.4: the field hhh determines the curve ηT\eta_TηT​. The same equality of boundary lengths on the two sides of an SLE is the defining property of the quantum-zipper and mating-of-trees constructions, which build random surfaces by welding wedges together.

All results here are proved in the paper, and none has a machine-checked proof. The proofs are partly sketches: Proposition 5.5 ends with a limiting estimate, and the zero–one step of Theorem 1.8 is delegated to [DMS14a, Lemma 8.2]. A formal development would therefore check the most cited welding argument in random conformal geometry. The definitions it needs (arc averages of a GFF, νh\nu_hνh​, quantum wedges, conditionally Gaussian fields) are reusable for any LQG statement.

Difficulty

The obvious argument tries to compare the left and right boundary measures directly, ball by ball along the curve. It fails because the two measures depend on the field near the curve in the same way (5.1): nothing local distinguishes them, and nothing local forces them to agree. The paper instead builds a stationary picture (Lemma 5.6, Proposition 5.5, Figure 1.7). It shows that the curve splits a (γ−2/γ)(\gamma-2/\gamma)(γ−2/γ)-wedge into two independent γ\gammaγ-wedges, and it uses the ergodic theorem with scale invariance to force the ratio of the two lengths to be a constant ccc, which symmetry makes equal to 111. The last step transfers the result from the wedge to the field of Theorem 1.3 by absolute continuity. Every step uses Gaussian conditioning on random conformal images of the field, which current libraries lack.

Formalization scope

Conventions committed to in Lean:

  • Time is R≥0\mathbb R_{\ge0}R≥0​, and Brownian motion is Mathlib's IsBrownianReal. Flows are pathwise ODE solutions, with no stochastic integrals.
  • A field is a random map Ψ(ω,μ)=(h,μ)\Psi(\omega,\mu)=(h,\mu)Ψ(ω,μ)=(h,μ) on admissible measures: finite, bounded support in H\mathbb HH, finite logarithmic energy. Its law is given in characteristic-function form, as "conditionally Gaussian given G\mathcal GG with mean mmm and covariance CCC". The arc averages hε(z)=(h,σz,ε)h_\varepsilon(z)=(h,\sigma_{z,\varepsilon})hε​(z)=(h,σz,ε​) are continuous in (z,ε)(z,\varepsilon)(z,ε).
  • Additive constants are fixed by h1(0)=0h_1(0)=0h1​(0)=0 (semicircle of radius 111), the paper's normalization (5.9).
  • νh\nu_hνh​ and μh\mu_hμh​ are predicates: the a.s. vague limits along 2−n2^{-n}2−n with locally integrable densities. The measure ν≡0\nu\equiv0ν≡0 cannot satisfy them vacuously, and the sanity file proves that adding CCC to the field multiplies ν\nuν by eγC/2e^{\gamma C/2}eγC/2.
  • The points z±z_\pmz±​ are encoded by radial boundary limits of fTf_TfT​. "Agree in law" means equality of the laws of all pairings, and convergence of random surfaces means convergence of the finite-dimensional laws of ∫f dμcan\int f\,d\mu^{\mathrm{can}}∫fdμcan.
  • Γ\GammaΓ is encoded by its restriction to (h0,(ft)t≥0)(h^0,(f_t)_{t\ge0})(h0,(ft​)t≥0​). The forward SLE of Theorem 1.8 is the platform definition OAI.SLEExactGauge.IsOrdinaryChordalSLE.

Disclosed readings of the text:

  • "α<0\alpha<0α<0" in (1.10) is read as α<Q\alpha<Qα<Q.
  • The force set C\mathcal CC of Theorem 4.5 lies in H‾\overline{\mathbb H}H.
  • Proposition 5.4 uses the measure 2κ ρ2\sqrt\kappa\,\rho2κ​ρ in (4.4)–(4.6).
  • The "unit circle" of Lemma 5.6 is the upper unit semicircle.
  • γ=0\gamma=0γ=0 is excluded in Proposition 1.6.

Contributions are welcome on any of the following:

  • existence of the predicates (νh\nu_hνh​, wedges, Γ\GammaΓ);
  • Gaussian conditioning on conformal images;
  • the Itô computations behind Theorem 4.5;
  • the milestones themselves.

Selected references

  • S. Sheffield, Conformal weldings of random surfaces: SLE and the quantum gravity zipper, Ann. Probab. 44(5), 2016. https://arxiv.org/abs/1012.4797 (v2), https://doi.org/10.1214/15-AOP1055
  • B. Duplantier, S. Sheffield, Liouville quantum gravity and KPZ, Invent. Math. 185, 2011. https://arxiv.org/abs/0808.1560
  • S. Rohde, O. Schramm, Basic properties of SLE, Ann. of Math. 161, 2005. https://arxiv.org/abs/math/0106036
  • P. Jones, S. Smirnov, Removability theorems for Sobolev functions and quasiconformal maps, Ark. Mat. 38, 2000. https://doi.org/10.1007/BF02384490
  • B. Duplantier, J. Miller, S. Sheffield, Liouville quantum gravity as a mating of trees, Astérisque 427, 2021. https://arxiv.org/abs/1409.7055
  • S. Sheffield, Gaussian free fields for mathematicians, Probab. Theory Related Fields 139, 2007. https://arxiv.org/abs/math/0312099
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Convex OptimizationDynamical SystemsOptimization·Captain: mikedeng1

A Differential Equation for Modeling Nesterov's Accelerated Gradient Method: Theory and Insights I: The ODE Ẍ + (3/t)Ẋ + ∇f(X) = 0 with X(0) = x₀, Ẋ(0) = 0 Has a Unique Global SolutionResearch Paper

Why this ODE needs a well-posedness theorem

Nesterov’s accelerated gradient method is a discrete procedure for minimizing a smooth convex function. Its iterates use both a gradient step and a momentum term, so the position at the next step depends on recent motion as well as on the current gradient. Su, Boyd, and Candès study a continuous-time model of that behavior: a trajectory whose acceleration is driven by the negative gradient and opposed by a time-dependent damping term. The model is useful only if its prescribed starting point determines an actual trajectory. The first theorem of the paper supplies that guarantee for the damping coefficient 3/t3/t3/t. Su, Boyd, and Candès, 2015, Theorem 1.

The coefficient 3/t3/t3/t is undefined at the stated initial time t=0t=0t=0. Standard results for differential equations with a continuous right-hand side at the initial time therefore cannot be applied directly. The existence and uniqueness claim is substantive: it makes the trajectory used in the paper’s later rate and restart theorems a defined mathematical object, including its behavior at the singular endpoint. The source proves the result; this mission asks for a machine-checked formalization of its statement and its supporting appendix lemmas.

The setting

Fix a dimension nnn, a starting point x0∈Rnx_0\in\mathbb R^nx0​∈Rn, and a real-valued objective fff. For a constant L>0L>0L>0, the paper’s class FL\mathcal F_LFL​ consists of functions that are convex, continuously differentiable, and have an LLL-Lipschitz gradient:

∥∇f(x)−∇f(y)∥≤L∥x−y∥for all x,y∈Rn.\|\nabla f(x)-\nabla f(y)\|\le L\|x-y\| \qquad\text{for all }x,y\in\mathbb R^n.∥∇f(x)−∇f(y)∥≤L∥x−y∥for all x,y∈Rn.

The larger class F∞\mathcal F_\inftyF∞​ is the union of these classes over positive LLL. In particular, the objective need not be strongly convex and need not have a minimizer for this mission.

A solution is a position X:[0,∞)→RnX:[0,\infty)\to\mathbb R^nX:[0,∞)→Rn and its velocity V=X˙V=\dot XV=X˙, starting at X(0)=x0X(0)=x_0X(0)=x0​ and V(0)=0V(0)=0V(0)=0, that satisfy equation (3) at every positive time:

V˙(t)+3tV(t)+∇f(X(t))=0,t>0.\dot V(t)+\frac{3}{t}V(t)+\nabla f(X(t))=0,\qquad t>0.V˙(t)+t3​V(t)+∇f(X(t))=0,t>0.

The trajectory is continuously differentiable through the initial endpoint, with a right derivative there, and twice continuously differentiable for t>0t>0t>0. The paper also uses a smoothed equation indexed by δ>0\delta>0δ>0, replacing 3/t3/t3/t with 3/max⁡(δ,t)3/\max(\delta,t)3/max(δ,t). Its solutions are denoted XδX_\deltaXδ​, and its velocity-growth quantity is

Mδ(t)=sup⁡0<u≤t∥X˙δ(u)∥u.M_\delta(t)=\sup_{0<u\le t}\frac{\|\dot X_\delta(u)\|}{u}.Mδ​(t)=0<u≤tsup​u∥X˙δ​(u)∥​.

For local uniqueness, two solutions X,YX,YX,Y on [0,a)[0,a)[0,a) are compared using M~(t)=sup⁡0≤u<t∥X˙(u)−Y˙(u)∥\widetilde M(t)=\sup_{0\le u<t}\|\dot X(u)-\dot Y(u)\|M(t)=sup0≤u<t​∥X˙(u)−Y˙(u)∥. These quantities appear in the appendix lemmas and are represented by pointwise bounds in the formal statements.

Formalization targets

The goal is Theorem 1, the well-posedness of equation (3). For every f∈F∞f\in\mathcal F_\inftyf∈F∞​ and every x0x_0x0​, it asserts both existence of a global trajectory with the regularity above and uniqueness on nonnegative time:

∃X solving (3) from (x0,0),X,Y both solve (3) from (x0,0)⟹X(t)=Y(t)(t≥0).\exists X\ \text{solving (3) from }(x_0,0), \qquad X,Y\ \text{both solve (3) from }(x_0,0) \Longrightarrow X(t)=Y(t)\quad(t\ge0).∃X solving (3) from (x0​,0),X,Y both solve (3) from (x0​,0)⟹X(t)=Y(t)(t≥0).

The milestone list follows the numbered statements in Appendix A. Lemma 16 controls the change in ∇f\nabla f∇f along a smoothed trajectory. Lemmas 15 and 17 bound MδM_\deltaMδ​ on the initial smoothing interval and beyond it, with the explicit thresholds δ<6/L\delta<\sqrt{6/L}δ<6/L​ and t<12/Lt<\sqrt{12/L}t<12/L​. Lemma 18 states that the family of smoothed trajectories with δ=3/L/2m\delta=\sqrt{3/L}/2^mδ=3/L​/2m is uniformly bounded and equicontinuous on [0,6/L][0,\sqrt{6/L}][0,6/L​]. Lemma 14 gives existence for equation (3). Lemma 20 bounds the difference between gradients along two local solutions, and Lemma 19 gives uniqueness in a neighborhood of zero. The goal and milestones preserve the source’s domains, constants, and order of dependence.

What the result provides

Theorem 1 permits the rest of the paper to refer to “the” trajectory of equation (3) from a specified initial point. In particular, statements about its objective value, energy, and restarts need an actual trajectory, and uniqueness makes those statements independent of a choice of solution. The appendix estimates also provide reusable facts about this singular second-order equation: quantitative control of smoothed velocities and local agreement at the singular time.

The paper proves Theorem 1 and the seven listed lemmas on pp. 6 and 28–32. This mission does not claim a new analytical result. Its output would be checked Lean statements and, when solvers finish the proofs, a machine-checked development of the singular initial-value problem. The formal definitions are shared by all items in this mission; the lemmas can be reused in later formal work on accelerated gradient trajectories. No machine-checked proof of these particular statements is being claimed by the draft proposal.

The central difficulty

The initial time is precisely where the damping 3/t3/t3/t has no finite value. Treating the problem as an ordinary initial-value problem at t=0t=0t=0 leaves the differential equation undefined there. Imposing the equation at t=0t=0t=0 after Lean’s total division would instead change it: Lean assigns a value to division by zero, while the paper imposes equation (3) only for t>0t>0t>0. The demanded derivative at zero is one-sided, and control of the behavior as t↓0t\downarrow0t↓0 is part of the result.

The smoothed equations are regular at zero, but a statement about each smoothed trajectory does not by itself give a solution of the original singular equation. The appendix’s uniform bounds and equicontinuity are formulated on a common compact interval for a specified sequence of smoothing parameters. Uniqueness has a second boundary issue: local agreement near zero must be connected to ordinary uniqueness at positive time to obtain agreement for every t≥0t\ge0t≥0.

Formalization scope

The Lean space is EuclideanSpace R (Fin n)\mathrm{EuclideanSpace}\ \mathbb R\ (\mathrm{Fin}\ n)EuclideanSpace R (Fin n), with its Euclidean norm; nnn is arbitrary. The objective class includes convexity, C1C^1C1 regularity, a positive Lipschitz constant, and a globally Lipschitz gradient. A solution is encoded as a pair (X,V)(X,V)(X,V), so V=X˙V=\dot XV=X˙ is witnessed by derivative assertions rather than by a total derivative operator. The initial conditions specify X(0)=x0X(0)=x_0X(0)=x0​, V(0)=0V(0)=0V(0)=0, a right derivative of XXX, and right continuity of VVV. The differential equation and ordinary derivatives are required only at positive times. For the smoothed equation, δ>0\delta>0δ>0 is part of the solution predicate.

These choices rule out a vacuous solution predicate and prevent division by zero from defining a different equation. Lean functions are represented on all real times, but the source’s solution lives on [0,∞)[0,\infty)[0,∞); uniqueness is therefore equality on that half-line. At negative times the formal representatives are unrestricted. The paper’s real suprema MδM_\deltaMδ​ and M~\widetilde MM are expressed as bounds on every member of their defining ranges, so an empty or unbounded real supremum cannot acquire a misleading default value. Every denominator in Lemmas 15 and 17 has the paper’s strict threshold in its hypotheses.

A full proof development needs ordinary differential equation existence and uniqueness at positive time, continuity and derivative facts at the right endpoint, and compactness of uniformly bounded equicontinuous families. The definitions of the objective class and solution predicates, the quantitative estimates, and the local uniqueness statement are welcome solver contributions. The target is the source theorem with its stated hypotheses and conclusion; a special objective, a weakened time interval, or a proof by an impossible hypothesis does not close it.

Selected references

  • Weijie Su, Stephen Boyd, and Emmanuel J. Candès, A Differential Equation for Modeling Nesterov’s Accelerated Gradient Method: Theory and Insights, arXiv:1503.01243v2, 2015; published in Journal of Machine Learning Research 17(153), 2016. Preprint.
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Operations ResearchOptimizationProbability·Captain: mikedeng1

On the Heavy-Tail Behavior of the Distributionally Robust Newsvendor 1: Worst-Case Expected Shortage under Known First and αth Moments Equals That of a Regularly Varying Demand of Tail Index αResearch Paper

Motivation

A newsvendor chooses an order quantity before seeing demand. Unsold units have no salvage value, while demand above the order quantity cannot be filled. If the demand law is unknown but a few moments are known, the decision maker may minimize cost against the worst distribution consistent with those moments. Das, Dhara and Natarajan study this distributionally robust problem when the known moments are the first and an arbitrary real moment of order α>1\alpha>1α>1 Das, Dhara and Natarajan, 2019. The high-demand tail matters especially when the cost ratio favors large orders. The mission asks what tail behavior is implicitly selected by the robust objective, even though each admissible distribution has a finite α\alphaαth moment.

The two-moment case α=2\alpha=2α=2 goes back to Scarf's newsvendor bound. The paper extends the model to noninteger α\alphaα and gives lower and upper shortage bounds before proving its tail result. Its preprint is the pinned source for every statement here; the proof of each numbered result follows that result in the paper Das, Dhara and Natarajan, 2019, §§1, 3–4.

Setting

Let q≥0q\ge0q≥0 be the order quantity and let d~≥0\tilde d\ge0d~≥0 be random demand. The expected shortage under a demand law FFF is EF[(d~−q)+]\mathbb E_F[(\tilde d-q)^+]EF​[(d~−q)+], where x+=max⁡(x,0)x^+=\max(x,0)x+=max(x,0). Fix α>1\alpha>1α>1, a positive mean m1m_1m1​, and a moment mα>m1αm_\alpha>m_1^\alphamα​>m1α​. The moment ambiguity set F1,α\mathcal F_{1,\alpha}F1,α​ contains all probability laws supported on [0,∞)[0,\infty)[0,∞) whose first moment is m1m_1m1​ and whose finite α\alphaαth moment is mαm_\alphamα​. Its worst-case expected shortage is

Π1,α(q)=sup⁡F∈F1,αEF[(d~−q)+].\Pi_{1,\alpha}(q)=\sup_{F\in\mathcal F_{1,\alpha}}\mathbb E_F[(\tilde d-q)^+].Π1,α​(q)=F∈F1,α​sup​EF​[(d~−q)+].

For a critical ratio η∈[0,1)\eta\in[0,1)η∈[0,1), the robust newsvendor minimizes (1−η)q+Π1,α(q)(1-\eta)q+\Pi_{1,\alpha}(q)(1−η)q+Π1,α​(q) over q≥0q\ge0q≥0. This mission centers on Π1,α\Pi_{1,\alpha}Π1,α​; the optimal-order threshold is treated in the companion mission. The ambiguity set and objective are the paper's (3.1)–(3.3) Das, Dhara and Natarajan, 2019, pp. 10–11.

A positive function uuu is regularly varying with index ρ\rhoρ if u(tx)/u(x)→tρu(tx)/u(x)\to t^\rhou(tx)/u(x)→tρ as x→∞x\to\inftyx→∞ for every t>0t>0t>0. The notation is u∈RVρu\in RV_\rhou∈RVρ​. For a probability law FFF, its survival tail is Fˉ(x)=PF(d~>x)\bar F(x)=P_F(\tilde d>x)Fˉ(x)=PF​(d~>x); Fˉ∈RV−α\bar F\in RV_{-\alpha}Fˉ∈RV−α​ means a tail parameter α\alphaα Das, Dhara and Natarajan, 2019, §4.1, p. 26.

Formalization targets

Worst-case shortage

The first target is Theorem 4.3(a):

Π1,α∈RV−(α−1).\Pi_{1,\alpha}\in RV_{-(\alpha-1)}.Π1,α​∈RV−(α−1)​.

It covers every α>1\alpha>1α>1, including α=2\alpha=2α=2. Scarf's piecewise formula (1.3), Proposition 3.3, and both parts of Proposition 3.4 supply the paper's cited bounds. Each upper bound retains its strict quantity threshold and its printed denominator Das, Dhara and Natarajan, 2019, pp. 3, 15, 19, 28.

One representative demand law

The full goal, Theorem 4.3, also states that a nonnegative probability law F∗F^*F∗ exists outside F1,α\mathcal F_{1,\alpha}F1,α​ with

EF∗[(d~∗−q)+]=Π1,α(q)(q≥0),Fˉ∗∈RV−α.\mathbb E_{F^*}[(\tilde d^*-q)^+]=\Pi_{1,\alpha}(q)\quad(q\ge0), \qquad \bar F^*\in RV_{-\alpha}.EF∗​[(d~∗−q)+]=Π1,α​(q)(q≥0),Fˉ∗∈RV−α​.

Every moment of F∗F^*F∗ of order 0≤a<α0\le a<\alpha0≤a<α is finite, while every moment of order a≥αa\ge\alphaa≥α is infinite. The milestone list includes the properties of Π1,α\Pi_{1,\alpha}Π1,α​ stated in §2.1 (non-increasing, convex, Π1,α(q)+q=m1\Pi_{1,\alpha}(q)+q=m_1Π1,α​(q)+q=m1​ for q≤0q\le0q≤0, Π1,α(q)→0\Pi_{1,\alpha}(q)\to0Π1,α​(q)→0), the single-law representation (2.1) and the two stated Karamata results used to characterize the tail Das, Dhara and Natarajan, 2019, pp. 6, 27–30.

High critical ratios

A companion milestone is Proposition 4.1. For η∈(0,1)\eta\in(0,1)η∈(0,1) let qη∗q^*_\etaqη∗​ be a robust optimal order quantity and Cη∗C^*_\etaCη∗​ the optimal robust cost. Then qη∗q^*_\etaqη∗​ is optimal for the standard newsvendor with demand law F∗F^*F∗, and

qη∗∼α−1α 11−η Cη∗,η→1q^*_\eta\sim\frac{\alpha-1}{\alpha}\,\frac{1}{1-\eta}\,C^*_\eta,\qquad \eta\to1qη∗​∼αα−1​1−η1​Cη∗​,η→1

Das, Dhara and Natarajan, 2019, p. 30, (4.9). It is a consequence of the goal, not a step toward it.

Significance

The theorem connects a decision made against an entire moment class to a single effective law. That law matches the robust expected shortage for every admissible order quantity but has an infinite α\alphaαth moment, so it does not belong to the class being optimized over. This distinction explains why large robust orders behave as though demand were heavy tailed. The paper also uses the result to relate the robust optimal order quantity to the optimal cost at high service levels in Proposition 4.1 Das, Dhara and Natarajan, 2019, pp. 30–31.

The mathematical theorem was proved in the cited paper. This mission asks for a Lean proof of its exact statement and reusable formal results for moment-constrained probability laws, stop-loss transforms, and regular variation. No machine-checked proof of these particular statements is part of the present draft. The cited bounds and analytic results are posed as separate milestones so their hypotheses and constants remain inspectable.

Difficulty

Pointwise optimization over demand laws does not automatically give one law that attains the worst-case shortage for every qqq. For a fixed qqq, an extremal law may depend on qqq, as Scarf's formula illustrates Das, Dhara and Natarajan, 2019, p. 3. The theorem asks for a single F∗F^*F∗ and then a precise tail index and a sharp moment cutoff. A generic upper bound on shortages would establish neither the representative law nor its infinite α\alphaαth moment. The regimes 1<α<21<\alpha<21<α<2, α=2\alpha=2α=2, and α>2\alpha>2α>2 have different cited upper-bound statements, yet the final theorem has no regime restriction.

Formalization scope

Lean represents a demand law by a Borel measure on R\mathbb RR with probability mass one and zero mass below zero. Membership in F1,α\mathcal F_{1,\alpha}F1,α​ requires both real moments to be integrable; this makes the moment equalities genuine rather than default values of a nonintegrable Bochner integral. Under m1>0m_1>0m1​>0 and mα>m1αm_\alpha>m_1^\alphamα​>m1α​, the paper's two-point law (3.6) makes the ambiguity set nonempty. Its shortage values are bounded above by m1+∣q∣m_1+|q|m1​+∣q∣, so the real supremum defining Π1,α\Pi_{1,\alpha}Π1,α​ is finite and meaningful. The strict thresholds in Propositions 3.3–3.4 keep their power denominators positive Das, Dhara and Natarajan, 2019, pp. 12, 15, 19.

Regular variation includes eventual positivity, excluding a zero-over-zero ratio from passing as a tail law. Infinite moments of F∗F^*F∗ are lower Lebesgue integrals in extended nonnegative reals. The existence of F∗F^*F∗ is asserted rather than built into a definition. Theorem 4.2(b)'s displayed limit has a negative sign in the preprint, although its nonnegative numerator and denominator require the positive value α\alphaα; the formal statement uses the corrected sign. Its regularly varying tail integral is eventually positive, which ensures genuine finite tail integrals for large lower limits. Theorem 4.1 explicitly requires local integrability. Two encodings would trivialize the goal and are excluded: defining F∗F^*F∗ inside the statement (it is existential), and a regular-variation predicate satisfied by the zero function. The properties of Π\PiΠ and the representation (2.1) are stated for F1,α\mathcal F_{1,\alpha}F1,α​, the instance the paper uses, rather than for a general finite-mean ambiguity set. In Proposition 4.1 the optimal cost is the cost at the chosen optimizer, the statement holds for every selection of optimizers, and ∼\sim∼ means that the ratio of the two sides tends to 111 as η↑1\eta\uparrow1η↑1. These analytic conventions and the probability and measure infrastructure can be reused beyond this mission. Contributions to any of the ten source milestones, including the difficult root assertion in Proposition 3.4(b), are welcome.

Selected references

  • B. Das, A. Dhara, and K. Natarajan, On the Heavy-Tail Behavior of the Distributionally Robust Newsvendor, Operations Research 69(4), 2021; preprint arXiv:1806.05379v2, 2019. Preprint, DOI.
  • H. Scarf, A min-max solution of an inventory problem, in K. Arrow, S. Karlin and H. Scarf (eds.), Studies in the Mathematical Theory of Inventory and Production, Stanford University Press, 1958, pp. 201–209.
  • A. Shapiro and A. Kleywegt, Minimax analysis of stochastic problems, Optimization Methods and Software 17, 2002, pp. 523–542. DOI.
  • N. H. Bingham, C. M. Goldie and J. L. Teugels, Regular Variation, Cambridge University Press, 1987. DOI.
12 thms2 active usersReviewed
🏆Completed
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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Optimization·Captain: mikedeng1

Semismooth and Semiconvex Functions in Constrained Optimization II: A Semismooth Composition of Semismooth Functions Is Semismooth, with a Chain Rule for Generalized GradientsResearch Paper

Why composition matters

Optimization models often build an objective from several intermediate quantities: constraints, penalties, and transformed measurements are evaluated first, then combined by an outer function. These intermediate and outer functions can be Lipschitz without being differentiable at the point of interest. Ordinary differentiation supplies no chain rule there. The generalized-gradient framework gives a set of possible first-order slopes, while semismoothness provides stronger directional behavior along sequences approaching the point. Mifflin's IIASA report asks whether this behavior survives such compositions and how the generalized gradient of the result relates to those of its ingredients.

The report first establishes basic properties of the generalized gradient in §2, including almost-everywhere differentiability and a nonsmooth mean value theorem. Section 4 then states a chain-rule inclusion as Theorem 4 and the semismooth composition result as Theorem 5. The report is dated December 1976; a journal version appeared in 1977. The mission cites theorem numbers and pages from the report version throughout. No claim about differences between the report and journal texts is needed here.

Setting and definitions

Work in finite-dimensional Euclidean spaces. Let fi:Rn→Rf_i:\mathbb R^n\to\mathbb Rfi​:Rn→R, for i=1,…,mi=1,\ldots,mi=1,…,m, be component functions, and let E:Rm→RE:\mathbb R^m\to\mathbb RE:Rm→R be an outer function. Define the component map YYY and the composite FFF by

Y(x)=(f1(x),…,fm(x)),F(x)=E(Y(x)).Y(x)=(f_1(x),\ldots,f_m(x)),\qquad F(x)=E(Y(x)).Y(x)=(f1​(x),…,fm​(x)),F(x)=E(Y(x)).

The functions are locally Lipschitz in the report's precise sense: on each bounded subset of their Euclidean domain they have a finite Lipschitz constant. For a scalar function HHH, a point xxx, and a direction ddd, the generalized directional derivative H0(x;d)H^0(x;d)H0(x;d) is the joint upper limit of [H(x+h+td)−H(x+h)]/t[H(x+h+td)-H(x+h)]/t[H(x+h+td)−H(x+h)]/t as h→0h\to0h→0 and t↓0t\downarrow0t↓0. Its associated generalized gradient is the support set

∂H(x)={g:⟨g,d⟩≤H0(x;d) for every direction d}.\partial H(x)=\{g:\langle g,d\rangle\le H^0(x;d)\text{ for every direction }d\}.∂H(x)={g:⟨g,d⟩≤H0(x;d) for every direction d}.

This is the definition used in Mifflin's report, not an identification assumed in advance with a hull of ordinary gradient limits. Proposition 1(c) supplies that identification under the paper's Lipschitz assumption. The ordinary one-sided directional derivative H′(x;d)H'(x;d)H′(x;d) is the limit of [H(x+td)−H(x)]/t[H(x+td)-H(x)]/t[H(x+td)−H(x)]/t for t↓0t\downarrow0t↓0, when that limit exists.

Mifflin calls HHH semismooth at xxx if it is Lipschitz on a ball about xxx and the scalar sequence ⟨gk,d⟩\langle g_k,d\rangle⟨gk​,d⟩ has exactly one accumulation point whenever tk>0t_k>0tk​>0 tends to zero, θk/tk→0\theta_k/t_k\to0θk​/tk​→0, and gk∈∂H(x+tkd+θk)g_k\in\partial H(x+t_kd+\theta_k)gk​∈∂H(x+tk​d+θk​). The quantification is over every direction and every such sequence. This pointwise condition is Definition 1 of the report, and its link to one-sided directional derivatives is Lemma 2.

To state the chain rule, form the set

G(x)=conv⁡{∑i=1mwigi:gi∈∂fi(x) for every i,w∈∂E(Y(x))}.G(x)=\operatorname{conv}\left\{\sum_{i=1}^{m}w_i g^i:g^i\in\partial f_i(x)\text{ for every }i,\quad w\in\partial E(Y(x))\right\}.G(x)=conv{i=1∑m​wi​gi:gi∈∂fi​(x) for every i,w∈∂E(Y(x))}.

The same www is used across all components. The sum is the action of the report's matrix [g1⋯gm][g^1\cdots g^m][g1⋯gm] on www.

Formalization targets

Generalized-gradient chain rule

Theorem 4 asserts that FFF is locally Lipschitz and that, at every point,

∂F(x)⊆G(x).\partial F(x)\subseteq G(x).∂F(x)⊆G(x).

This is an inclusion, not a general equality. The report gives an example immediately after Theorem 4 in which the inclusion is strict: two identical absolute-value components cancel under an outer difference, while G(0)G(0)G(0) remains larger than ∂F(0)\partial F(0)∂F(0).

Semismooth composition

The goal, Theorem 5, assumes the setting of Theorem 4. If each fif_ifi​ is semismooth at a selected xxx and EEE is semismooth at Y(x)Y(x)Y(x), then

E∘Y is semismooth at x.E\circ Y\text{ is semismooth at }x.E∘Y is semismooth at x.

The conclusion is pointwise. It does not assert semismoothness throughout Rn\mathbb R^nRn from hypotheses at one point. The milestone list contains the chain rule and the source's stated support results: Proposition 2, Lemma 1, Proposition 1(c) and (d), Lemma 2, and the claims (4.2) and (4.11)–(4.12) from the proofs.

What the results provide

Theorem 5 permits composite nonsmooth objectives to be treated within the same semismooth class as their components. Theorem 4 gives a concrete set built from component generalized gradients that contains the composite's generalized gradient. Together, they let later statements about a composite use first-order information from its stated ingredients, subject to the inclusion's possible strictness. These are results proved in Mifflin's report, not open mathematical conjectures.

This mission drafts machine-checkable statements of those known results and their definition layer. The local Lean modules compile with proof placeholders; this staging does not supply machine-checked proofs of the theorems. A complete development would formalize the known arguments or another proof of the same statements. The reusable output would include the support-set generalized gradient, sequence-based semismoothness, the nonsmooth mean value result, and the chain-rule inclusion, all with their source assumptions exposed.

Main difficulty

At a point where FFF is differentiable, the component functions fif_ifi​ need not be differentiable, and the outer function EEE need not be differentiable at Y(x)Y(x)Y(x). The ordinary smooth chain rule therefore cannot simply multiply ordinary gradients. The candidate G(x)G(x)G(x) is a convex set of combinations of generalized gradients; a single chosen combination does not in general describe all nearby limiting slopes. The report's strict-inclusion example also shows why replacing Theorem 4 by equality would be false. For semismoothness, the condition concerns every admissible sequence of generalized gradients near the point, so checking just one path or one gradient selection does not establish Theorem 5.

Formalization scope

The Lean domain is EuclideanSpace ℝ (Fin n) and the outer domain is EuclideanSpace ℝ (Fin m). The report's norm is the Euclidean norm and its pairing is the real inner product. An index of type Fin m represents the mmm components; m=0m=0m=0 is admitted, in which case the component space is a point and the composite is constant. A finite sum represents the column-matrix product. The generalized gradient is defined by all directional support inequalities, so Proposition 1(c) remains a theorem rather than becoming true by definition.

The generalized directional derivative is imported from the published definition matching the report's joint limit. Lean's real limsup has a default value for an unbounded quotient; Lipschitz hypotheses are carried wherever that operation is used. “Locally Lipschitz” is imported as Lipschitzness on every bounded subset, and the explicit constants of §2 use nonnegative reals, equivalent to the report's positive constants by enlarging them. The directional derivative is a relation asserting a limit, so no value is assigned when the limit fails. “Exactly one accumulation point” remains an existence-and-uniqueness assertion about cluster points. The report's tk↓0t_k\downarrow0tk​↓0 means positive convergence to zero, as its proof of Lemma 2 says explicitly. These choices exclude a vacuous formulation that only asks about one convenient sequence or gives a default directional value.

The scope includes the two local definition files and the cited theorem statements, including both conclusions of Theorem 4 and Lemma 2. Proof contributions would need finite-dimensional Lipschitz and differentiability infrastructure, limiting-gradient compactness, convex hull and separation facts, and sequence convergence facts. Results about the alternative Qi–Sun vector-valued semismoothness notion are outside this mission's definition layer.

Selected references

  • R. Mifflin, Semismooth and Semiconvex Functions in Constrained Optimization, IIASA Research Report RR-76-21, December 1976. Report PDF.
  • R. Mifflin, “Semismooth and Semiconvex Functions in Constrained Optimization,” SIAM Journal on Control and Optimization 15(6), 1977. DOI. This mission's page and theorem references are to the IIASA report.
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Probability·Captain: mikedeng1

Discrete Analogues of Self-Decomposability and Stability 1: A p.g.f. Is Discrete Self-Decomposable iff P(z) = exp{−λ∫_z^1 (1−G(u))/(1−u) du}, iff It Is Infinitely Divisible with Nonincreasing r_nResearch Paper

Motivation

A probability distribution on the real line is self-decomposable (of class L) if its characteristic function satisfies φ(t)=φ(αt) φα(t)\varphi(t)=\varphi(\alpha t)\,\varphi_\alpha(t)φ(t)=φ(αt)φα​(t) for every α∈(0,1)\alpha\in(0,1)α∈(0,1), with φα\varphi_\alphaφα​ again a characteristic function. Equivalently, a random variable XXX can be written as X=dαX′+XαX\overset{d}{=}\alpha X'+X_\alphaX=dαX′+Xα​ with X′X'X′ a copy of XXX independent of XαX_\alphaXα​. Class L consists exactly of the limit laws of normalized sums of independent summands, and its members are infinitely divisible, absolutely continuous (when nondegenerate) and unimodal.

None of this transfers to counting variables: apart from X≡0X\equiv0X≡0, no random variable on N0={0,1,2,… }\mathbb N_0=\{0,1,2,\dots\}N0​={0,1,2,…} satisfies X=αX′+XαX=\alpha X'+X_\alphaX=αX′+Xα​, because αX′\alpha X'αX′ leaves the lattice. Steutel and van Harn (Memorandum COSOR 78-07, 1978; Ann. Probab. 7 (1979) 893–899) replaced scalar multiplication by binomial thinning, which keeps the variable integer valued. The resulting notion of discrete self-decomposability later became the basis of integer-valued autoregressive (INAR) time-series models (Al-Osh and Alzaid, 1987).

Timeline:

  • 1968: Feller, An Introduction to Probability Theory and Its Applications, vol. 1, 3rd ed., characterizes the infinitely divisible distributions on N0\mathbb N_0N0​ as the compound Poisson distributions.
  • 1971: Steutel, On the zeros of infinitely divisible densities (Ann. Math. Statist. 42), and 1977: van Harn and Steutel, Generalized renewal sequences and infinitely divisible lattice distributions (Stoch. Proc. Appl. 5), give the recursive criterion (n+1)pn+1=∑kpkrn−k(n+1)p_{n+1}=\sum_k p_k r_{n-k}(n+1)pn+1​=∑k​pk​rn−k​ with rn≥0r_n\ge0rn​≥0.
  • 1978–1979: Steutel and van Harn introduce discrete self-decomposability and discrete stability and prove the canonical form (Theorem 2.2, the goal of this mission), unimodality, and the characterization of the discrete stable laws.

Setting

A distribution on N0\mathbb N_0N0​ is a sequence pn≥0p_n\ge0pn​≥0 with ∑npn=1\sum_n p_n=1∑n​pn​=1; its probability generating function (p.g.f.) is P(z)=∑n≥0pnznP(z)=\sum_{n\ge0}p_nz^nP(z)=∑n≥0​pn​zn. The generating function of a sequence (gn)(g_n)(gn​) is written GGG.

The α\alphaα-thinning of a variable XXX with p.g.f. PPP is α∘X=∑j=1XNj\alpha\circ X=\sum_{j=1}^{X}N_jα∘X=∑j=1X​Nj​ with independent Bernoulli(α\alphaα) variables NjN_jNj​; its p.g.f. is P(1−α+αz)P(1-\alpha+\alpha z)P(1−α+αz). A distribution with p.g.f. PPP is discrete self-decomposable (Definition 2.1) if for every α∈(0,1)\alpha\in(0,1)α∈(0,1)

P(z)=P(1−α+αz) Pα(z)(∣z∣≤1)P(z)=P(1-\alpha+\alpha z)\,P_\alpha(z)\qquad(|z|\le1)P(z)=P(1−α+αz)Pα​(z)(∣z∣≤1)

with PαP_\alphaPα​ a p.g.f.; in variables, X=dα∘X′+XαX\overset{d}{=}\alpha\circ X'+X_\alphaX=dα∘X′+Xα​.

A distribution is infinitely divisible if for every n≥1n\ge1n≥1 its p.g.f. is the nnn-th power of a p.g.f. When p0>0p_0>0p0​>0, its canonical sequence (rn)(r_n)(rn​) is the unique solution of

(n+1) pn+1=∑k=0npk rn−k(n∈N0).(n+1)\,p_{n+1}=\sum_{k=0}^{n}p_k\,r_{n-k}\qquad(n\in\mathbb N_0).(n+1)pn+1​=k=0∑n​pk​rn−k​(n∈N0​).

Throughout §2 the paper assumes 0<p0<10<p_0<10<p0​<1.

Formalization targets

Goal: Theorem 2.2

For a distribution (pn)(p_n)(pn​) with 0<p0<10<p_0<10<p0​<1:

(pn) discrete self-dec  ⟺  P(z)=exp⁡{−λ∫z11−G(u)1−u du}(0≤z<1)(p_n)\ \text{discrete self-dec}\iff P(z)=\exp\Big\{-\lambda\int_z^1\frac{1-G(u)}{1-u}\,du\Big\}\quad(0\le z<1)(pn​) discrete self-dec⟺P(z)=exp{−λ∫z1​1−u1−G(u)​du}(0≤z<1)

for some λ>0\lambda>0λ>0 and some p.g.f. GGG of a distribution with G(0)=0G(0)=0G(0)=0, the pair (λ,G)(\lambda,G)(λ,G) being unique; and

(pn) discrete self-dec  ⟺  (pn) inf div and (rn) nonincreasing.(p_n)\ \text{discrete self-dec}\iff (p_n)\ \text{inf div and } (r_n)\ \text{nonincreasing}.(pn​) discrete self-dec⟺(pn​) inf div and (rn​) nonincreasing.

Milestones

  1. Lemma 1.1: lim⁡x↑1(1−x)P′(x)=0\lim_{x\uparrow1}(1-x)P'(x)=0limx↑1​(1−x)P′(x)=0 for every p.g.f.
  2. Lemma 1.2: for 0<p0<10<p_0<10<p0​<1, PPP is infinitely divisible iff P(z)=exp⁡{λ(G(z)−1)}P(z)=\exp\{\lambda(G(z)-1)\}P(z)=exp{λ(G(z)−1)} (unique λ>0\lambda>0λ>0, G(0)=0G(0)=0G(0)=0), iff P(z)=exp⁡{−∫z1R(u) du}P(z)=\exp\{-\int_z^1R(u)\,du\}P(z)=exp{−∫z1​R(u)du} with R=∑rnunR=\sum r_nu^nR=∑rn​un, rn≥0r_n\ge0rn​≥0 (necessarily ∑rn/(n+1)<∞\sum r_n/(n+1)<\infty∑rn​/(n+1)<∞), iff the canonical sequence is nonnegative.
  3. (2.6): if PPP is discrete self-decomposable, exp⁡{−r(1−z)P′(z)/P(z)}\exp\{-r(1-z)P'(z)/P(z)\}exp{−r(1−z)P′(z)/P(z)} is a p.g.f. for every r>0r>0r>0.
  4. (2.7)–(2.8): the form (2.4) gives P′/P=λ(1−G)/(1−z)P'/P=\lambda(1-G)/(1-z)P′/P=λ(1−G)/(1−z), infinite divisibility, and rn=λ∑j>ngjr_n=\lambda\sum_{j>n}g_jrn​=λ∑j>n​gj​, nonincreasing.
  5. The converse (pp. 3–4): if PPP is infinitely divisible with nonincreasing rnr_nrn​, then P(z)/P(1−α+αz)P(z)/P(1-\alpha+\alpha z)P(z)/P(1−α+αz) is an infinitely divisible p.g.f. for each α∈(0,1)\alpha\in(0,1)α∈(0,1).

Significance

Theorem 2.2 reduces discrete self-decomposability, a condition quantified over all α∈(0,1)\alpha\in(0,1)α∈(0,1) and over unknown factors PαP_\alphaPα​, to a single monotonicity condition on the sequence (rn)(r_n)(rn​) computed recursively from (pn)(p_n)(pn​). It is the entry point of the rest of the paper: combined with Theorem 2.3 it gives unimodality of every discrete self-decomposable distribution (Corollary 2.4), and §3 shows that discrete stable distributions are discrete self-decomposable. In time-series modelling it identifies the marginals that a stationary INAR(1) process Xt=α∘Xt−1+εtX_t=\alpha\circ X_{t-1}+\varepsilon_tXt​=α∘Xt−1​+εt​ can have for every α∈(0,1)\alpha\in(0,1)α∈(0,1).

The result has been proved since 1979; to our knowledge none of it is formalized in any proof assistant, and Mathlib has neither probability generating functions on N0\mathbb N_0N0​ nor infinite divisibility. The mission produces a machine-checked version of the canonical form together with the compound-Poisson characterization of infinite divisibility on N0\mathbb N_0N0​ (Lemma 1.2), which the paper only cites.

Difficulty

The forward direction is not a consequence of (2.1) for any single α\alphaα: one factorization P(z)=P(1−α+αz)Pα(z)P(z)=P(1-\alpha+\alpha z)P_\alpha(z)P(z)=P(1−α+αz)Pα​(z) constrains PPP very little, and the information sits in the whole family of factors PαP_\alphaPα​, α∈(0,1)\alpha\in(0,1)α∈(0,1), which are not given explicitly. Turning that family into a statement about PPP needs a passage to a limit of p.g.f.'s, and the fact that such a limit is again a p.g.f. (the continuity theorem for p.g.f.'s, Feller vol. 1, p. 280) is not in Mathlib. The paper does not prove Lemma 1.2 either; it cites Feller and Steutel. For the converse, nonnegativity of the canonical sequence is not enough: the obvious attempt to show that P(z)/P(1−α+αz)P(z)/P(1-\alpha+\alpha z)P(z)/P(1−α+αz) has nonnegative coefficients fails for infinitely divisible PPP in general, and the monotonicity of rnr_nrn​ is exactly what is needed. Finally, every identity is stated between real functions on [0,1][0,1][0,1], and passing to identities between coefficients requires the uniqueness of power-series coefficients on a real interval.

Formalization scope

  • A distribution is p : ℕ → ℝ with ∀ n, 0 ≤ p n and HasSum p 1; the p.g.f. is the real function pgf p z = ∑' n, p n * z ^ n. All identities between p.g.f.'s are required for real z∈[0,1]z\in[0,1]z∈[0,1] (or [0,1)[0,1)[0,1) for (1.4), (2.4), (2.6), (2.7)), not for complex ∣z∣≤1|z|\le1∣z∣≤1; p.g.f.'s agreeing on [0,1][0,1][0,1] have equal coefficients, so this is equivalent. P′P'P′ is Lean's deriv of pgf p.
  • Infinite divisibility follows Feller: for every n≥1n\ge1n≥1 an nnn-th root that is the p.g.f. of a distribution on N0\mathbb N_0N0​. It is not defined as rn≥0r_n\ge0rn​≥0 or as the form (1.3); those are Lemma 1.2.
  • The canonical sequence is defined by the recursion rn=((n+1)pn+1−∑k=1npkrn−k)/p0r_n=((n+1)p_{n+1}-\sum_{k=1}^np_kr_{n-k})/p_0rn​=((n+1)pn+1​−∑k=1n​pk​rn−k​)/p0​; every statement using it assumes p0>0p_0>0p0​>0.
  • The standing assumption 0<p0<10<p_0<10<p0​<1 of §2 is a hypothesis of Theorem 2.2 and of the §2 milestones.
  • The improper integrals in (1.4) and (2.4) carry an explicit integrability clause on (z,1)(z,1)(z,1), and the series RRR an explicit convergence clause on [0,1)[0,1)[0,1). Lean's integral of a non-integrable function, and the sum of a divergent series, are 000; without these clauses the forms (1.4) and (2.4) could hold vacuously, so a formalization that drops them does not state the theorem.
  • Uniqueness of (λ,G)(\lambda,G)(λ,G) in (1.3) and (2.4) is part of the statements.

Reusable beyond this mission: the p.g.f. and infinite-divisibility vocabulary, Lemma 1.2 (compound Poisson characterization), and Lemma 1.1. A continuity theorem for p.g.f.'s on N0\mathbb N_0N0​, and the uniqueness of power-series coefficients from values on [0,1)[0,1)[0,1), are welcome as independent contributions.

Selected references

  • F. W. Steutel, K. van Harn, Discrete analogues of self-decomposability and stability, Memorandum COSOR 78-07, Technische Hogeschool Eindhoven, 1978. https://pure.tue.nl/ws/files/1719387/340666.pdf — published as Ann. Probab. 7(5) (1979) 893–899. https://doi.org/10.1214/aop/1176994950
  • W. Feller, An Introduction to Probability Theory and Its Applications, vol. 1, 3rd ed., Wiley, New York, 1968 (XII.2; continuity theorem p. 280).
  • F. W. Steutel, On the zeros of infinitely divisible densities, Ann. Math. Statist. 42 (1971) 812–815.
  • K. van Harn, F. W. Steutel, Generalized renewal sequences and infinitely divisible lattice distributions, Stochastic Process. Appl. 5 (1977) 47–55.
  • M. A. Al-Osh, A. A. Alzaid, First-order integer-valued autoregressive (INAR(1)) process, J. Time Series Anal. 8 (1987) 261–275. https://doi.org/10.1111/j.1467-9892.1987.tb00438.x
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Optimization·Captain: mikedeng1

Semismooth and Semiconvex Functions in Constrained Optimization I: The Pointwise Maximum or Minimum over a Compact Family of Continuously Differentiable Functions Is SemismoothResearch Paper

Motivation

Many objective functions in engineering design, Chebyshev approximation and game-theoretic planning are extremal-valued: they are the pointwise maximum or minimum of a family of smooth functions, E(x)=max⁡u∈Uf(x,u)E(x)=\max_{u\in U} f(x,u)E(x)=maxu∈U​f(x,u). Such a function is typically not differentiable at points where two or more members of the family are active, so gradient methods do not apply directly. In 1976 R. Mifflin introduced the class of semismooth functions to identify which nondifferentiable functions can be minimized by bundle-type and line-search methods whose convergence relies only on generalized gradients (Mifflin, IIASA RR-76-21; journal version SIAM J. Control Optim. 15 (1977), doi:10.1137/0315061). For that class to be useful it must contain the functions that actually occur in practice. §3 of the report shows that it contains min–max objectives, which is the content of this mission.

Background: F. H. Clarke defined the generalized gradient of a locally Lipschitz function and computed it for max functions (Clarke, Trans. AMS 205 (1975), Theorem 2.1). A. Feuer's Columbia dissertation (1974) proved the formulas of Theorem 1 below under stronger assumptions and a result close to semismoothness, from which Mifflin's proof of Theorem 2 is adapted (report, Remark, p. 8). Mifflin's notion of semismoothness was later extended to vector-valued maps by Qi and Sun (1993), where it became the standard hypothesis for superlinear convergence of nonsmooth Newton methods.

Setting

Let Rn\mathbb R^nRn carry the Euclidean inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ and norm ∣⋅∣|\cdot|∣⋅∣, and let F:Rn→RF:\mathbb R^n\to\mathbb RF:Rn→R. FFF is Lipschitz on a set BBB if ∣F(y)−F(z)∣≤K∣y−z∣|F(y)-F(z)|\le K|y-z|∣F(y)−F(z)∣≤K∣y−z∣ for all y,z∈By,z\in By,z∈B. Clarke's generalized directional derivative is

F0(x;d)=lim sup⁡h→0, t↓0F(x+h+td)−F(x+h)t,F^0(x;d)=\limsup_{h\to 0,\ t\downarrow 0}\frac{F(x+h+td)-F(x+h)}{t},F0(x;d)=h→0, t↓0limsup​tF(x+h+td)−F(x+h)​,

and the generalized gradient is ∂F(x)={g:⟨g,d⟩≤F0(x;d) ∀d}\partial F(x)=\{g:\langle g,d\rangle\le F^0(x;d)\ \forall d\}∂F(x)={g:⟨g,d⟩≤F0(x;d) ∀d}. When lim⁡t↓0[F(x+td)−F(x)]/t\lim_{t\downarrow 0}[F(x+td)-F(x)]/tlimt↓0​[F(x+td)−F(x)]/t exists it is the directional derivative F′(x;d)F'(x;d)F′(x;d); FFF is quasidifferentiable at xxx if F′(x;d)F'(x;d)F′(x;d) exists and equals F0(x;d)F^0(x;d)F0(x;d) for all ddd.

FFF is semismooth at xxx (Definition 1) if it is Lipschitz on a ball about xxx and, for each ddd and all sequences tk↓0t_k\downarrow 0tk​↓0, θk\theta_kθk​ with θk/tk→0\theta_k/t_k\to 0θk​/tk​→0, and gk∈∂F(x+tkd+θk)g_k\in\partial F(x+t_kd+\theta_k)gk​∈∂F(x+tk​d+θk​), the real sequence ⟨gk,d⟩\langle g_k,d\rangle⟨gk​,d⟩ has exactly one accumulation point. FFF is semiconvex at xxx with respect to XXX (Definition 2) if it is Lipschitz on a ball about xxx, quasidifferentiable at xxx, and x+d∈Xx+d\in Xx+d∈X, F′(x;d)≥0F'(x;d)\ge 0F′(x;d)≥0 imply F(x+d)≥F(x)F(x+d)\ge F(x)F(x+d)≥F(x).

In §3, B⊆RnB\subseteq\mathbb R^nB⊆Rn is open, TTT is a topological space, U⊆TU\subseteq TU⊆T is sequentially compact, f:Rn×T→Rf:\mathbb R^n\times T\to\mathbb Rf:Rn×T→R, and E:Rn→RE:\mathbb R^n\to\mathbb RE:Rn→R satisfies either (d) E(x)=max⁡u∈Uf(x,u)E(x)=\max_{u\in U}f(x,u)E(x)=maxu∈U​f(x,u) on BBB or (d′) E(x)=min⁡u∈Uf(x,u)E(x)=\min_{u\in U}f(x,u)E(x)=minu∈U​f(x,u) on BBB. The active set is A(x)={u∈U:E(x)=f(x,u)}A(x)=\{u\in U:E(x)=f(x,u)\}A(x)={u∈U:E(x)=f(x,u)}, and ∂xf(x,u)\partial_x f(x,u)∂x​f(x,u) is the generalized gradient of f(⋅,u)f(\cdot,u)f(⋅,u) at xxx. Hypotheses (a)–(c) ask that fff be continuous on B×UB\times UB×U, Lipschitz in xxx uniformly in uuu, and that ∂xf\partial_x f∂x​f be upper semicontinuous on B×UB\times UB×U; (e) and (e′) ask that fx′(x,u;d)f'_x(x,u;d)fx′​(x,u;d) exist and equal fx0(x,u;d)f^0_x(x,u;d)fx0​(x,u;d), respectively −fx0(x,u;−d)-f^0_x(x,u;-d)−fx0​(x,u;−d).

Formalization targets

Goal: Theorem 2 (p. 8)

If (a) holds, EEE has the max form (d) or the min form (d′), f(⋅,u)f(\cdot,u)f(⋅,u) is differentiable on BBB for each u∈Uu\in Uu∈U, and ∇xf\nabla_x f∇x​f is continuous and bounded on B×UB\times UB×U, then

E is semismooth on B.E\ \text{is semismooth on } B.E is semismooth on B.

Milestones

  • Proposition 1(a), (b), (d) (p. 3): ∂F(x)\partial F(x)∂F(x) is nonempty, convex and compact; F0(x;d)=max⁡{⟨g,d⟩:g∈∂F(x)}F^0(x;d)=\max\{\langle g,d\rangle:g\in\partial F(x)\}F0(x;d)=max{⟨g,d⟩:g∈∂F(x)}; ∂F\partial F∂F is bounded by the Lipschitz constant and upper semicontinuous.
  • Theorem 1 (pp. 7–8), max and min forms: EEE is Lipschitz on BBB,
∂E(x)=conv⁡⋃u∈A(x)∂xf(x,u),E′(x;d)=E0(x;d)=max⁡{⟨g,d⟩:g∈∂xf(x,u), u∈A(x)}\partial E(x)=\operatorname{conv}\bigcup_{u\in A(x)}\partial_x f(x,u),\qquad E'(x;d)=E^0(x;d)=\max\{\langle g,d\rangle:g\in\partial_x f(x,u),\ u\in A(x)\}∂E(x)=convu∈A(x)⋃​∂x​f(x,u),E′(x;d)=E0(x;d)=max{⟨g,d⟩:g∈∂x​f(x,u), u∈A(x)}

in the max form, and E′(x;d)=−E0(x;−d)=min⁡{⋯ }E'(x;d)=-E^0(x;-d)=\min\{\cdots\}E′(x;d)=−E0(x;−d)=min{⋯} in the min form.

  • Two claims from the proof of Theorem 2 (p. 8): the smoothness assumption yields (b), (c), (e), (e′) and ∂xf={∇xf}\partial_x f=\{\nabla_x f\}∂x​f={∇x​f}; and lim sup⁡k⟨gk,d⟩≤E′(x;d)\limsup_k\langle g_k,d\rangle\le E'(x;d)limsupk​⟨gk​,d⟩≤E′(x;d).
  • Theorem 3 (p. 10): a max function of functions semiconvex at xxx is semiconvex at xxx.
  • Propositions 3 and 4 (pp. 5–6): convex, concave and continuously differentiable functions are semismooth, with the corresponding semiconvexity and quasidifferentiability statements.

Significance

Theorem 2 places every min–max objective with continuously differentiable data inside the class on which Mifflin's descent algorithms, and the bundle methods that followed them, are proved to converge. Theorem 1 is the generalized-gradient form of Danskin's theorem, the standard tool for computing subgradients of max functions. Theorem 3 shows that semiconvexity, unlike pseudoconvexity, survives pointwise maximization, which is what the sufficient optimality results of §5 of the report need.

All of these results are proved in the report and in the literature since 1977; none is open. As far as is known, none of them has a machine-checked proof. Mathlib has Fréchet derivatives and convex analysis but no Clarke generalized gradient calculus, no semismoothness and no Danskin-type theorem. A formalization produces those pieces as reusable infrastructure, and checks the report's statements under exactly stated hypotheses. One printed claim already needs a correction (see Formalization scope).

Difficulty

Lipschitz continuity of EEE and the inequality lim sup⁡k⟨gk,d⟩≤E′(x;d)\limsup_k\langle g_k,d\rangle\le E'(x;d)limsupk​⟨gk​,d⟩≤E′(x;d) follow from Theorem 1 and the upper semicontinuity of ∂E\partial E∂E. The difficulty is the matching lower bound: semismoothness asks that the slopes ⟨gk,d⟩\langle g_k,d\rangle⟨gk​,d⟩ along an arbitrary sequence xk=x+tkd+θkx_k=x+t_kd+\theta_kxk​=x+tk​d+θk​, with arbitrary gk∈∂E(xk)g_k\in\partial E(x_k)gk​∈∂E(xk​), not accumulate strictly below E′(x;d)E'(x;d)E′(x;d). A generalized gradient of EEE at xkx_kxk​ is only a convex combination of gradients of the active functions at xkx_kxk​, and the active set can change discontinuously along the sequence. Upper semicontinuity of ∂E\partial E∂E alone does not prevent this; the function x2sin⁡(1/x)x^2\sin(1/x)x2sin(1/x) (p. 6) is Lipschitz and has an upper semicontinuous ∂F\partial F∂F but is not semismooth at 000. The argument has to use the continuity of ∇xf\nabla_x f∇x​f jointly in (x,u)(x,u)(x,u) and the compactness of UUU. Theorem 1 itself needs a mean value theorem for Lipschitz functions and a compactness argument over the active set, neither of which is in Mathlib in this form.

Formalization scope

Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n). F0F^0F0 is the published ClarkeGradients.Shared.genDirDeriv, a real limsup; every statement assumes the Lipschitz hypothesis of the page at the points where F0F^0F0 or ∂F\partial F∂F is used, so that this limsup is the true value. ∂F\partial F∂F is the support-set definition of the page, not Clarke's convex hull of gradient limits; the two coincide by Proposition 1(c), which is not assumed. F′(x;d)F'(x;d)F′(x;d) is a relation (HasDirDeriv), so "F′(x;d)≥0F'(x;d)\ge 0F′(x;d)≥0" means "exists and is nonnegative". "Exactly one accumulation point" is a unique cluster point, not convergence. "tk↓0t_k\downarrow 0tk​↓0" is read as "positive and tending to 000", as the report reads it in the proof of Lemma 2. "max" and "min" are attained extrema (IsGreatest, IsLeast), never suprema with default values.

EEE is a given function constrained by (d) or (d′), not a supremum; this rules out the trivializing formalization in which EEE is defined as ⨆ u ∈ U, f x u and takes the default value 000 for an empty or unbounded family. (d) and (d′) force U≠∅U\neq\emptysetU=∅. The page's "for each x∈Bx\in Bx∈B either (d) and (e) or (d′) and (e′)" is read as one form on all of BBB, as the proof of Theorem 2 treats it, and Theorem 1 is stated as two items. Hypothesis (c) is the sequential accumulation-point form in which Proposition 1(d) glosses upper semicontinuity.

The goal does not assume (b), (c), (e), (e′) or convexity of BBB; the report derives the first four from smoothness. The report claims (b) on all of BBB, which fails for non-convex open BBB (a bounded gradient gives a uniform Lipschitz constant only on convex sets). The corresponding milestone states (b) on balls contained in BBB, which is all the proof needs.

The development needs Clarke's calculus for Lipschitz functions on Rn\mathbb R^nRn (Propositions 1 and 2, a Lebourg mean value theorem), a Danskin-type theorem, and the regularity of C1C^1C1 functions. These are reusable well beyond this mission; a companion mission of the series covers Propositions 1(c), 2 and the chain rule. Contributions are welcome on any milestone, including alternative proofs of Theorem 1.

Selected references

  • R. Mifflin, Semismooth and semiconvex functions in constrained optimization, IIASA Research Report RR-76-21, December 1976. https://pure.iiasa.ac.at/id/eprint/524/ (journal version: SIAM J. Control Optim. 15(6) (1977) 959–972, https://doi.org/10.1137/0315061).
  • F. H. Clarke, Generalized gradients and applications, Trans. Amer. Math. Soc. 205 (1975) 247–262. https://doi.org/10.1090/S0002-9947-1975-0367131-6
  • A. Feuer, An Implementable Mathematical Programming Algorithm for Admissible Fundamental Functions, Ph.D. dissertation, Department of Mathematics, Columbia University, 1974.
  • G. Lebourg, Valeur moyenne pour gradient généralisé, C. R. Acad. Sci. Paris Sér. A 281 (1975) 795–797.
  • L. Qi and J. Sun, A nonsmooth version of Newton's method, Math. Programming 58 (1993) 353–367. https://doi.org/10.1007/BF01581275
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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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Operations ResearchOptimization·Captain: mikedeng1

Extrapolated Proximal Subgradient Algorithms for Nonconvex and Nonsmooth Fractional Programs 3: Enhanced e-PSG Cluster Points Are Strong Lifted Stationary Points for Max-Type DenominatorsResearch Paper

Motivation

Fractional programs minimize a ratio f(x)/g(x)f(x)/g(x)f(x)/g(x) over a constraint set. They arise whenever a quantity has to be normalized: the scale-invariant sparse recovery model minimizes ∥x∥1/∥x∥2\|x\|_1/\|x\|_2∥x∥1​/∥x∥2​ (Rahimi, Wang, Dong, Lou 2019), robust Sharpe-ratio portfolio selection maximizes a mean-to-worst-case-risk ratio, and generalized eigenvalue problems minimize Rayleigh quotients. Classical methods such as Dinkelbach's algorithm assume convex fff and concave ggg; many modern instances have neither.

Boţ, Dao and Li (arXiv:2003.04124, Math. Oper. Res. 2022) study the nonconvex nonsmooth case in which the numerator is a smooth convex part plus a lower semicontinuous part and the denominator is weakly convex on the constraint set. Their basic method, the extrapolated proximal subgradient (e-PSG) algorithm, converges subsequentially to lifted stationary points. When the denominator is a maximum of finitely many smooth functions, a lifted stationary point may be spurious: it only requires one element of the subdifferential of ggg to balance the numerator. Section 6 of the paper proposes an enhanced algorithm, in the spirit of the enhanced DC algorithm of Pang, Razaviyayn, Alvarado 2017, whose cluster points satisfy the stronger condition for all such elements. This mission formalizes that result.

Setting

HHH is a finite-dimensional real Hilbert space, S⊆HS\subseteq HS⊆H is nonempty, closed and convex, and the problem is

min⁡x∈S f(x)g(x).(P)\min_{x\in S}\ \frac{f(x)}{g(x)} .\qquad (P)x∈Smin​ g(x)f(x)​.(P)
  • Numerator (Assumption 1). f=fs+fnf=f^{\mathfrak s}+f^{\mathfrak n}f=fs+fn, where fs:H→Rf^{\mathfrak s}:H\to\mathbb Rfs:H→R is convex and continuously differentiable with an ℓ\ellℓ-Lipschitz gradient, fn:H→(−∞,+∞]f^{\mathfrak n}:H\to(-\infty,+\infty]fn:H→(−∞,+∞] is proper and lower semicontinuous, S∩dom⁡f≠∅S\cap\operatorname{dom}f\neq\emptysetS∩domf=∅, and f≥0f\ge0f≥0 on S∩dom⁡fS\cap\operatorname{dom}fS∩domf.
  • Denominator (Assumption 2′). g=max⁡{gi:1≤i≤p}g=\max\{g_i:1\le i\le p\}g=max{gi​:1≤i≤p}, each gig_igi​ continuously differentiable on an open set containing SSS and weakly convex on SSS with modulus β≥0\beta\ge0β≥0, meaning gi+β2∥⋅∥2g_i+\frac\beta2\|\cdot\|^2gi​+2β​∥⋅∥2 is convex on SSS. The boundedness condition (BC) holds: m≤g≤Mm\le g\le Mm≤g≤M on S∩dom⁡fS\cap\operatorname{dom}fS∩domf for some m,M>0m,M>0m,M>0.
  • Active sets. Iε(x)={i:gi(x)≥g(x)−ε}I_\varepsilon(x)=\{i: g_i(x)\ge g(x)-\varepsilon\}Iε​(x)={i:gi​(x)≥g(x)−ε}; I0(x)I_0(x)I0​(x) is the set of indices attaining the maximum.
  • Subdifferentials. ∂L\partial_L∂L​ is the limiting (Mordukhovich) subdifferential, and ιS\iota_SιS​ is the indicator of SSS.
  • Strong lifted stationarity (Definition 3.1(iii)). xˉ∈S\bar x\in Sxˉ∈S is a strong lifted stationary point if f(xˉ) ∂Lg(xˉ)⊆g(xˉ) ∂L(f+ιS)(xˉ)f(\bar x)\,\partial_L g(\bar x)\subseteq g(\bar x)\,\partial_L(f+\iota_S)(\bar x)f(xˉ)∂L​g(xˉ)⊆g(xˉ)∂L​(f+ιS​)(xˉ).

Algorithm 2 starts from x−1=x0∈S∩dom⁡fx_{-1}=x_0\in S\cap\operatorname{dom}fx−1​=x0​∈S∩domf. At step nnn it sets θn=f(xn)/g(xn)\theta_n=f(x_n)/g(x_n)θn​=f(xn​)/g(xn​), picks a step size τn\tau_nτn​ and extrapolation weights κn∈[0,κˉ]\kappa_n\in[0,\bar\kappa]κn​∈[0,κˉ], μn∈[0,μˉτn]\mu_n\in[0,\bar\mu\tau_n]μn​∈[0,μˉ​τn​], and forms un=xn+κn(xn−xn−1)u_n=x_n+\kappa_n(x_n-x_{n-1})un​=xn​+κn​(xn​−xn−1​) and vn=xn+μn(xn−xn−1)v_n=x_n+\mu_n(x_n-x_{n-1})vn​=xn​+μn​(xn​−xn−1​). For every i∈Iε(xn)i\in I_\varepsilon(x_n)i∈Iε​(xn​) it computes a proximal candidate

wni∈argmin⁡x∈S(fn(x)+⟨∇fs(un),x⟩+12τn∥x−vn−τnθn∇gi(xn)∥2+ℓ2∥x−un∥2)w_n^{i}\in\operatorname*{argmin}_{x\in S}\Big(f^{\mathfrak n}(x)+\langle\nabla f^{\mathfrak s}(u_n),x\rangle+\tfrac1{2\tau_n}\|x-v_n-\tau_n\theta_n\nabla g_i(x_n)\|^2+\tfrac\ell2\|x-u_n\|^2\Big)wni​∈x∈Sargmin​(fn(x)+⟨∇fs(un​),x⟩+2τn​1​∥x−vn​−τn​θn​∇gi​(xn​)∥2+2ℓ​∥x−un​∥2)

(up to constants), and keeps as xn+1x_{n+1}xn+1​ the candidate minimizing the merit value f(w)−θng(w)+12(1−βζτn−MμnmMτn)∥w−xn∥2f(w)-\theta_n g(w)+\frac12\big(\frac{1-\sqrt\beta\zeta}{\tau_n}-\frac{M\mu_n}{\sqrt{mM}\tau_n}\big)\|w-x_n\|^2f(w)−θn​g(w)+21​(τn​1−β​ζ​−mM​τn​Mμn​​)∥w−xn​∥2.

Formalization targets

Goal: Theorem 6.1(iii)

Assume the sublevel set S0={x∈S:f(x)/g(x)≤f(x0)/g(x0)}S_0=\{x\in S: f(x)/g(x)\le f(x_0)/g(x_0)\}S0​={x∈S:f(x)/g(x)≤f(x0​)/g(x0​)} is bounded and lim inf⁡nτn=τˉ>0\liminf_n\tau_n=\bar\tau>0liminfn​τn​=τˉ>0. Then every cluster point xˉ\bar xxˉ of (xn)(x_n)(xn​) satisfies xˉ∈S∩dom⁡f\bar x\in S\cap\operatorname{dom}fxˉ∈S∩domf, f(xn)/g(xn)→f(xˉ)/g(xˉ)f(x_n)/g(x_n)\to f(\bar x)/g(\bar x)f(xn​)/g(xn​)→f(xˉ)/g(xˉ),

f(xˉ)g(xˉ)⋃i∈I0(xˉ)∇gi(xˉ)⊆∂L(f+ιS)(xˉ),(28)\frac{f(\bar x)}{g(\bar x)}\bigcup_{i\in I_0(\bar x)}\nabla g_i(\bar x)\subseteq\partial_L(f+\iota_S)(\bar x),\qquad(28)g(xˉ)f(xˉ)​i∈I0​(xˉ)⋃​∇gi​(xˉ)⊆∂L​(f+ιS​)(xˉ),(28)

and, if fff is weakly convex on SSS, xˉ\bar xxˉ is a strong lifted stationary point of (P).

Milestones, in proof order

  1. Lemma 4.4 (descent lemma; already proved on the platform) and Lemma 4.3 (subgradient inequality for weakly convex functions).
  2. Inequality (32): the merit value of xn+1x_{n+1}xn+1​ is at most that of any candidate, which is bounded by a model of fff at any x∈Sx\in Sx∈S.
  3. The one-step decrease of f(xn)/g(xn)f(x_n)/g(x_n)f(xn​)/g(xn​) that follows from (32).
  4. Theorem 6.1(i): xn∈S∩dom⁡fx_n\in S\cap\operatorname{dom}fxn​∈S∩domf, and the sequence Fn=f(xn)/g(xn)+(ℓκˉ22m+μˉ2mM)∥xn−xn−1∥2F_n=f(x_n)/g(x_n)+\big(\frac{\ell\bar\kappa^2}{2m}+\frac{\bar\mu}{2\sqrt{mM}}\big)\|x_n-x_{n-1}\|^2Fn​=f(xn​)/g(xn​)+(2mℓκˉ2​+2mM​μˉ​​)∥xn​−xn−1​∥2 of (27) is nonincreasing and convergent.
  5. Theorem 6.1(ii): the iterates are bounded and ∑n∥xn+1−xn∥2<+∞\sum_n\|x_{n+1}-x_n\|^2<+\infty∑n​∥xn+1​−xn​∥2<+∞.
  6. The limit inequality at a cluster point, and inclusion (34) (= (28)).
  7. Lemma 2.2(i): ∂L(h+ιS)\partial_L(h+\iota_S)∂L​(h+ιS​) is closed and convex for weakly convex hhh.

Significance

For max-type denominators the result separates the enhanced algorithm from the basic one. A lifted stationary point only needs 0∈g(xˉ)∂L(f+ιS)(xˉ)−f(xˉ)∂Lg(xˉ)0\in g(\bar x)\partial_L(f+\iota_S)(\bar x)-f(\bar x)\partial_L g(\bar x)0∈g(xˉ)∂L​(f+ιS​)(xˉ)−f(xˉ)∂L​g(xˉ). The paper's Example 3.3 (min⁡∣x∣≤1(x2+1)/(∣x∣+1)\min_{|x|\le1}(x^2+1)/(|x|+1)min∣x∣≤1​(x2+1)/(∣x∣+1)) has the lifted stationary point 000, which is not a local minimizer; the strong lifted stationary points of that example are exactly its minimizers. Lemma 3.4 of the paper identifies strong lifted stationarity with d-stationarity of f−f(xˉ)g(xˉ)gf-\frac{f(\bar x)}{g(\bar x)}gf−g(xˉ)f(xˉ)​g on SSS when f+ιSf+\iota_Sf+ιS​ and ggg are weakly convex. This is the sharpest first-order notion used for DC-type programs.

The theorem is proved in the paper (pp. 22–24). No machine-checked version of it, of the e-PSG analysis, or of lifted stationarity exists on the platform. Formalizing it checks the step-size bookkeeping that the printed algorithm gets wrong (see below). It also produces reusable statements about weakly convex functions and the limiting subdifferential of h+ιSh+\iota_Sh+ιS​.

Difficulty

The descent part follows the template of the basic e-PSG analysis, but the merit criterion couples the candidate selection with the extrapolation: the coefficient 1−βζτn−MμnmMτn\frac{1-\sqrt\beta\zeta}{\tau_n}-\frac{M\mu_n}{\sqrt{mM}\tau_n}τn​1−β​ζ​−mM​τn​Mμn​​ has to stay positive, and the cross term ⟨w−xn,xn−xn−1⟩\langle w-x_n,x_n-x_{n-1}\rangle⟨w−xn​,xn​−xn−1​⟩ has to be split with the specific weight m/M\sqrt{m/M}m/M​ for the constants of (27) to close.

The limit step is the main obstacle. The algorithm works with Iε(xn)I_\varepsilon(x_n)Iε​(xn​), but the conclusion concerns I0(xˉ)I_0(\bar x)I0​(xˉ) at a limit point. One must show that every index active at xˉ\bar xxˉ was a candidate along the subsequence. One must also show that f(xkn+1)→f(xˉ)f(x_{k_n+1})\to f(\bar x)f(xkn​+1​)→f(xˉ) although fff is only lower semicontinuous. The naive approach, passing to the limit in the optimality condition of a single subproblem, gives one element of ∂Lg(xˉ)\partial_L g(\bar x)∂L​g(xˉ) only, which is lifted stationarity again. The final step needs the limiting subdifferential of a finite max of C1C^1C1 functions to be the convex hull of the active gradients. The paper uses this fact without proof, and Mathlib does not provide it for ∂L\partial_L∂L​.

Formalization scope

  • Carrier. HHH is EuclideanSpace ℝ (Fin N). Functions into (−∞,+∞](-\infty,+\infty](−∞,+∞] are EReal-valued. ∂L\partial_L∂L​ is the published NonconvexSplitting.Shared.LimitingSubdiff, and properness is IsProperFn.
  • Indices and the max. Indices are Fin p with p≥1p\ge1p≥1, so they run 0,…,p−10,\dots,p-10,…,p−1. ggg is defined as Finset.sup' of the gig_igi​, never as an independent function. The standing assumptions of (P) are kept: ggg is lower semicontinuous and positive on SSS.
  • Weak convexity. "Modulus" means "a valid constant". For real gig_igi​ it is ConvexOn of gi+β2∥⋅∥2g_i+\frac\beta2\|\cdot\|^2gi​+2β​∥⋅∥2 on SSS. For extended-real fff it is convexity of the epigraph of f+ιS+ρ2∥⋅∥2f+\iota_S+\frac\rho2\|\cdot\|^2f+ιS​+2ρ​∥⋅∥2.
  • Algorithm 2. A run is a predicate on iterates, candidates, selected indices, step sizes and weights. Each argmin is "some minimizer", candidates outside Iε(xn)I_\varepsilon(x_n)Iε​(xn​) are unconstrained, x−1=x0x_{-1}=x_0x−1​=x0​, and ratios are real numbers on S∩dom⁡fS\cap\operatorname{dom}fS∩domf.
  • Two misprints corrected. Step 1 declares an unused ω\omegaω and never declares ε\varepsilonε; it is read as ε>0\varepsilon>0ε>0. The printed step-size rule τn≤1/max⁡{βθn/(1−ζ),δ}\tau_n\le1/\max\{\beta\theta_n/(1-\zeta),\delta\}τn​≤1/max{βθn​/(1−ζ),δ} does not give the inequality βθn≤βζ/τn\beta\theta_n\le\sqrt\beta\zeta/\tau_nβθn​≤β​ζ/τn​ that the proof uses. The run therefore uses τn≤1/max⁡{βθn/ζ,δ}\tau_n\le1/\max\{\sqrt\beta\theta_n/\zeta,\delta\}τn​≤1/max{β​θn​/ζ,δ}, the rule of Algorithm 1.
  • Other conventions. τˉ\bar\tauτˉ is Filter.liminf τ atTop, which is well defined because 0<τn≤1/δ0<\tau_n\le1/\delta0<τn​≤1/δ. The κˉ\bar\kappaκˉ-range is multiplied out to avoid dividing by ℓ\ellℓ.
  • Ruled out. The theorem cannot be satisfied trivially: the run constrains every iterate, and the strong lifted conclusion quantifies over all of ∂Lg(xˉ)\partial_L g(\bar x)∂L​g(xˉ). Membership xˉ∈dom⁡f\bar x\in\operatorname{dom}fxˉ∈domf is concluded explicitly, so the toReal value of +∞+\infty+∞ never enters.
  • Needed infrastructure. The subgradient inequality for weakly convex functions, the convexity of ∂L(h+ιS)\partial_L(h+\iota_S)∂L​(h+ιS​) for weakly convex hhh, a Fermat rule for ∂L\partial_L∂L​, and the formula for ∂Lmax⁡igi\partial_L\max_i g_i∂L​maxi​gi​. Each is reusable beyond this paper, and a contribution of any of them is welcome.

Selected references

  • R. I. Boţ, M. N. Dao, G. Li, Extrapolated proximal subgradient algorithms for nonconvex and nonsmooth fractional programs, arXiv:2003.04124v2 (2020); Math. Oper. Res. 47 (2022). https://arxiv.org/abs/2003.04124
  • J.-S. Pang, M. Razaviyayn, A. Alvarado, Computing B-stationary points of nonsmooth DC programs, Math. Oper. Res. 42(1) (2017). https://doi.org/10.1287/moor.2016.0795
  • Y. Rahimi, C. Wang, H. Dong, Y. Lou, A scale invariant approach for sparse signal recovery, SIAM J. Sci. Comput. 41 (2019). https://arxiv.org/abs/1812.08852
  • B. S. Mordukhovich, Variational Analysis and Generalized Differentiation I, Springer, 2006. https://doi.org/10.1007/3-540-31247-1
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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Operations ResearchOptimization·Captain: mikedeng1

Extrapolated Proximal Subgradient Algorithms for Nonconvex and Nonsmooth Fractional Programs 2: Sufficient Decrease, Multi-Step Relative Error and KL Give Finite Length and Linear RatesResearch Paper

Motivation

Many first-order methods for nonconvex and nonsmooth optimization are analysed with the same template: a merit function decreases by a definite amount at every step, a subgradient of the merit function at the current point is bounded by the step length, and the Kurdyka–Łojasiewicz (KL) property of the merit function turns these two facts into a proof that the whole sequence of iterates has finite length and converges. Attouch and Bolte (Math. Program. 2009), Attouch, Bolte and Svaiter (Math. Program. 2013) and Bolte, Sabach and Teboulle (Math. Program. 2014) isolated this template as a set of abstract conditions. Later frameworks for methods with inertia or extrapolation, such as iPiano (Ochs, Chen, Brox and Pock, SIAM J. Imaging Sci. 2014), needed the relative error bound to involve more than one past step.

Boţ, Dao and Li (arXiv:2003.04124, Math. Oper. Res. 2022) state a framework (H1)–(H5) in which the relative error bound is a convex combination of several step lengths, past or future, plus a summable error, and the iterates of the algorithm may live in a different space from the merit function. They prove finite length, convergence, stationarity and, for KL exponent at most 12\tfrac1221​, linear rates; they then apply it to an extrapolated proximal subgradient method for fractional programs. This mission formalizes that abstract result, Theorem 5.2 of the paper.

Setting

Let H\mathcal HH and K\mathcal KK be finite-dimensional real Hilbert spaces and h:K→(−∞,+∞]h:\mathcal K\to(-\infty,+\infty]h:K→(−∞,+∞] a proper (never −∞-\infty−∞, finite somewhere) lower semicontinuous function. ∂Lh(z)\partial_L h(z)∂L​h(z) denotes the limiting subdifferential of hhh at zzz, empty where h(z)=+∞h(z)=+\inftyh(z)=+∞, and dist⁡(0,∅)=+∞\operatorname{dist}(0,\emptyset)=+\inftydist(0,∅)=+∞.

Data: sequences (xn)(x_n)(xn​) in H\mathcal HH and (zn)(z_n)(zn​) in K\mathcal KK; αn,βn>0\alpha_n,\beta_n>0αn​,βn​>0; Δn,εn≥0\Delta_n,\varepsilon_n\ge0Δn​,εn​≥0, with the convention Δk=0\Delta_k=0Δk​=0 for k<0k<0k<0; integers ı‾≤ıˉ\underline\imath\le\bar\imath​≤ˉ (not necessarily positive), I={ı‾,…,ıˉ}I=\{\underline\imath,\dots,\bar\imath\}I={​,…,ˉ}, and weights λi≥0\lambda_i\ge0λi​≥0 with ∑i∈Iλi=1\sum_{i\in I}\lambda_i=1∑i∈I​λi​=1. The conditions, for all n∈Nn\in\mathbb Nn∈N, are:

  • (H1) sufficient decrease: h(zn+1)+αnΔn2≤h(zn)h(z_{n+1})+\alpha_n\Delta_n^2\le h(z_n)h(zn+1​)+αn​Δn2​≤h(zn​);
  • (H2) relative error: βndist⁡(0,∂Lh(zn))≤∑i∈IλiΔn−i+εn\beta_n\operatorname{dist}(0,\partial_L h(z_n))\le\sum_{i\in I}\lambda_i\Delta_{n-i}+\varepsilon_nβn​dist(0,∂L​h(zn​))≤∑i∈I​λi​Δn−i​+εn​;
  • (H3) continuity: some subsequence zkn→z~z_{k_n}\to\tilde zzkn​​→z~ has h(zkn)→h(z~)h(z_{k_n})\to h(\tilde z)h(zkn​​)→h(z~);
  • (H4) parameters: α‾:=inf⁡αn>0\underline\alpha:=\inf\alpha_n>0α​:=infαn​>0, γ‾:=inf⁡αnβn>0\underline\gamma:=\inf\alpha_n\beta_n>0γ​:=infαn​βn​>0, ∑εn<+∞\sum\varepsilon_n<+\infty∑εn​<+∞;
  • (H5) distance: there are j∈Zj\in\mathbb Zj∈Z, c∈Rc\in\mathbb Rc∈R with ∥xn+1−xn∥≤c Δn+j\|x_{n+1}-x_n\|\le c\,\Delta_{n+j}∥xn+1​−xn​∥≤cΔn+j​.

Ω\OmegaΩ is the set of cluster points of (zn)(z_n)(zn​), Ω0={zˉ∈Ω:h(zn)→h(zˉ)}\Omega_0=\{\bar z\in\Omega:h(z_n)\to h(\bar z)\}Ω0​={zˉ∈Ω:h(zn​)→h(zˉ)}, and hˉ=h(zˉ)\bar h=h(\bar z)hˉ=h(zˉ) for zˉ∈Ω0\bar z\in\Omega_0zˉ∈Ω0​. A desingularizing function φ∈Φη\varphi\in\Phi_\etaφ∈Φη​ is continuous and concave on [0,η)[0,\eta)[0,η), vanishes at 000, and is C1C^1C1 with φ′>0\varphi'>0φ′>0 on (0,η)(0,\eta)(0,η). hhh has the KL property at zˉ\bar zzˉ if for some neighbourhood UUU of zˉ\bar zzˉ, η>0\eta>0η>0 and φ∈Φη\varphi\in\Phi_\etaφ∈Φη​, φ′(h(z)−h(zˉ))dist⁡(0,∂Lh(z))≥1\varphi'(h(z)-h(\bar z))\operatorname{dist}(0,\partial_L h(z))\ge1φ′(h(z)−h(zˉ))dist(0,∂L​h(z))≥1 whenever z∈Uz\in Uz∈U and h(zˉ)<h(z)<h(zˉ)+ηh(\bar z)<h(z)<h(\bar z)+\etah(zˉ)<h(z)<h(zˉ)+η; it has the KL property with exponent a∈[0,1)a\in[0,1)a∈[0,1) if φ\varphiφ can be taken as γs1−a\gamma s^{1-a}γs1−a.

Formalization targets

Goal: Theorem 5.2

Assume (H1)–(H4), (zn)(z_n)(zn​) bounded, hhh constant on Ω\OmegaΩ with the KL property at every point of Ω\OmegaΩ. Then

(i) ∑n=0∞Δn<∞;(ii) (H5)⇒∑n=0∞∥xn+1−xn∥<∞ and xn→xˉ;(iii) inf⁡βn>0⇒0∈∂Lh(zˉ)  ∀zˉ∈Ω0;\text{(i)}\ \sum_{n=0}^{\infty}\Delta_n<\infty;\qquad \text{(ii)}\ \text{(H5)}\Rightarrow\sum_{n=0}^{\infty}\|x_{n+1}-x_n\|<\infty \text{ and } x_n\to\bar x;\qquad \text{(iii)}\ \inf\beta_n>0\Rightarrow 0\in\partial_L h(\bar z)\ \ \forall\bar z\in\Omega_0;(i) n=0∑∞​Δn​<∞;(ii) (H5)⇒n=0∑∞​∥xn+1​−xn​∥<∞ and xn​→xˉ;(iii) infβn​>0⇒0∈∂L​h(zˉ)  ∀zˉ∈Ω0​;

(iv) if hhh has KL exponent a≤12a\le\tfrac12a≤21​ on Ω\OmegaΩ, ı‾≤1\underline\imath\le1​≤1, inf⁡n,iαn−iβn2>0\inf_{n,i}\alpha_{n-i}\beta_n^2>0infn,i​αn−i​βn2​>0 and εn/βn=O(h(zn−ıˉ)−h(zn+1−ı‾))\varepsilon_n/\beta_n=O(\sqrt{h(z_{n-\bar\imath})-h(z_{n+1-\underline\imath})})εn​/βn​=O(h(zn−ˉ​)−h(zn+1−​​)​), then for some γ1>0\gamma_1>0γ1​>0, ρ∈(0,1)\rho\in(0,1)ρ∈(0,1),

h(zn)−hˉ≤γ1ρn∀n,h(z_n)-\bar h\le\gamma_1\rho^n\quad\forall n,h(zn​)−hˉ≤γ1​ρn∀n,

and under (H5) and ∑k≥nεk=O(h(zn−ıˉ)−hˉ)\sum_{k\ge n}\varepsilon_k=O(\sqrt{h(z_{n-\bar\imath})-\bar h})∑k≥n​εk​=O(h(zn−ˉ​)−hˉ​), ∥xn−xˉ∥≤γ2ρn/2\|x_n-\bar x\|\le\gamma_2\rho^{n/2}∥xn​−xˉ∥≤γ2​ρn/2 for the same ρ\rhoρ.

Milestones

Lemma 2.3 (uniformized KL along a bounded sequence, and its power form under an exponent); Lemma 5.1(i)–(iii) (nonemptiness of Ω0\Omega_0Ω0​ and monotone convergence of values; ∑Δn2≤(h(z0)−h(zˉ))/α‾\sum\Delta_n^2\le(h(z_0)-h(\bar z))/\underline\alpha∑Δn2​≤(h(z0​)−h(zˉ))/α​; the subgradient bound and stationarity); the tail bound (24) from the proof of (i); Theorem 5.2(i); and the first claim of Theorem 5.2(iv).

Significance

The theorem separates what is specific to an algorithm (checking (H1)–(H5) for its iterates) from what is common to all KL-based analyses (finite length, convergence, rates). In the paper it yields global convergence of the extrapolated proximal subgradient method (Theorem 5.5) with zn=(xn+1,xn)z_n=(x_{n+1},x_n)zn​=(xn+1​,xn​) and I={0,1}I=\{0,1\}I={0,1}, and Remark 5.4 shows that the frameworks of Attouch–Bolte–Svaiter, Bolte–Sabach–Teboulle, Frankel–Garrigos–Peypouquet and iPiano are special cases, while the linear rate for the iterates in the multi-step setting is new relative to those frameworks.

The result is proved on paper. To our knowledge no machine-checked version of this abstract framework exists. A formal proof yields a reusable theorem: any later mission that verifies (H1)–(H5) for a specific method gets convergence and rates by citation. Related single-algorithm KL convergence results on the platform (proximal alternating minimization, PALM, proximal ADMM) each repeat the same argument; this framework is the common abstraction.

Difficulty

The naive argument—sum (H1) to get ∑Δn2<∞\sum\Delta_n^2<\infty∑Δn2​<∞—gives only square-summability, which does not imply convergence of the iterates. Finite length needs the KL inequality along the whole tail of the sequence with one function φ\varphiφ, but the KL property is only pointwise; this requires a uniformization over the (compact) cluster set and the restriction to Ω0\Omega_0Ω0​, where values converge. The multi-step error with possibly negative indices in III means the right-hand side of (H2) can involve future steps, so the telescoping estimate must absorb sums with shifted index ranges. For the rates, the KL exponent turns the inequality into a recursion between rn+1−ı‾r_{n+1-\underline\imath}rn+1−​​ and rn−ıˉr_{n-\bar\imath}rn−ˉ​ separated by several steps, whose contraction must be shown to give a geometric rate.

Formalization scope

H\mathcal HH is EuclideanSpace ℝ (Fin N) and K\mathcal KK is EuclideanSpace ℝ (Fin P); hhh takes values in EReal, with properness and limiting subdifferential from the published NonconvexSplitting.Shared definitions and the KL property (HasKLProperty, IsDesingularizer, KLIneq) from the published NonconvexSplitting.ADMMKL definitions. η\etaη is a positive real. Δ\DeltaΔ is indexed by Z\mathbb ZZ and vanishes on negative integers. dist⁡(0,∂Lh(z))≤r\operatorname{dist}(0,\partial_L h(z))\le rdist(0,∂L​h(z))≤r is encoded as "some v∈∂Lh(z)v\in\partial_L h(z)v∈∂L​h(z) has ∥v∥≤r\|v\|\le r∥v∥≤r", and the KL inequality as "every v∈∂Lh(z)v\in\partial_L h(z)v∈∂L​h(z) satisfies φ′(⋅)∥v∥≥1\varphi'(\cdot)\|v\|\ge1φ′(⋅)∥v∥≥1"; Metric.infDist is never used, because it returns 000 on the empty set where the paper's distance is +∞+\infty+∞, which would make (H2) trivially satisfiable. Infima are encoded by positive lower bounds; O(⋅)O(\cdot)O(⋅) hypotheses as eventual bounds with a constant; hˉ\bar hhˉ by quantifying over Ω0\Omega_0Ω0​. Lemma 5.1(ii) assumes h(z0)<+∞h(z_0)<+\inftyh(z0​)<+∞ explicitly, which the page presupposes.

The definitions file FracPSG.Abstract.Basic (the setting, (H1)–(H5), Ω\OmegaΩ, Ω0\Omega_0Ω0​, the KL exponent) is reusable by any mission that instantiates the framework. Contributions welcome: proofs of the milestones, the uniformized KL lemma in general form, and summation lemmas for sequences indexed by Z\mathbb ZZ.

Selected references

  • R. I. Boţ, M. N. Dao, G. Li, Extrapolated Proximal Subgradient Algorithms for Nonconvex and Nonsmooth Fractional Programs, Math. Oper. Res., 2022; preprint arXiv:2003.04124v2 (2020). https://arxiv.org/abs/2003.04124
  • H. Attouch, J. Bolte, B. F. Svaiter, Convergence of descent methods for semi-algebraic and tame problems, Math. Program. 137, 2013. https://doi.org/10.1007/s10107-011-0484-9
  • J. Bolte, S. Sabach, M. Teboulle, Proximal alternating linearized minimization for nonconvex and nonsmooth problems, Math. Program. 146, 2014. https://doi.org/10.1007/s10107-013-0701-9
  • H. Attouch, J. Bolte, On the convergence of the proximal algorithm for nonsmooth functions involving analytic features, Math. Program. 116, 2009. https://doi.org/10.1007/s10107-007-0133-5
  • P. Ochs, Y. Chen, T. Brox, T. Pock, iPiano: Inertial proximal algorithm for nonconvex optimization, SIAM J. Imaging Sci. 7, 2014. https://doi.org/10.1137/130942954
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Probability·Captain: mikedeng1

Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs? 4: The Correlated Gaussian Orthant Probability Satisfies Λρ(μ) ≤ (1 + ρ)·φ(t)/t·N(t√((1 − ρ)/(1 + ρ)))Research Paper

Motivation

Khot, Kindler, Mossel and O'Donnell, Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs? (SIAM J. Comput. 37(1), 2007), prove that, assuming the Unique Games Conjecture, the Goemans–Williamson approximation ratio for MAX-CUT is optimal, and they extend the method to MAX-q-CUT and to Γ-MAX-2LIN(q). For the q-ary problems the key analytic input is the theorem of Mossel, O'Donnell and Oleszkiewicz (arXiv:math/0503503), the MOO theorem. It bounds the noise stability of a low-influence function with mean µ by a Gaussian quantity, the correlated Gaussian orthant probability Λ_ρ(µ): the probability that two ρ-correlated standard Gaussians both exceed the threshold t at which a single one has tail mass µ.

The hardness bounds of the paper for Γ-MAX-2LIN(q) are stated in terms of Λ_ρ(1/q). They are explicit only after Λ_ρ(µ) is estimated. Proposition 6.1 of the paper gives such an estimate in closed form, by slightly improving a bound from the proof of Lemma 11.1 of de Klerk, Pasechnik and Warners (Approximate graph colouring and MAX-k-CUT algorithms based on the theta function, J. Combin. Optim., 2004). The same quantity at µ = 1/2 is Sheppard's orthant probability (Phil. Trans. R. Soc. A 192, 1899), the source of the arccos formulas used throughout the MAX-CUT part of the paper.

This mission formalizes Proposition 6.1 and the steps of its printed proof.

Setting

Let φ be the standard Gaussian density and N the Gaussian tail probability function:

ϕ(x)=12πe−x2/2,N(x)=∫x∞ϕ(s) ds.\phi(x)=\frac{1}{\sqrt{2\pi}}e^{-x^2/2},\qquad N(x)=\int_x^\infty \phi(s)\,ds .ϕ(x)=2π​1​e−x2/2,N(x)=∫x∞​ϕ(s)ds.

So N(x) = Pr[X ≥ x] for a standard Gaussian X. N is strictly decreasing from 1 to 0, and N(0) = 1/2.

Let X and Y be independent standard Gaussian random variables. For ρ ∈ [0, 1] put

X′=ρX+1−ρ2 Y.X'=\rho X+\sqrt{1-\rho^2}\,Y .X′=ρX+1−ρ2​Y.

Then (X, X′) is a centred normal pair with unit variances and covariance ρ, the pair of Definition 8 of the paper. For 0 < µ < 1 let t be the unique real number with Pr[X ≥ t] = µ, and define

Λρ(μ)=Pr⁡[X≥t and X′≥t].\Lambda_\rho(\mu)=\Pr[X\ge t\ \text{and}\ X'\ge t].Λρ​(μ)=Pr[X≥t and X′≥t].

The threshold t is positive exactly when µ < 1/2. Λ_ρ(µ) is the noise stability, in Gaussian space, of the indicator of a half-line of measure µ.

The proof uses two exponents. For u, v ∈ ℝ, with ρ < 1 and t > 0,

g(u,v)=u+v1+ρ+(u−v)2+2(1−ρ)uv2(1−ρ2)t2,h(u,v)=u+v1+ρ+(u−v)22(1−ρ2)t2.g(u,v)=\frac{u+v}{1+\rho}+\frac{(u-v)^2+2(1-\rho)uv}{2(1-\rho^2)t^2},\qquad h(u,v)=\frac{u+v}{1+\rho}+\frac{(u-v)^2}{2(1-\rho^2)t^2}.g(u,v)=1+ρu+v​+2(1−ρ2)t2(u−v)2+2(1−ρ)uv​,h(u,v)=1+ρu+v​+2(1−ρ2)t2(u−v)2​.

In Lean these are phi, tailN, orthantProb ρ t, Lambda ρ μ, gExp ρ t u v and hExp ρ t u v in the namespace OptInapprox.Orthant.

Formalization targets

Goal: Proposition 6.1 (p. 14)

For any 0 ≤ µ < 1/2, let t > 0 be the number with N(t) = µ. Then for all 0 ≤ ρ ≤ 1,

Λρ(μ) ≤ (1+ρ)⋅ϕ(t)t⋅N ⁣(t1−ρ1+ρ).(4)\Lambda_\rho(\mu)\ \le\ (1+\rho)\cdot\frac{\phi(t)}{t}\cdot N\!\Big(t\sqrt{\tfrac{1-\rho}{1+\rho}}\Big).\tag{4}Λρ​(μ) ≤ (1+ρ)⋅tϕ(t)​⋅N(t1+ρ1−ρ​​).(4)

The endpoint ρ = 1 is part of the goal. There X′ = X, Λ₁(µ) = µ, and (4) becomes the classical Mills-ratio inequality N(t) ≤ φ(t)/t.

Milestones (proof of Proposition 6.1, pp. 30–31)

  1. (18). For 0 ≤ ρ < 1, t > 0 and µ = N(t),
Λρ(μ)=12π1−ρ2⋅t2exp⁡(−t21+ρ)∫0∞ ⁣ ⁣∫0∞e−g(u,v) du dv.\Lambda_\rho(\mu)=\frac{1}{2\pi\sqrt{1-\rho^2}\cdot t^2}\exp\Big(-\frac{t^2}{1+\rho}\Big)\int_0^\infty\!\!\int_0^\infty e^{-g(u,v)}\,du\,dv .Λρ​(μ)=2π1−ρ2​⋅t21​exp(−1+ρt2​)∫0∞​∫0∞​e−g(u,v)dudv.
  1. g ≥ h on u, v ≥ 0.
  2. (19)–(20).
∫0∞ ⁣ ⁣∫0∞e−g≤∫0∞ ⁣ ⁣∫0∞e−h=2π(1+ρ)1−ρ2⋅t⋅exp⁡(1−ρ1+ρ⋅t22)⋅N(t1−ρ1+ρ).\int_0^\infty\!\!\int_0^\infty e^{-g}\le\int_0^\infty\!\!\int_0^\infty e^{-h}=\sqrt{2\pi}(1+\rho)\sqrt{1-\rho^2}\cdot t\cdot\exp\Big(\frac{1-\rho}{1+\rho}\cdot\frac{t^2}{2}\Big)\cdot N\Big(t\sqrt{\tfrac{1-\rho}{1+\rho}}\Big).∫0∞​∫0∞​e−g≤∫0∞​∫0∞​e−h=2π​(1+ρ)1−ρ2​⋅t⋅exp(1+ρ1−ρ​⋅2t2​)⋅N(t1+ρ1−ρ​​).
  1. Lower bound (side note in the proof of Corollary 10, p. 31):
μ⋅N(t1−ρ1+ρ)≤Λρ(μ).\mu\cdot N\Big(t\sqrt{\tfrac{1-\rho}{1+\rho}}\Big)\le\Lambda_\rho(\mu).μ⋅N(t1+ρ1−ρ​​)≤Λρ​(μ).

Significance

Proposition 6.1 makes the MOO theorem quantitative for thresholds. With the lower bound of milestone 4 it determines Λ_ρ(µ) up to the factor 1 + ρ, and up to 1 + o(1) as µ → 0, since φ(t)/t ∼ N(t) as t → ∞ (Corollary 10, part 1). Through Corollary 10 it yields the asymptotics of qΛ_ρ(1/q) used in the paper's hardness results for MAX-q-CUT and Γ-MAX-2LIN(q). These quantities also appear in later work on q-ary noise stability and on the approximability of 2-CSPs.

The proposition is proved in the paper; nothing here is open. Mathlib (at the pinned revision) contains no proof of it, of the bivariate-normal integral representation (18), or of the Mills-ratio inequality N(t) ≤ φ(t)/t. On the platform, Mills' inequality appears only as an open statement in the two-sided form Pr[|X| > z] ≤ √(2/π)·e^{−z²/2}/z (KLTNuclear.Lasso.gaussian_tail), and there is no item for orthant probabilities. A complete development provides:

  • the substitution x = t + u/t, y = t + v/t in the bivariate normal density;
  • a closed-form quadrant integral after the rotation r = u + v, s = u − v;
  • the identification of a probability under a product Gaussian measure with an explicit double integral.

Each of these is reusable for Gaussian tail and orthant estimates.

Difficulty

The inequality itself is elementary once (18) and (20) are available. The work lies in the two integral identities and in their measure-theoretic glue.

For (18), the orthant probability is defined as a measure of a set under the product of two one-dimensional Gaussian laws. Writing it as a double integral of the bivariate density is a linear change of variables with Jacobian √(1 − ρ²). The shift and scaling by t then has Jacobian 1/t², and the quadratic form has to be expanded exactly.

For (20), the region u, v ≥ 0 becomes the wedge |s| ≤ r after the rotation, so the inner integral is a truncated Gaussian integral rather than a full one. The closed form appears only after an integration by parts in r, or an equivalent completion of the square.

The endpoint ρ = 1 is not covered by the printed argument, because (18) divides by √(1 − ρ²). It needs Mills' inequality separately. A proof that only treats ρ < 1 does not close the goal.

Formalization scope

  • Gaussian law. Λ_ρ(µ) is a genuine probability. stdGaussPair is the product of two copies of Mathlib's gaussianReal 0 1 on ℝ × ℝ. orthantProb ρ t is the real-valued measure of {X ≥ t, ρX + √(1 − ρ²)Y ≥ t}, which is the representation the paper itself uses on p. 31.
  • Choice of t. Lambda ρ μ chooses a t with Pr[X ≥ t] = µ, where the probability is taken under gaussianReal 0 1. Such a t is unique, so the choice does not matter. For µ ∉ (0, 1) no such t exists and the value is a placeholder 0 that no statement uses.
  • Hypotheses of the statements. Every theorem takes t > 0 and N(t) = µ as hypotheses, as Proposition 6.1 does; the redundant 0 ≤ µ < 1/2 is kept as printed.
  • Functions. φ is written out explicitly and N is the Bochner integral of φ over (x, ∞).
  • Integrals. The double integrals of (18)–(20) are iterated integrals over (0, ∞), inner variable u, as printed. Milestone 3 also asserts that e^{−h} is integrable on the quadrant, so (19) cannot hold through a junk zero integral.
  • Range of ρ. The goal and milestone 4 take 0 ≤ ρ ≤ 1, as on the page. Milestones 1–3 take 0 ≤ ρ < 1, because their constants divide by √(1 − ρ²) or 1 − ρ², and the printed proof uses them only there. This is the only hypothesis added relative to the page.
  • Trivializing formalizations, ruled out.
    • Defining Λ_ρ(µ) by the right-hand side of (18) would make milestone 1 a tautology and the goal a calculus exercise about a formula unrelated to Gaussians. The definition here is a measure of a set.
    • Allowing t = 0 would put the junk value φ(0)/0 = 0 on the right of (4). The statements require t > 0.

The two remarks printed right after Proposition 6.1 (on Λ_ρ(1/2) and on removing the factor 1 + ρ) are not part of this mission.

Contributions are welcome on all four milestones, on the case ρ = 1 of the goal (Mills' inequality), and on general lemmas: N as Pr[X ≥ x], monotonicity and positivity of N, and the law of (X, ρX + √(1 − ρ²)Y) as a bivariate normal.

Selected references

  • S. Khot, G. Kindler, E. Mossel, R. O'Donnell, Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs?, SIAM J. Comput. 37(1), 2007 (authors' version of February 7, 2007). https://doi.org/10.1137/S0097539705447372
  • E. Mossel, R. O'Donnell, K. Oleszkiewicz, Noise stability of functions with low influences: invariance and optimality, FOCS 2005; Annals of Mathematics 171, 2010. https://arxiv.org/abs/math/0503503
  • E. de Klerk, D. Pasechnik, J. Warners, Approximate graph colouring and MAX-k-CUT algorithms based on the theta function, Journal of Combinatorial Optimization 8, 2004 (Lemma 11.1).
  • W. F. Sheppard, On the application of the theory of error to cases of normal distribution and normal correlation, Phil. Trans. R. Soc. London A 192, 101–168, 1899. https://doi.org/10.1098/rsta.1899.0003
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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.
20 thms2 active usersReviewed
Discrete Geometry·Captain: marwahaha

Slope-field perturbations of the two-cylinder coveringOpen Problem

Motivation

A slope-field perturbation of a two-cylinder cover trades a reduction in projected area against the extra overlap needed to maintain coverage. The slope-field manuscript studies when the net cost becomes strictly smaller. The companion radial-sweep manuscript establishes finite triangular approximation with arbitrary tagged equal subdivisions. Both manuscripts map to the same published Lean goal, so this draft covers their shared target. The source manuscript presents the surrounding research claim.

Setting

A cylinder is a measurable finite-area planar base plus a line in its perpendicular unit direction. Ruled sets vary the segment direction over compact planar labels. Radial sweeps use p₀+ρ(a+tb)+s(e+w(t)), with 0≤ρ≤R(t), |s|≤L, and w′(t)=λ(t)(a+tb).

Formalization target

Prove the seven-part fourPaperMain conjunction: the explicit angular-area construction; C¹ hyperbolic approximation; C¹ square-zero-derivative approximation; regular-tetrahedron counterexamples with parallelogram bases and with bounded open bases; aligned radial triangular approximation; and actual-sweep projection bounds. In particular, the tetrahedron clauses require

∑i∣Bi∣<12Amin⁡(K),∑i∣Bi∣∣πui⊥K∣<12.\sum_i|B_i|<\frac12 A_{\min}(K),\qquad\sum_i\frac{|B_i|}{|\pi_{u_i^\perp}K|}<\frac12.i∑​∣Bi​∣<21​Amin​(K),i∑​∣πui⊥​​K∣∣Bi​∣​<21​.

The selected formal target is OAI.CylinderCovering.fourPaperMain.

Significance and status

The selected published goal is a joint endpoint shared by four related manuscripts, and therefore includes more than the slope-field application alone. Its finite covers retain both cost inequalities. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

A local area decrease cannot guarantee a global cover. All regularity, exact coverage and error bounds in the separate conjuncts must hold in their stated regimes.

Formalization scope

Hyperbolic and nilpotent clauses use their C¹ definitions; radial data require a nonempty parameter interval, positive segment half-length, continuous nonnegative cap and alignment derivative. All tagged equal subdivisions are covered. The radial clause requires triangular-base area to converge to weightedArea(D), while actual sweep projections have eventual cost at most weightedArea(D)+ε and the corresponding limsup bound. The separate RuledApproximation.fullMain is also retained as a related reference but is not mislabeled as one of these seven conjuncts.

Selected references

  • OpenAI, Finite triangular approximation of radial sweeps, preprint, 2026. Pinned manuscript.
  • OpenAI, Slope-field perturbations of the two-cylinder covering, 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.
30 thms2 active usersReviewed
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