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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XXVI: Individual-Risk Aggregate Claims by ConvolutionTextbook

Actuarial Mathematics XXVI: Individual-Risk Aggregate Claims by Convolution

Research provenance and new formalisation

R. J. Verrall (1989), The individual risk model: a compound distribution, Journal of the Institute of Actuaries, volume 116(1), pages 101–107, DOI https://doi.org/10.1017/S0020268100036465, develops the connection between individual and collective aggregate-risk modelling. Nelson De Pril (1989), The Aggregate Claims Distribution in the Individual Model with Arbitrary Positive Claims, ASTIN Bulletin, volume 19(1), pages 9–24, DOI https://doi.org/10.2143/AST.19.1.2014913, develops exact aggregate-distribution recursion for the individual-risk model.

The present mission is a finite, integer-lattice, independent Bernoulli-policy formalisation. It derives probability-mass support, nonnegativity and normalisation from convolution, rather than claiming that either author already supplied these exact Lean theorem types.

Individual policies, integer benefits and dependence assumptions

Policy iii pays a fixed nonnegative integer benefit bib_ibi​ with probability pip_ipi​, where 0≤pi≤10\le p_i\le10≤pi​≤1. It pays nothing otherwise. The Bernoulli policy's payment distribution, as opposed to its event distribution, is

hi(s)=(1−pi)1{s=0}+pi1{s=bi},s∈N.h_i(s)=(1-p_i)\mathbf1_{\{s=0\}}+p_i\mathbf1_{\{s=b_i\}}, \qquad s\in\mathbb N.hi​(s)=(1−pi​)1{s=0}​+pi​1{s=bi​}​,s∈N.

A zero-benefit policy has both events paying zero. Therefore its single payment coefficient at s=0s=0s=0 is 111, not 1−pi1-p_i1−pi​. This corner case is explicitly retained, rather than assuming every bib_ibi​ is strictly positive.

The total loss over n independent policies is Sn=∑i<nbiBiS_n=\sum_{i<n}b_iB_iSn​=∑i<n​bi​Bi​, with independent Bernoulli indicators BiB_iBi​. Its maximum possible loss is Bn=∑i<nbiB_n=\sum_{i<n}b_iBn​=∑i<n​bi​.

Exact convolution and portfolio recursion

For coefficient arrays f,g:N→Rf,g:\mathbb N\to\mathbb Rf,g:N→R, define their discrete convolution by

(f∗g)(s)=∑k=0sf(k)g(s−k).(f*g)(s)=\sum_{k=0}^{s}f(k)g(s-k).(f∗g)(s)=k=0∑s​f(k)g(s−k).

With no policies the payment mass is δ0(s)=1{s=0}\delta_0(s)=\mathbf1_{\{s=0\}}δ0​(s)=1{s=0}​. Each additional policy is introduced by

g0(s)=δ0(s),gn+1(s)=(gn∗hn)(s).g_0(s)=\delta_0(s),\qquad g_{n+1}(s)=\bigl(g_n*h_{n}\bigr)(s).g0​(s)=δ0​(s),gn+1​(s)=(gn​∗hn​)(s).

A bound-aware mass operator is MB(f)=∑s=0Bf(s)M_B(f)=\sum_{s=0}^{B}f(s)MB​(f)=∑s=0B​f(s). If the first distribution vanishes above B and the second above C, convolution satisfies MB+C(f∗g)=MB(f)MC(g)M_{B+C}(f*g)=M_B(f)M_C(g)MB+C​(f∗g)=MB​(f)MC​(g), even for unnormalised intermediate coefficient arrays.

The companion algebraic lemmas establish convolution identity, commutativity and associativity. A distributional lemma establishes that nonnegative component masses imply nonnegative convolution coefficients.

Fundamental theorem

Under 0≤pi≤10\le p_i\le10≤pi​≤1 for every included policy, the portfolio aggregate is a valid bounded probability mass function:

gn(s)≥0(∀s≥0),∑s=0Bngn(s)=1,gn(s)=0(s>Bn).\boxed{ g_n(s)\ge0\quad(\forall s\ge0),\qquad \sum_{s=0}^{B_n}g_n(s)=1,\qquad g_n(s)=0\quad(s>B_n). }gn​(s)≥0(∀s≥0),s=0∑Bn​​gn​(s)=1,gn​(s)=0(s>Bn​).​

These are three distinct requirements: nonnegativity, normalisation on the exact finite benefit bound and zero support above that bound. All must be proved, including empty portfolios and policies whose benefit is zero. Independence is encoded by the convolution construction, not inferred from unrelated marginal Bernoulli probabilities.

Proof structure and validation

Five new definitions introduce convolution, one-policy Bernoulli mass, bounded total mass, maximum possible claim and recursive portfolio probability mass. Fourteen supporting milestones prove convolution identities and support/mass preservation, the policy recursion, and bounded portfolio mass and nonnegativity; the fifteenth theorem is the capstone.

An independent exact-rational benchmark enumerated all binary claim/no-claim events across 1,365 distinct heterogeneous policy configurations, with zero and repeated benefits and probabilities at 0, 1/4, 1/2 and 1. Direct event enumeration agreed exactly with recursive convolution, giving nonnegative coefficients and unit total mass.

The source uses natural-valued grid claims, not continuous severities, and finite portfolios only. It does not assume any unpublished other mission's definitions exist in the Lean environment. Imported Lean definitions are local within this mission, with all imports before namespaces. Every theorem remains an open proof obligation until proved on the authoritative Prove2Me remote compiler.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XXVII: Compound Poisson Panjer RecursionTextbook

Actuarial Mathematics XXVII: Compound Poisson Panjer Recursion

Original actuarial research and the exact specialisation

Harry H. Panjer (1981), Recursive Evaluation of a Family of Compound Distributions, ASTIN Bulletin 12(1), 22–26, DOI https://doi.org/10.1017/S0515036100006796, proves a recursion for aggregate-claim distributions with suitable claim-frequency laws. The original paper treats a wider class than Poisson claim counts. Sundt and Jewell (1981), Further Results on Recursive Evaluation of Compound Distributions, ASTIN Bulletin 12(1), 27–39, DOI https://doi.org/10.1017/S0515036100006802, develops its extensions.

This mission formalises the positive-integer-severity compound Poisson case. The restriction on zero-sized claims is essential to the exact finite-count mixture used by the Lean definitions. It does not claim that a finite truncated Poisson mixture is automatically a probability distribution if zero severity has positive mass.

Count frequency and conditional aggregate severity

Let N∼Poisson⁡(λ)N\sim\operatorname{Poisson}(\lambda)N∼Poisson(λ) with λ≥0\lambda\ge0λ≥0. Its count probabilities are

pm=e−λλmm!,m=0,1,….p_m=e^{-\lambda}\frac{\lambda^m}{m!},\qquad m=0,1,\ldots.pm​=e−λm!λm​,m=0,1,….

Each claim has a positive integer severity with mass fjf_jfj​. The key support condition is f0=0f_0=0f0​=0. The usual stochastic interpretation additionally requires fj≥0f_j\ge0fj​≥0 and total severity mass one, although the algebraic Panjer theorem itself works for arbitrary real fjf_jfj​ satisfying f0=0f_0=0f0​=0.

For exactly m independent claims, f∗mf^{*m}f∗m is the m-fold discrete convolution, with f∗0=δ0f^{*0}=\delta_0f∗0=δ0​ and f∗(m+1)=f∗f∗mf^{*(m+1)}=f*f^{*m}f∗(m+1)=f∗f∗m. Each positive claim contributes at least one unit, hence

s<m⟹f∗m(s)=0.s<m\Longrightarrow f^{*m}(s)=0.s<m⟹f∗m(s)=0.

It follows that the compound Poisson coefficient at aggregate loss s can be written as an exact finite sum, despite the count distribution being unbounded:

gs=∑m=0se−λλmm!f∗m(s).g_s=\sum_{m=0}^{s}e^{-\lambda}\frac{\lambda^m}{m!}f^{*m}(s).gs​=m=0∑s​e−λm!λm​f∗m(s).

At λ=0\lambda=0λ=0, the distribution is δ0\delta_0δ0​. When f0=0f_0=0f0​=0, the zero-loss aggregate mass equals g0=e−λg_0=e^{-\lambda}g0​=e−λ.

Panjer recurrence and uniqueness

Panjer's recursion for this model is

g0=e−λ,gs=λs∑j=1sj fj gs−j(s≥1).\boxed{ g_0=e^{-\lambda},\qquad g_s=\frac{\lambda}{s}\sum_{j=1}^{s}j\,f_j\,g_{s-j} \quad(s\ge1). }g0​=e−λ,gs​=sλ​j=1∑s​jfj​gs−j​(s≥1).​

It can be derived by combining the Poisson count ratio (m+1)pm+1=λpm(m+1)p_{m+1}=\lambda p_m(m+1)pm+1​=λpm​ with the convolution-power coefficients. The zero-severity term has a factor j=0 and vanishes. Consequently the right-hand side at s depends only on the earlier aggregate coefficients g0,…,gs−1g_0,\ldots,g_{s-1}g0​,…,gs−1​. A separate theorem asserts that the initial mass and this recurrence uniquely determine the aggregate mass sequence.

The main Lean theorem is a conjunction of the no-claim initial value, the one-step recursion for every s+1s+1s+1, and uniqueness for any real sequence satisfying those identities. It is an exact theorem about coefficients, not a numerical approximation or an unsupported claim of convergence of a severity generating function.

Validation and important boundaries

Five local definitions represent severity convolution, m-claim convolution powers, Poisson frequency mass, the aggregate mixture and the Panjer coefficient update. Thirteen supporting theorems include power recursion, support, count ratio, zero rate, nonnegative coefficients, the Panjer identity and uniqueness. The fourteenth is the capstone.

The independent high-precision benchmark compared two implementations: (i) direct Poisson-weighted convolution powers and (ii) the Panjer recurrence. They agreed to better than 10−6010^{-60}10−60 across 264 rate, severity and aggregate-size combinations using 70-digit decimal arithmetic, including zero frequency, fixed unit severity, two-point severity and a three-point severity with a gap.

The positive integer severity condition f0=0f_0=0f0​=0 cannot simply be dropped: when zero-valued claims occur, m>sm>sm>s can still contribute to aggregate loss s, and the true Poisson initial value becomes exp⁡[−λ(1−f0)]\exp[-\lambda(1-f_0)]exp[−λ(1−f0​)]. That more general form, and arbitrary Panjer (a,b,0) counting laws, are explicitly out of scope.

No unpublished definitions are imported from Actuarial XXVI. The problem is mathematically linked but formally self-contained while XXVI is still a Draft. The theorem targets remain unproved until valid Lean submissions are accepted by Prove2Me.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XXV: Mean-Variance Reinsurance and Optimal Quota ShareTextbook

Actuarial Mathematics XXV: Mean-Variance Reinsurance and Optimal Quota Share

Primary research and scope

Marek Kaluszka (2001), Optimal reinsurance under mean-variance premium principles, Insurance: Mathematics and Economics 28(1), 61–67, https://doi.org/10.1016/S0167-6687(00)00066-4, examines optimal retention when the reinsurance premium depends on claim mean and variance. Manuel Guerra and Maria de Lourdes Centeno (2010), Optimal Reinsurance for Variance Related Premium Calculation Principles, ASTIN Bulletin 40(1), 97–121, https://doi.org/10.2143/AST.40.1.2049220, studies the effect of variance-based loading on reinsurance decisions.

This mission isolates a clean Bernoulli claim and continuous quota-share specialisation, with a closed-form optimum and a finite-menu alternative. It does not assert the general optimal-retention functional results or the VaR/CVaR optimisations in the cited papers.

Insurer and reinsurer cashflow model

Let X=b BX=b\,BX=bB, where BBB is a Bernoulli indicator with Pr⁡(B=1)=q\Pr(B=1)=qPr(B=1)=q. Its claim amount is b≥0b\ge0b≥0 and the claim probability satisfies 0≤q≤10\le q\le10≤q≤1. A quota share r∈[0,1]r\in[0,1]r∈[0,1] is the insurer's retained proportion of each realised claim:

Rr(X)=rX,Cr(X)=(1−r)X,Rr(X)+Cr(X)=X.R_r(X)=rX,\qquad C_r(X)=(1-r)X,\qquad R_r(X)+C_r(X)=X.Rr​(X)=rX,Cr​(X)=(1−r)X,Rr​(X)+Cr​(X)=X.

The reinsurer receives a fixed premium at policy inception that is an expected-value premium plus a loading on ceded variance. Using parameters λ≥0\lambda\ge0λ≥0 and α≥0\alpha\ge0α≥0, where each variance coefficient has reciprocal currency units, define

Πr=E[Cr(X)]+λVar⁡(Cr(X))=q(1−r)b+λq(1−q)(1−r)2b2.\Pi_r=\mathbb E[C_r(X)]+\lambda\operatorname{Var}(C_r(X)) =q(1-r)b+\lambda q(1-q)(1-r)^2b^2.Πr​=E[Cr​(X)]+λVar(Cr​(X))=q(1−r)b+λq(1−q)(1−r)2b2.

The insurer's objective adds expected retained claims, the reinsurance premium and a variance-based risk-capital charge on retained loss:

J(r)=E[Rr(X)]+Πr+αVar⁡(Rr(X)).J(r)=\mathbb E[R_r(X)]+\Pi_r+\alpha\operatorname{Var}(R_r(X)).J(r)=E[Rr​(X)]+Πr​+αVar(Rr​(X)).

For any real rrr, the relevant expectation and variance formulas yield

J(r)=qb+q(1−q)b2[λ(1−r)2+αr2].J(r)=qb+q(1-q)b^2\bigl[\lambda(1-r)^2+\alpha r^2\bigr].J(r)=qb+q(1−q)b2[λ(1−r)2+αr2].

The premium Πr\Pi_rΠr​ is deterministic once the contract and model are fixed, so it does not contribute additional random loss variance. A quota-share arrangement may change both the expected ceded premium and the variance of retained claims; both effects are included.

Continuous optimal quota-share retention

Assume λ+α>0\lambda+\alpha>0λ+α>0 in addition to nonnegative coefficients. Completing the square gives

λ(1−r)2+αr2=λαλ+α+(λ+α)(r−λλ+α)2.\lambda(1-r)^2+\alpha r^2 =\frac{\lambda\alpha}{\lambda+\alpha} +(\lambda+\alpha)\left(r-\frac{\lambda}{\lambda+\alpha}\right)^2.λ(1−r)2+αr2=λ+αλα​+(λ+α)(r−λ+αλ​)2.

It follows that the optimal insurer retention, not the ceded proportion, is

r∗=λλ+α∈[0,1],J(r∗)≤J(r)  for all r∈R.\boxed{r^*=\frac{\lambda}{\lambda+\alpha}\in[0,1],\qquad J(r^*)\le J(r)\;\text{for all }r\in\mathbb R.}r∗=λ+αλ​∈[0,1],J(r∗)≤J(r)for all r∈R.​

The solution can be at a boundary. If λ=0<α\lambda=0<\alphaλ=0<α the insurer fully cedes the claim, r∗=0r^*=0r∗=0. If α=0<λ\alpha=0<\lambdaα=0<λ, it retains everything, r∗=1r^*=1r∗=1. If both coefficients vanish, all retentions have the same objective and the displayed ratio is undefined: this case is explicitly excluded. With 0<q<10<q<10<q<1, nonzero claim amount and positive total coefficient, r∗r^*r∗ is unique. For zero variance, for example q=0q=0q=0 or q=1q=1q=1, every retention has the same variance component, so uniqueness does not follow and is not asserted.

A real insurer may instead face a finite menu AAA of quoted retentions rar_ara​. Since AAA is nonempty and finite, a cost-minimising member a∗a^*a∗ always exists, but there is no promise that ra∗=r∗r_{a^*}=r^*ra∗​=r∗.

Structure and intended Lean proof

The five definitions represent retained claim, ceded claim, variance premium, insurer capital objective and closed-form continuous retention. Twelve intermediate theorem obligations establish cashflow conservation, claim nonnegativity, full retention and full cession boundaries, objective expansion, admissibility of the candidate, quadratic square completion, global optimality, strict uniqueness when appropriate and finite-menu attainment. The capstone combines 0≤r∗≤10\le r^*\le10≤r∗≤1 with J(r∗)≤J(r)J(r^*)\le J(r)J(r∗)≤J(r) for every real alternative.

The proof uses elementary real algebra and finite-set minimum selection. It requires neither local stochastic simulation nor a limit-of-policy-years theorem. The Bernoulli setup is deliberate, making the mean/variance premium principle analytically exact and testable before attempting general loss distributions.

Model boundaries

Annual claim occurrence is a single Bernoulli event. Multiple correlated claims, expense loadings, default, credit risk, taxes, multi-period dynamic adjustment and Solvency II regulatory capital are not modelled. The capital coefficient is a chosen deterministic variance penalty rather than a regulatory capital formula. An optimal r∗r^*r∗ in this model should not be confused with an optimal excess-of-loss attachment point or with the entropic risk-sensitive optimum in Missions XXI–XXII.

All displayed theorem targets are unproved obligations until the authoritative Prove2Me compiler accepts a valid Lean proof. The owner Draft is for captain confirmation and moderator review, not an accepted theorem library.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XXIV: Multiple-Decrement Mortality Innovation VarianceTextbook

Actuarial Mathematics XXIV: Multiple-Decrement Mortality Innovation Variance

Research and distinction from the single-decrement formula

Shiu and Xiong (2021), An elementary derivation of Hattendorff's theorem, European Actuarial Journal 11, 319–323, https://doi.org/10.1007/s13385-020-00256-9, derives the fully discrete mortality variance formula using reserve differences and summation by parts. The present mission develops the multiple-decrement extension on a countable lifetime space, keeping the covariance of different termination causes in the same policy year. This is a new derived formalisation rather than a claim that Shiu and Xiong printed these exact competing-risk theorems.

The earlier Actuarial XIV mission considers multiple-decrement valuation and premium recursion, while XVI investigates yearly mortality innovation orthogonality. Neither automatically supplies the countable competing-cause variance theorem, particularly when the net amount at risk is different for each decrement cause.

Model, parameters and timing

The termination year is a natural number K∈NK\in\mathbb NK∈N. Its cause DDD belongs to a finite type CCC. For every policy year ttt and cause ccc, write wt,c=Pr⁡(K=t,D=c)w_{t,c}=\Pr(K=t,D=c)wt,c​=Pr(K=t,D=c). Causes are mutually exclusive: exactly one cause is realised on termination.

Require wt,c≥0w_{t,c}\ge0wt,c​≥0, ∑t=0∞∑c∈Cwt,c=1\sum_{t=0}^\infty\sum_{c\in C}w_{t,c}=1∑t=0∞​∑c∈C​wt,c​=1 and a strictly positive in-force mass at every policy year:

Dt=∑c∈Cwt,c,St=∑k≥tDk>0,qt,c=wt,cSt.D_t=\sum_{c\in C}w_{t,c},\qquad S_t=\sum_{k\ge t}D_k>0,\qquad q_{t,c}=\frac{w_{t,c}}{S_t}.Dt​=c∈C∑​wt,c​,St​=k≥t∑​Dk​>0,qt,c​=St​wt,c​​.

The cause probabilities do not have to be equal. Their sum is at most one because survival through the year remains possible. The realised cause has no independent probability after termination: this is one joint time-and-cause categorical distribution, not a collection of independent single-decrement lives.

Cause-specific year surprises

For a realised scenario (k,d)(k,d)(k,d), define the year ttt, cause ccc surprise:

It,c(k,d)=1{k=t, d=c}−qt,c1{k≥t}.I_{t,c}(k,d)=\mathbf1_{\{k=t,\ d=c\}}- q_{t,c}\mathbf1_{\{k\ge t\}}.It,c​(k,d)=1{k=t, d=c}​−qt,c​1{k≥t}​.

All these innovations vanish when k<tk<tk<t. At termination (t,c)(t,c)(t,c), the cause-c innovation is 1−qt,c1-q_{t,c}1−qt,c​. The innovation of any other cause d≠cd\ne cd=c in the same year equals −qt,d-q_{t,d}−qt,d​. Therefore treating the cause indicators as independent would be wrong.

Let ρt,c\rho_{t,c}ρt,c​ be the discounted cause-specific net amount at risk payable at the end of year t+1t+1t+1. With cause-dependent death benefits bt+1,cb_{t+1,c}bt+1,c​ and an appropriate prospective reserve Vt+1V_{t+1}Vt+1​, a typical amount is ρt,c=vt+1(bt+1,c−Vt+1)\rho_{t,c}=v^{t+1}(b_{t+1,c}-V_{t+1})ρt,c​=vt+1(bt+1,c​−Vt+1​). The finite-horizon centred reserve surprise is

Zn(k,d)=∑t<n∑c∈Cρt,cIt,c(k,d).Z_n(k,d)=\sum_{t<n}\sum_{c\in C}\rho_{t,c}I_{t,c}(k,d).Zn​(k,d)=t<n∑​c∈C∑​ρt,c​It,c​(k,d).

The mission defines this random variable directly. A cashflow-specific reserve recursion would be a further theorem, not a hidden hypothesis.

Correct annual variance including cause covariance

Cause-specific innovations from different years are orthogonal. At the same year, however, distinct causes have negative weighted cross moments:

E[It,cIt,d]=−wt,cwt,dSt(c≠d).\mathbb E[I_{t,c}I_{t,d}] =-\frac{w_{t,c}w_{t,d}}{S_t}\qquad(c\ne d).E[It,c​It,d​]=−St​wt,c​wt,d​​(c=d).

The full annual Hattendorff contribution is therefore

At=∑c∈Cwt,cρt,c2−(∑c∈Cwt,cρt,c)2St.A_t=\sum_{c\in C}w_{t,c}\rho_{t,c}^2- \frac{\bigl(\sum_{c\in C}w_{t,c}\rho_{t,c}\bigr)^2}{S_t}.At​=c∈C∑​wt,c​ρt,c2​−St​(∑c∈C​wt,c​ρt,c​)2​.

This subtracts the square of the aggregate weighted amount at risk, rather than subtracting separate squares for individual causes. It is the unconditional variance contribution from one year's categorical decrement shock. The assumptions wt,c≥0w_{t,c}\ge0wt,c​≥0, St>0S_t>0St​>0 and Dt≤StD_t\le S_tDt​≤St​ imply At≥0A_t\ge0At​≥0 by weighted Cauchy–Schwarz.

The capstone asserts

E[Zn2]=∑t=0n−1At.\boxed{\mathbb E[Z_n^2]=\sum_{t=0}^{n-1}A_t.}E[Zn2​]=t=0∑n−1​At​.​

It works with an arbitrary finite cause set and a countably infinite possible termination-year set. It does not yet claim an infinite-horizon limit, which can be developed by applying XXIII-style summability to these AtA_tAt​.

Proof programme and boundaries

There are five new definitions, ten supporting milestone theorems and one capstone. The supporting obligations establish nonnegative year masses, exact observed/other-cause innovation values, zero horizon, the successor-year identity, nonnegative annual variance, scaling of risk exposure, and the negative cross-cause moment before proving the full year-by-year allocation.

The proof must distinguish the finite inner cause sum from the infinite outer lifetime sum; nonnegative mass and summability are explicitly required for countable expectation manipulations. The formal model allows zero annual incidence for a particular cause, but demands positive aggregate survival tails so the conditional fractions are defined. All proof obligations use the pinned Mathlib version and require authoritative Prove2Me remote compilation and accepted Lean proofs.

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Quantum Error CorrectionQuantum GravityQuantum Information·Captain: Alien60

Almheiri–Dong–Harlow 2015: Bulk Locality and Quantum Error Correction in AdS/CFTResearch Paper

Motivation

The AdS/CFT correspondence relates a theory of quantum gravity in anti-de Sitter space (the bulk) to a quantum field theory without gravity on its boundary (the CFT). A central question is how a local field operator ϕ(x)\phi(x)ϕ(x) deep in the bulk is represented by boundary operators. Almheiri, Dong and Harlow (JHEP 04 (2015) 163) pointed out a puzzle.

  • The bulk operator can be reconstructed on several different boundary regions. For example, it can be reconstructed on A∪BA\cup BA∪B, on B∪CB\cup CB∪C or on A∪CA\cup CA∪C, but not on any single one of them.
  • These reconstructions cannot all be the same CFT operator: an operator commuting with all local operators on a time slice must be trivial.

Their resolution is that the bulk effective theory is a quantum error-correcting code. Bulk operators are logical operators acting on a code subspace of the CFT Hilbert space. Different boundary representations agree only on that subspace, as one logical operator of an erasure-correcting code can be implemented on different subsets of qubits.

The mathematical backbone of that resolution is a finite-dimensional criterion for when a logical operator can be implemented on a given subsystem. This mission formalizes it (Appendix B of the paper), with the examples and corollaries of Section 3.

Timeline.

  • 1996–1997: Schumacher and Nielsen characterize correctability by vanishing correlations with a reference system, condition (3.14) (arXiv:quant-ph/9604022). Grassl, Beth and Pellizzari give the matrix-element form (3.19) (arXiv:quant-ph/9610042).
  • 1999: Cleve, Gottesman and Lo introduce the three-qutrit code as a quantum secret-sharing scheme (arXiv:quant-ph/9901025).
  • 2006: Ryu and Takayanagi propose the holographic entanglement-entropy formula (arXiv:hep-th/0603001).
  • 2007: Bény, Kempf and Kribs develop operator-algebra quantum error correction (arXiv:quant-ph/0608071, arXiv:0705.1574), of which the theorem here is a special case.
  • 2014–2015: Almheiri, Dong and Harlow recast bulk reconstruction as quantum error correction; Pastawski, Yoshida, Harlow and Preskill build holographic tensor-network codes (arXiv:1503.06237).
  • 2016: Dong, Harlow and Wall establish reconstruction in the entanglement wedge (arXiv:1601.05416). Harlow derives the Ryu–Takayanagi formula from operator-algebra error correction (arXiv:1607.03901).

Setting

The physical Hilbert space is a tensor product H=HE⊗HEˉ\mathcal H = \mathcal H_E\otimes\mathcal H_{\bar E}H=HE​⊗HEˉ​ of finite-dimensional spaces. EEE is the part that may be erased (lost), and Eˉ\bar EEˉ is the part that remains. A code subspace is a subspace HC⊆H\mathcal H_{\mathcal C}\subseteq\mathcal HHC​⊆H.

An operator OOO acts within the code subspace if both OOO and O†O^\daggerO† map HC\mathcal H_{\mathcal C}HC​ into itself. Such an operator has a representation on Eˉ\bar EEˉ if there is an operator OEˉO_{\bar E}OEˉ​ acting only on Eˉ\bar EEˉ, that is of the form 1E⊗Y\mathbb 1_E\otimes Y1E​⊗Y, with

OEˉ∣ψ~⟩=O∣ψ~⟩,OEˉ†∣ψ~⟩=O†∣ψ~⟩for all ∣ψ~⟩∈HC.O_{\bar E}|\tilde\psi\rangle = O|\tilde\psi\rangle,\qquad O_{\bar E}^\dagger|\tilde\psi\rangle = O^\dagger|\tilde\psi\rangle\qquad\text{for all }|\tilde\psi\rangle\in\mathcal H_{\mathcal C}.OEˉ​∣ψ~​⟩=O∣ψ~​⟩,OEˉ†​∣ψ~​⟩=O†∣ψ~​⟩for all ∣ψ~​⟩∈HC​.

Representations on EEE are defined in the same way, with operators X⊗1EˉX\otimes\mathbb 1_{\bar E}X⊗1Eˉ​.

The three-qutrit code (Section 3.1) encodes one qutrit into three via

∣ı~⟩=13∑a∈Z3∣a, a+i, a+2i⟩,|\tilde\imath\rangle = \tfrac{1}{\sqrt3}\textstyle\sum_{a\in\mathbb Z_3}|a,\ a+i,\ a+2i\rangle,∣~⟩=3​1​∑a∈Z3​​∣a, a+i, a+2i⟩,

that is, ∣0~⟩=(∣000⟩+∣111⟩+∣222⟩)/3|\tilde 0\rangle = (|000\rangle+|111\rangle+|222\rangle)/\sqrt3∣0~⟩=(∣000⟩+∣111⟩+∣222⟩)/3​ and so on (Eq. (3.3)).

Formalization targets

Goal: the basic theorem of operator-algebra quantum error correction (Section 3.5, proof in Appendix B)

For an operator OOO acting within HC\mathcal H_{\mathcal C}HC​,

O has a representation on Eˉ  ⟺  ⟨ψ~′∣ [O, XE⊗1Eˉ] ∣ψ~⟩=0  for all XE on E and all ∣ψ~⟩,∣ψ~′⟩∈HC.O\ \text{has a representation on }\bar E\iff \langle\tilde\psi'|\,[O,\,X_E\otimes\mathbb 1_{\bar E}]\,|\tilde\psi\rangle = 0\ \ \text{for all } X_E \text{ on } E \text{ and all } |\tilde\psi\rangle,|\tilde\psi'\rangle\in\mathcal H_{\mathcal C}.O has a representation on Eˉ⟺⟨ψ~​′∣[O,XE​⊗1Eˉ​]∣ψ~​⟩=0  for all XE​ on E and all ∣ψ~​⟩,∣ψ~​′⟩∈HC​.

Milestones (in source order)

  1. Section 3.1 (after Eq. (3.3)): for every encoded three-qutrit state, the reduced density matrix of each single qutrit is 131\tfrac13\mathbb 131​1.
  2. Eqs. (3.4)–(3.6): the permutation U12U_{12}U12​ of Eq. (3.6) is unitary, and (U12⊗I3)∣ı~⟩=∣i⟩⊗13(∣00⟩+∣11⟩+∣22⟩)(U_{12}\otimes I_3)|\tilde\imath\rangle = |i\rangle\otimes\tfrac1{\sqrt3}(|00\rangle+|11\rangle+|22\rangle)(U12​⊗I3​)∣~⟩=∣i⟩⊗3​1​(∣00⟩+∣11⟩+∣22⟩).
  3. Eqs. (3.9)–(3.10): for every single-qutrit operator OOO, the operator O12=U12†(O⊗1)U12O_{12} = U_{12}^\dagger (O\otimes\mathbb 1) U_{12}O12​=U12†​(O⊗1)U12​, with OOO acting on the first qutrit, satisfies O12∣ı~⟩=∑jOji∣ȷ~⟩O_{12}|\tilde\imath\rangle = \sum_j O_{ji}|\tilde\jmath\rangleO12​∣~⟩=∑j​Oji​∣~​⟩.
  4. Section 3.2, Eqs. (3.19) ⟺ (3.21): the projection of every XEX_EXE​ onto the code subspace is proportional to the identity iff every operator acting within the code subspace has a representation on Eˉ\bar EEˉ. The source states, citing the literature, that (3.19) is equivalent to correctability of the erasure of EEE; that equivalence is not formalized.
  5. Section 3.5, two-qubit example: on the code spanned by (∣00⟩+∣11⟩)/2(|00\rangle+|11\rangle)/\sqrt2(∣00⟩+∣11⟩)/2​ and (∣01⟩+∣10⟩)/2(|01\rangle+|10\rangle)/\sqrt2(∣01⟩+∣10⟩)/2​, the logical XXX is realized by the bit flip of either qubit. No operator on the first qubit alone reproduces the logical ZZZ on the code, and every logical operator realizable on the first qubit acts on the code as a1+bXˉa\mathbb 1 + b\bar Xa1+bXˉ: the code corrects only the subalgebra generated by 1\mathbb 11 and Xˉ\bar XXˉ.
  6. Section 3.5, algebraic no-cloning: if O1O_1O1​ has a representation on Eˉ\bar EEˉ and O2O_2O2​ has a representation on EEE, then O1O_1O1​ and O2O_2O2​ commute on the code subspace. Consequently, the elements of any family of logical operators that is represented both on EEE and on Eˉ\bar EEˉ commute pairwise on the code subspace, so a non-abelian algebra cannot be represented on both.

Significance

The result. The goal theorem characterizes, by a checkable commutation condition, which logical operators survive the loss of EEE; milestone 4 is its specialization to full erasure correction. Milestone 6 explains why a non-commuting algebra of bulk operators cannot be represented on two complementary boundary regions at once, so reconstructions of ϕ(x)\phi(x)ϕ(x) on different regions are distinct operators that agree only on the code subspace. The three-qutrit code models this: every logical operator is realized on any two qutrits, and no single qutrit carries information.

Formalizing it. All statements are proved in the source, or cited there from standard references, and are finite-dimensional. This mission produces machine-checked versions and a reusable vocabulary of code subspaces, logical operators and subsystem representations. That vocabulary is the starting point for formalizing the later results it underlies, in particular the subsystem and operator-algebra theorems of Harlow's derivation of the Ryu–Takayanagi formula (arXiv:1607.03901).

Status honesty. The mathematics is unconditional finite-dimensional linear algebra. The application to AdS/CFT rests on the conjectured duality and on bulk effective field theory, and is context only; none of it enters the hypotheses. The appendix proof is the authors' own, and the theorem is a special case of the results of Bény, Kempf and Kribs. The equivalence of (3.19) with correctability of the erasure (the existence of a recovery unitary, Eqs. (3.14)–(3.18)) is cited in the source from Schumacher–Nielsen and Grassl–Beth–Pellizzari, and is not part of this mission. No machine-checked proof of any of these statements is known. Neither Mathlib nor Physlib (including its quantum-information library) formalizes code subspaces, erasure correction or operator-algebra quantum error correction.

Difficulty

The forward direction of the goal is a direct computation. The converse is an existence statement: an operator OEˉ=1E⊗YO_{\bar E}=\mathbb 1_E\otimes YOEˉ​=1E​⊗Y has to be produced from a hypothesis that constrains only the matrix elements of OOO between code states. That hypothesis says nothing about how OOO acts off the code subspace, and OOO generally acts nontrivially on EEE. So no candidate for YYY can be read off from OOO itself.

Milestone 4 has the same character in both directions. One direction must produce a representation on Eˉ\bar EEˉ for every operator acting within the code subspace, starting from the scalar condition (3.19), which concerns operators on EEE alone. The other direction is a non-existence claim about operators on EEE, to be derived from a property quantified over all logical operators.

The explicit-code milestones are finite but involve the irrational normalization 1/31/\sqrt31/3​ and a 272727-dimensional space.

Formalization scope

  • Representation. Vectors on HE⊗HEˉ\mathcal H_E\otimes\mathcal H_{\bar E}HE​⊗HEˉ​ are functions on e×eˉe\times\bar ee×eˉ for finite types e,eˉe,\bar ee,eˉ, with EEE first. Operators are complex matrices, tensor products are Mathlib's Kronecker product ⊗ₖ, O†O^\daggerO† is the conjugate transpose, and ⟨w∣u⟩\langle w|u\rangle⟨w∣u⟩ is star w ⬝ᵥ u.
  • Code subspace. The code subspace is an arbitrary complex subspace (Submodule ℂ). It is described without a basis: "⟨ı~∣⋯∣ȷ~⟩=0\langle\tilde\imath|\cdots|\tilde\jmath\rangle = 0⟨~∣⋯∣~​⟩=0 for all i,ji,ji,j" is stated for all pairs of code vectors, which is equivalent by sesquilinearity.
  • Proportionality. Eq. (3.19), ⟨ı~∣XE∣ȷ~⟩=δijC(X)\langle\tilde\imath|X_E|\tilde\jmath\rangle = \delta_{ij}C(X)⟨~∣XE​∣~​⟩=δij​C(X), is stated basis-free as ⟨w∣XEv⟩=c ⟨w∣v⟩\langle w|X_E v\rangle = c\,\langle w|v\rangle⟨w∣XE​v⟩=c⟨w∣v⟩ for one constant ccc and all code vectors v,wv,wv,w.
  • Three-qutrit vectors. These are indexed by ((q1,q2),q3)((q_1,q_2),q_3)((q1​,q2​),q3​). U12U_{12}U12​ is the permutation matrix of the table in Eq. (3.6), and the single-qutrit reduced states are partial traces over the other two qutrits.
  • Not trivial. The goal quantifies over every code subspace and every operator acting within it. The zero subspace makes both sides true and is harmless. The examples are fixed concrete codes.
  • Not formalized. Cited but not proved in the source: (3.14) with the recovery unitary (3.16)–(3.18), and the bound (3.25). Heuristic: the count (3.22) and the Page-theorem argument after it. Definitions only: quantum secret sharing (Section 3.3), (3.23) and (3.24). Immediate or by symmetry: (3.20), recovery from qutrits 2,3 or 1,3, and the ∗*∗-subalgebra remark after the theorem. Out of scope: Sections 4–5 (the AdS/CFT model, backreaction).
  • Infrastructure. A complete development needs lemmas on Kronecker products acting on vectors ((A ⊗ₖ B) *ᵥ v), conjugate transposes of Kronecker products, orthogonal projection onto a Submodule, and partial traces. These are reusable; stand-alone contributions are welcome.

Selected references

  • A. Almheiri, X. Dong, D. Harlow, Bulk locality and quantum error correction in AdS/CFT, JHEP 04 (2015) 163. arXiv:1411.7041
  • C. Bény, A. Kempf, D. W. Kribs, Generalization of quantum error correction via the Heisenberg picture, Phys. Rev. Lett. 98, 100502 (2007). arXiv:quant-ph/0608071
  • C. Bény, A. Kempf, D. W. Kribs, Quantum error correction of observables, Phys. Rev. A 76, 042303 (2007). arXiv:0705.1574
  • B. Schumacher, M. A. Nielsen, Quantum data processing and error correction, Phys. Rev. A 54, 2629 (1996). arXiv:quant-ph/9604022
  • M. Grassl, T. Beth, T. Pellizzari, Codes for the quantum erasure channel, Phys. Rev. A 56, 33 (1997). arXiv:quant-ph/9610042
  • R. Cleve, D. Gottesman, H.-K. Lo, How to share a quantum secret, Phys. Rev. Lett. 83, 648 (1999). arXiv:quant-ph/9901025
  • S. Ryu, T. Takayanagi, Holographic derivation of entanglement entropy from AdS/CFT, Phys. Rev. Lett. 96, 181602 (2006). arXiv:hep-th/0603001
  • F. Pastawski, B. Yoshida, D. Harlow, J. Preskill, Holographic quantum error-correcting codes: toy models for the bulk/boundary correspondence, JHEP 06 (2015) 149. arXiv:1503.06237
  • X. Dong, D. Harlow, A. C. Wall, Reconstruction of bulk operators within the entanglement wedge in gauge-gravity duality, Phys. Rev. Lett. 117, 021601 (2016). arXiv:1601.05416
  • D. Harlow, The Ryu–Takayanagi formula from quantum error correction, Commun. Math. Phys. 354, 865 (2017). arXiv:1607.03901
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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XXII: Finite-State Entropic Bellman ControlTextbook

Fully Discrete Entropic Bellman Control with Finite Insurance States and Retention Actions

Insurance motivation and valuation horizon

An insurer choosing a retention or other reinsurance action in one year may affect both the immediate net claim cost and the distribution of liabilities in the following year. When the insurer values uncertainty using an exponential risk measure, the relevant policy objective applies the same conditional risk valuation recursively across policy years. A finite-horizon state-and-action model makes the timing, transition probabilities and policy optimality statement mathematically explicit.

This mission studies a finite-state, finite-action, discrete-time cost minimisation problem. Actions may represent a menu of excess-of-loss retention levels, but the formal statements allow any finite action menu and any state-dependent insurer cost schedule. It extends the cost-control ideas in prior actuarial missions into an explicitly risk-sensitive dynamic model. The result is a specialisation of finite-horizon recursive risk-sensitive Markov decision theory, with its own finite real-valued hypotheses and theorem proof obligations.

Timing, transition probabilities and discounting

Let SSS be the finite collection of financial, underwriting or liability states and AAA a finite nonempty set of insurance actions. At the beginning of a policy year the insurer observes the current state s∈Ss\in Ss∈S and selects an action a∈Aa\in Aa∈A. At the end of that year, the state becomes t∈St\in St∈S with conditional transition probability P(s,a,t)P(s,a,t)P(s,a,t).

We require, for each current state and action,

P(s,a,t)≥0for all t,∑t∈SP(s,a,t)=1.P(s,a,t)\ge0\quad\text{for all }t, \qquad \sum_{t\in S}P(s,a,t)=1.P(s,a,t)≥0for all t,t∈S∑​P(s,a,t)=1.

An individual destination is allowed to have probability zero. The annual real-valued cost c(s,a,t)c(s,a,t)c(s,a,t) includes the insurer's net premium, claim and treaty cashflows for the covered year, with its sign convention chosen so that larger positive values mean higher losses. A deterministic terminal amount h(s)h(s)h(s) values residual liabilities when the chosen finite horizon ends. With consistent payment-date conventions, let β≥0\beta\ge0β≥0 be the factor applied to the next year's continuation cost and γ>0\gamma>0γ>0 the entropic risk-aversion parameter for costs.

The real-valued stage costs are finite by construction. Hence, because the transition row is a genuine probability law, the exponential moment defined below is strictly positive.

Conditional entropic valuation of one year

For any future state-value function F:S→RF:S\to\mathbb RF:S→R, define

Mγ,β(s,a;F)=∑t∈SP(s,a,t)exp⁡ ⁣(γ[c(s,a,t)+βF(t)])M_{\gamma,\beta}(s,a;F) =\sum_{t\in S}P(s,a,t) \exp\!\left(\gamma\bigl[c(s,a,t)+\beta F(t)\bigr]\right)Mγ,β​(s,a;F)=t∈S∑​P(s,a,t)exp(γ[c(s,a,t)+βF(t)])

and the one-year risk-sensitive insurer cost

Qγ,β(s,a;F)=1γlog⁡Mγ,β(s,a;F).\boxed{ Q_{\gamma,\beta}(s,a;F) =\frac{1}{\gamma}\log M_{\gamma,\beta}(s,a;F). }Qγ,β​(s,a;F)=γ1​logMγ,β​(s,a;F).​

The cost and continuation value are included in one conditional exponential moment. The former is paid or valued within the current period, and the latter carries the next-year discount factor. The same chosen action changes both the costs and the transition row.

If every destination has the identical current-period cost ccc and continuation uuu, then probability normalisation implies Qγ,β=c+βuQ_{\gamma,\beta}=c+\beta uQγ,β​=c+βu. If every annual cost is increased by a fixed kkk, the stage value increases by kkk under the unit-mass probability row. With nonnegative transition probabilities, γ>0\gamma>0γ>0 and β≥0\beta\ge0β≥0, increasing either annual costs or future costs cannot decrease the entropic stage value.

The discount factor must remain inside the exponential

For an annual cost c(s,a,t)=d(s,a)c(s,a,t)=d(s,a)c(s,a,t)=d(s,a) independent of the next state, the expression simplifies to

Qγ,β(s,a;F)=d(s,a)+1γlog⁡(∑t∈SP(s,a,t)eγβF(t)).Q_{\gamma,\beta}(s,a;F) =d(s,a)+\frac1\gamma \log\left(\sum_{t\in S}P(s,a,t) e^{\gamma\beta F(t)}\right).Qγ,β​(s,a;F)=d(s,a)+γ1​log(t∈S∑​P(s,a,t)eγβF(t)).

Writing ρη(F)=η−1log⁡∑tP(s,a,t)eηF(t)\rho_\eta(F)=\eta^{-1}\log\sum_tP(s,a,t)e^{\eta F(t)}ρη​(F)=η−1log∑t​P(s,a,t)eηF(t), the continuation term for β>0\beta>0β>0 is βργβ(F)\beta\rho_{\gamma\beta}(F)βργβ​(F). In general it differs from βργ(F)\beta\rho_\gamma(F)βργ​(F). Entropic risk valuation is cash-additive and monotone under the stated conditions, but it is not generally homogeneous in the random cost. For β=0\beta=0β=0, continuation costs make no contribution and no division by γβ\gamma\betaγβ is performed.

This matters in actuarial applications: transplanting an expectation-based Bellman formula and simply replacing each conditional expectation with a fixed-parameter entropic premium would alter the intended discounted model.

Remaining-horizon policy and Bellman recursions

Let n∈Nn\in\mathbb Nn∈N denote the number of policy years remaining. A deterministic nonstationary Markov policy π:N×S→A\pi:\mathbb N\times S\to Aπ:N×S→A selects action π(k,s)\pi(k,s)π(k,s) when k+1k+1k+1 years remain and the current state is sss.

Its recursively valued insurer cost is

J0π(s)=h(s),Jk+1π(s)=Qγ,β ⁣(s,π(k,s);Jkπ).J^\pi_0(s)=h(s), \qquad J^\pi_{k+1}(s) =Q_{\gamma,\beta}\!\left(s,\pi(k,s);J^\pi_k\right).J0π​(s)=h(s),Jk+1π​(s)=Qγ,β​(s,π(k,s);Jkπ​).

Define the finite-action entropic Bellman minimum by TF(s)=min⁡a∈AQγ,β(s,a;F)TF(s)=\min_{a\in A}Q_{\gamma,\beta}(s,a;F)TF(s)=mina∈A​Qγ,β​(s,a;F). Its finite-horizon optimum satisfies

V0(s)=h(s),Vk+1(s)=min⁡a∈AQγ,β(s,a;Vk).V_0(s)=h(s), \qquad V_{k+1}(s) =\boxed{\min_{a\in A}Q_{\gamma,\beta}(s,a;V_k)}.V0​(s)=h(s),Vk+1​(s)=a∈Amin​Qγ,β​(s,a;Vk​)​.

At horizon zero the terminal amount is the entire valuation. At each successor horizon, the minimum is attained because the action set is finite and nonempty. Positive risk aversion, nonnegative discounting and a stochastic transition row make the entropic stage map monotone in its continuation argument. Those properties support induction from the terminal year backwards.

Proposed fundamental theorem

For the finite model above, the capstone combines domination of every deterministic nonstationary Markov policy with existence of an attaining Markov policy:

Vn(s)≤Jnπ(s)for every policy π and state s,∃ π∗Jnπ∗(s)=Vn(s)for every state s.\boxed{ \begin{aligned} &V_n(s)\le J^\pi_n(s) &&\text{for every policy }\pi\text{ and state }s,\\ &\exists\,\pi^*\quad J^{\pi^*}_n(s)=V_n(s) &&\text{for every state }s. \end{aligned} }​Vn​(s)≤Jnπ​(s)∃π∗Jnπ∗​(s)=Vn​(s)​​for every policy π and state s,for every state s.​​

The second line asserts a single policy that works simultaneously for all starting states. Its state- and remaining-horizon-dependent actions may be obtained by selecting a minimiser at each finite Bellman step.

The formal graph contains definitions for the transition exponential moment, entropic stage valuation, finite-action minimum, fixed-policy value and Bellman value. The supporting theorem targets establish strict positivity, deterministic-value reduction, monotonicity, cash additivity, minimum comparison and attainment, the base and successor horizon identities, policy cost domination and an attaining policy. The capstone joins the latter optimality statements.

Mathematical scope and boundary cases

All probability distributions here have finite support in a finite state space, and the horizon is finite. Stochastic rows are required only where a conditional cost interpretation or positivity is used. Zero transition probabilities for particular destinations cause no division-by-zero problem. A zero-horizon value is exactly its terminal cost; β=0\beta=0β=0 removes future exposure from each one-step valuation. The type-level definition permits an empty state type, for which assertions at each starting state are vacuous, while the action type remains nonempty.

The positive-risk-aversion assumption excludes γ=0\gamma=0γ=0. Any analytical expected-value limit as γ→0\gamma\to0γ→0 would require a separate result. Negative gamma is outside the proposed monotone insurer-cost interpretation.

The capstone is stated for deterministic nonstationary Markov policies only. It does not formally establish comparison with all randomised or history-dependent strategies, optimality for infinite horizons or an HJB verification theorem for continuous-time stochastic factors. A finite treaty price from other actuarial missions may later be substituted into ccc, after its own publication and consistency checks. No additional imported theorem dependencies are assumed here.

Evidence and source attribution

The source declarations have been checked by Prove2Me's private remote Lean compiler at the pinned Mathlib revision. The remote compiler's overall failure is deliberately caused by the incomplete proof bodies and a terminal type-mismatch sentinel; there were no unexpected declaration elaboration errors. This validates the proposed types and definitions, not any Lean proof. Independent high-precision finite model evaluation supports the mathematical direction, subject to the limitations of numerical evidence. The listed mathematical results remain proof obligations until accepted proof submissions exist.

[1] Bäuerle, Nicole and Glauner, Alexander (2022), Markov decision processes with recursive risk measures, European Journal of Operational Research, 296(3), 953–966. In the author preprint, Definition 4.6 states the one-step recursive risk operators, Theorem 4.7 establishes the finite-horizon Bellman value and existence of Markov optimal policies under Assumptions 3.1 and 4.2, and equation (4.2) is the one-step minimisation in the backward-induction proof. This mission explicitly specialises the framework to finite insurance costs and entropic valuation.

[2] Bäuerle, Nicole and Jaśkiewicz, Anna (2024), Markov decision processes with risk-sensitive criteria: an overview, Mathematical Methods of Operations Research, 99, 141–178. Example 1(a), equation (2) gives an entropic certainty equivalent in reward convention. The sign has been translated to an insurer cost/loss convention here.

[3] Actuarial Mathematics XVII: Finite-Horizon Markov Decision and Optimal Policy Valuation, previously published finite-state/action Markov recursion declarations. The present mission uses a distinct cost-minimising entropic stage operator, so it does not import XVII's reward-maximising Bellman definitions.

[4] Actuarial Mathematics XXI: Finite Exponential Premiums and Risk-Sensitive Retention, an earlier owner Draft concerning one-period entropic reinsurance premiums. Its unpublished declarations are not imported as available source modules.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XVIII: Expected-Value Reinsurance Premiums and Optimal Finite RetentionTextbook

Motivation: a priced excess-of-loss treaty and a finite retention decision

An excess-of-loss reinsurance treaty divides each insurance claim between the insurer and a reinsurer at an agreed retention. The cedant retains the first portion of the claim while the reinsurer pays the excess. The decision to purchase reinsurance trades off the reinsurer's premium against the insurer's retained claims and risk-capital requirement.

Bäuerle and Glauner [1, §6] discuss the classic expected-value premium principle for reinsurance,

πR(C)=(1+θ) E[C],\pi_R(C)=(1+\theta)\,\mathbb E[C],πR​(C)=(1+θ)E[C],

where CCC is the ceded claim amount and θ\thetaθ is the reinsurer's safety loading. Their paper develops a broader discrete-time dynamic reinsurance application under risk measures. Glauner [2] develops a risk-sensitive Markov decision formulation for dynamic reinsurance with general premium principles. Brachetta and Ceci [3] provide the related continuous-time stochastic-factor excess-of-loss problem, which includes a more complicated HJB verification theorem.

This mission establishes a finite-scenario, single-period insurance cost and finite-retention optimisation layer. It makes the expected-value premium algebra precise, shows how the safety loading changes expected insurer cost, and introduces an illustrative, transparently specified variance-based capital add-on. The finite optimum is then attained by one of a nonempty set of allowable retentions. This mathematical bridge can later be incorporated into Mission XVII's finite-horizon optimal policy recursion.

Split each claim at the retention

Let z∈Rz\in\mathbb Rz∈R be a realised gross insurance claim and a∈Ra\in\mathbb Ra∈R the retention limit. The actuarial interpretation concerns z≥0z\ge0z≥0, a≥0a\ge0a≥0; the Lean definitions extend the formulas to all reals for algebraic convenience.

The retained and ceded claims are respectively

r(z,a)=min⁡(z,a),c(z,a)=z−min⁡(z,a).r(z,a)=\min(z,a),\qquad c(z,a)=z-\min(z,a).r(z,a)=min(z,a),c(z,a)=z−min(z,a).

Consequently

r(z,a)+c(z,a)=z.r(z,a)+c(z,a)=z.r(z,a)+c(z,a)=z.

The insurer cannot retain more than either the original claim or its chosen retention. The ceded amount is nonnegative and decreases, or stays constant, as the retention is increased. These results follow directly from the minimum function without needing a particular claim distribution.

Finite-scenario expected-value reinsurance cost

Let Ω\OmegaΩ be a finite set of claim scenarios, with weights wω≥0w_\omega\ge0wω​≥0 summing to one, and gross claim function Z(ω)Z(\omega)Z(ω). Define

Ew[X]=∑ω∈ΩwωX(ω).\mathbb E_w[X]=\sum_{\omega\in\Omega}w_\omega X(\omega).Ew​[X]=ω∈Ω∑​wω​X(ω).

The expected retained loss is Ew[r(Z,a)]\mathbb E_w[r(Z,a)]Ew​[r(Z,a)], while the reinsurer's premium for the ceded part, under the expected-value premium principle with loading θ\thetaθ, is

πR(a)=(1+θ) Ew[c(Z,a)].\pi_R(a)=(1+\theta)\,\mathbb E_w[c(Z,a)].πR​(a)=(1+θ)Ew​[c(Z,a)].

The insurer's expected cost, comprising retained claims plus reinsurance premium, is

Cθ(a)=Ew[r(Z,a)]+(1+θ)Ew[c(Z,a)].C_\theta(a)=\mathbb E_w[r(Z,a)] +(1+\theta)\mathbb E_w[c(Z,a)].Cθ​(a)=Ew​[r(Z,a)]+(1+θ)Ew​[c(Z,a)].

Because retained and ceded claims add to gross claims, linearity gives the useful exact identity

Cθ(a)=Ew[Z]+θ Ew[c(Z,a)].\boxed{ C_\theta(a)=\mathbb E_w[Z] +\theta\,\mathbb E_w[c(Z,a)]. }Cθ​(a)=Ew​[Z]+θEw​[c(Z,a)].​

If θ=0\theta=0θ=0, total expected cost equals gross expected claims and is independent of retention. If θ≥0\theta\ge0θ≥0 and scenario weights are nonnegative, increasing retention reduces the expected ceded amount and therefore cannot increase this pure expected cost:

a≤b  ⟹  Cθ(b)≤Cθ(a).a\le b\implies C_\theta(b)\le C_\theta(a).a≤b⟹Cθ​(b)≤Cθ​(a).

This is not a general claim that greater retention is better for an insurer. It shows precisely why a risk criterion is needed when retention involves a trade-off: expected-value pricing with a nonnegative loading alone rewards retaining more risk.

An explicit retained-risk capital charge

To introduce a simple finite model of capital cost, define the retained-claim variance

Var⁡w[r(Z,a)]=∑ω∈Ωwω(r(Z(ω),a)−Ew[r(Z,a)])2.\operatorname{Var}_w[r(Z,a)] =\sum_{\omega\in\Omega}w_\omega \left(r(Z(\omega),a)-\mathbb E_w[r(Z,a)]\right)^2.Varw​[r(Z,a)]=ω∈Ω∑​wω​(r(Z(ω),a)−Ew​[r(Z,a)])2.

For nonnegative weights this variance is nonnegative. Let λ≥0\lambda\ge0λ≥0 be an illustrative cost per unit of retained variance and define

Jθ,λ(a)=Cθ(a)+λ Var⁡w[r(Z,a)].\boxed{ J_{\theta,\lambda}(a)= C_\theta(a)+ \lambda\,\operatorname{Var}_w[r(Z,a)]. }Jθ,λ​(a)=Cθ​(a)+λVarw​[r(Z,a)].​

The functional JJJ is an explicit modelling choice for this mission, not a formula attributed directly to Bäuerle and Glauner. Their paper uses more general risk measures and cost-of-capital principles, which motivate the need for a risk-sensitive criterion. A variance charge is a mathematically simple finite-scenario proxy rather than the complete dynamic capital methodology of [1–2].

Under λ≥0\lambda\ge0λ≥0 and nonnegative scenario weights,

Jθ,λ(a)≥Cθ(a).J_{\theta,\lambda}(a)\ge C_\theta(a).Jθ,λ​(a)≥Cθ​(a).

At λ=0\lambda=0λ=0, the added capital cost disappears. Unlike pure expected cost, the variance-adjusted objective need not be monotone in retention. The optimum can depend on the distribution, reinsurer loading and variance charge.

Selecting an optimal retention from a finite menu

Let AAA be a finite nonempty set of permissible treaty choices, and let α:A→R\alpha:A\to\mathbb Rα:A→R give the retention level associated with each choice. For an actuarial contract assume αa≥0\alpha_a\ge0αa​≥0, though the Lean maximum/minimum existence theorems need only finiteness and nonemptiness.

Define the best achievable risk-adjusted cost

J⋆=min⁡a∈AJθ,λ(αa).J^\star=\min_{a\in A}J_{\theta,\lambda}(\alpha_a).J⋆=a∈Amin​Jθ,λ​(αa​).

The supporting theorems establish that every candidate has cost at least J⋆J^\starJ⋆, and some admissible choice a⋆a^\stara⋆ achieves equality:

J⋆≤Jθ,λ(αa)for every a∈A,J⋆=Jθ,λ(αa⋆).J^\star\le J_{\theta,\lambda}(\alpha_a) \quad\text{for every }a\in A, \qquad J^\star=J_{\theta,\lambda}(\alpha_{a^\star}).J⋆≤Jθ,λ​(αa​)for every a∈A,J⋆=Jθ,λ​(αa⋆​).

This result is finite-action existence, not a claimed optimal continuous stochastic control. If the chosen retention menu and claim process become state dependent, this one-step reward or cost can be fed into the finite-horizon dynamic programming model of Mission XVII, subject to an appropriate specification of state transitions.

Formal theorem graph, boundaries and limitations

The draft has seven definitions: retained claim, ceded claim, finite weighted expectation, loaded expected premium cost, retained variance, risk-adjusted objective and finite optimal retention cost. Fourteen supporting theorem targets prove split and bounds, the monotone ceded claim, premium decomposition, zero loading, monotonic pure expected cost, nonnegative retained variance, zero variance-charge limit and finite argmin existence. The capstone combines universal optimal-cost lower bounds and an attaining retention choice.

The algebraic identities hold for arbitrary real weights and monetary amounts, with nonnegative weights required for probability inequalities and variance nonnegativity. A unit-sum condition is necessary for interpreting weights as a probability law, although the core finite-sum identities remain true without it. The actuarial discussion assumes nonnegative claims and retention, and nonnegative loading and capital coefficient where specified.

No Monte Carlo approximation, continuous-time wealth process, ruin probability, stochastic premium model or HJB partial differential equation is asserted. The mission is a finite expected-cost and finite risk-penalty formalisation, designed as a controlled predecessor to more complex dynamic reinsurance.

All Lean statements are proposed proof obligations. A private declaration-compilation check, even if all statements elaborate, is not an accepted proof, and unpublished local definitions cannot be treated as already importable in individual theorem files.

References

[1] Bäuerle, Nicole and Glauner, Alexander (2021), “Minimizing spectral risk measures applied to Markov decision processes”, Mathematical Methods of Operations Research, Section 6, Dynamic optimal reinsurance, particularly equation (6.1), the premium-principle discussion and the discrete-time risk-sensitive optimisation context.

[2] Glauner, Alexander (2022), “Dynamic reinsurance in discrete time minimizing the insurer's cost of capital”, Scandinavian Actuarial Journal, pp. 279–306. Establishes a broader discrete-time reinsurance/Markov decision framework with general risk measures and premium principles; it does not specifically prescribe the variance-only charge chosen here.

[3] Brachetta, Matteo and Ceci, Claudia (2019), “Optimal Excess-of-Loss Reinsurance for Stochastic Factor Risk Models”, Risks 7(2), article 48, and open preprint. Motivates the retained claim function and later continuous-time control research, not a direct derivation of this finite-stage capital add-on.

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Actuarial Mathematics XXI: Finite Exponential Premiums and Risk-Sensitive RetentionTextbook

Motivation and actuarial context

Insurance premiums are commonly calculated from an expected claim with a safety loading, but this approach does not by itself distinguish risks having the same mean and different tail behaviour. A classical alternative is the exponential premium principle, also known as the entropic certainty equivalent. It charges for the full distribution of a loss through the expectation of an exponential transformation. Tsanakas and Desli [1] explain how the exponential premium principle arises from expected utility theory, and compare its properties with other premium and risk-measure principles.

Bäuerle and Glauner [2–3] study risk-sensitive Markov decision processes, including recursively applied risk measures and the entropic functional. This motivates a later dynamic reinsurance programme. The present mission deliberately formalises the finite-scenario, one-step algebra: positivity of the exponential moment, cash additivity and monotonicity of the premium, and attainment of a risk-sensitive choice from a finite menu of reinsurance retentions. It is not a theorem about general stochastic processes, asymptotic ruin probabilities or continuous-time optimal control.

Finite weighted exponential valuation

Let Ω\OmegaΩ be a finite set of insurance-claim scenarios, X:Ω→RX:\Omega\to\mathbb RX:Ω→R a loss amount, and wωw_\omegawω​ the weight of each scenario. For a probability law assume

wω≥0,∑ω∈Ωwω=1.w_\omega\ge0,\qquad\sum_{\omega\in\Omega}w_\omega=1.wω​≥0,ω∈Ω∑​wω​=1.

The positive risk-sensitivity parameter is γ>0\gamma>0γ>0. Define the exponential moment

Mγ(X)=∑ω∈ΩwωeγX(ω).M_\gamma(X)=\sum_{\omega\in\Omega}w_\omega e^{\gamma X(\omega)}.Mγ​(X)=ω∈Ω∑​wω​eγX(ω).

For a nonnegative unit-sum weight law, Mγ(X)>0M_\gamma(X)>0Mγ​(X)>0 for every real γ\gammaγ, since at least one scenario has positive weight and every exponential factor is positive. This guarantees that the real logarithm is applied to a strictly positive number.

The entropic insurance premium is

ργ(X)=1γlog⁡Mγ(X).\boxed{ \rho_\gamma(X)=\frac{1}{\gamma}\log M_\gamma(X). }ργ​(X)=γ1​logMγ​(X).​

For any γ≠0\gamma\ne0γ=0 with positive exponential moment this is a well-defined finite certainty equivalent. The formal Lean definition uses real division for every γ\gammaγ, which is totalised at zero, but the actuarial interpretation and monotonicity theorem use strictly positive sensitivity. The formalisation does not assert that the γ=0\gamma=0γ=0 formula is the limiting expected-value premium: proving that limit requires a separate analytic theorem.

Premium principles and deterministic cash shifts

If X(ω)=cX(\omega)=cX(ω)=c in every scenario, then

Mγ(X)=eγc,ργ(X)=c,γ≠0.M_\gamma(X)=e^{\gamma c}, \qquad \rho_\gamma(X)=c,\quad\gamma\ne0.Mγ​(X)=eγc,ργ​(X)=c,γ=0.

In particular, zero claims have zero premium. The key cash-additivity or translation-invariance identity is

Mγ(X+c)=eγcMγ(X),M_\gamma(X+c)=e^{\gamma c}M_\gamma(X),Mγ​(X+c)=eγcMγ​(X),

and consequently, whenever Mγ(X)>0M_\gamma(X)>0Mγ​(X)>0 and γ≠0\gamma\ne0γ=0,

ργ(X+c)=ργ(X)+c.\boxed{\rho_\gamma(X+c)=\rho_\gamma(X)+c.}ργ​(X+c)=ργ​(X)+c.​

Thus a known extra expense of ccc is added directly to the premium, rather than changing how stochastic variability is priced. This monetary risk-measure property is one of the central axioms discussed by Tsanakas and Desli [1].

For two scenario claim amounts satisfying X(ω)≤Y(ω)X(\omega)\le Y(\omega)X(ω)≤Y(ω) for every ω\omegaω, positive sensitivity γ>0\gamma>0γ>0, and nonnegative probability weights, exponential and logarithmic monotonicity give

ργ(X)≤ργ(Y).\rho_\gamma(X)\le\rho_\gamma(Y).ργ​(X)≤ργ​(Y).

The supporting theorems prove the exponential-moment ordering first, then transfer it through the increasing logarithm and division by γ>0\gamma>0γ>0. The formal source does not assume the two risks are independent or that a moment-generating function exists outside the finite scenario model.

A finite excess-of-loss reinsurance decision

Suppose the cedant chooses an excess-of-loss retention aaa. For a realised gross claim zzz, the amount retained by the insurer is

r(z,a)=min⁡(z,a).r(z,a)=\min(z,a).r(z,a)=min(z,a).

Conventional insurance interpretation requires nonnegative claims and retention. The underlying Lean function is real-valued on all arguments so algebraic order properties can be stated without additional domain restrictions.

Let q(a)q(a)q(a) be a deterministic reinsurance premium quoted for retention aaa. The combined risk-sensitive cost of the retention choice is

Jγ(a)=q(a)+ργ(r(Z,a)).\boxed{ J_\gamma(a)=q(a)+\rho_\gamma(r(Z,a)). }Jγ​(a)=q(a)+ργ​(r(Z,a)).​

This is a model choice: the insurer adds the quoted cost of its treaty to the entropic valuation of the stochastic losses it still retains. The quoted premium is an arbitrary input function. The mission does not assume it decreases with higher retention, or that it has been calculated by the reinsurer using the same exponential premium principle.

Let AAA be a finite, nonempty set of allowed treaty choices, with α:A→R\alpha:A\to\mathbb Rα:A→R mapping each choice to a retention level. The optimal cost is

Jγ⋆=min⁡a∈AJγ(αa).J_\gamma^\star=\min_{a\in A}J_\gamma(\alpha_a).Jγ⋆​=a∈Amin​Jγ​(αa​).

Since the action set is finite and nonempty, the minimum is attained. The capstone establishes that every menu action has cost at least Jγ⋆J_\gamma^\starJγ⋆​, and there is an action a⋆a^\stara⋆ satisfying

Jγ⋆≤Jγ(αa)∀a∈A,Jγ⋆=Jγ(αa⋆).\boxed{ J_\gamma^\star\le J_\gamma(\alpha_a)\quad\forall a\in A, \qquad J_\gamma^\star=J_\gamma(\alpha_{a^\star}). }Jγ⋆​≤Jγ​(αa​)∀a∈A,Jγ⋆​=Jγ​(αa⋆​).​

This is finite-menu optimisation. It does not by itself establish a finite-horizon optimal policy, solve a risk-sensitive Bellman equation, or prove optimality over a continuous retention interval. Those extensions require explicit state transitions and additional regularity or compactness assumptions.

Formal proof graph and important boundaries

Five definitions establish the finite exponential moment, entropic premium, retained claim, risk-sensitive one-period reinsurance cost, and finite-menu optimal cost. Thirteen supporting theorems establish nonnegative and positive exponential moments, constant-claim cases, factorisation and cash additivity, exponential and premium monotonicity, monotonic retained claim, and finite argmin bounds and attainment. The capstone combines finite-menu domination and an attaining retention.

The definitions and theorem statements apply to arbitrary finite types and real weights where algebraically meaningful; the probabilistic interpretation needs nonnegative weights of total one. Finite moments are automatically finite for real-valued scenarios, but the logarithm requires a positive moment for the usual risk valuation. The proof of cash additivity uses γ≠0\gamma\ne0γ=0. The monotonicity theorem uses γ>0\gamma>0γ>0 and nonnegative scenario weights.

This draft is a finite actuarial risk-valuation precursor. The literature includes further results, such as comparisons with expected value, convexity and recursion of risk measures. They are not declared proved by this mission. Neither a successfully elaborated Lean statement nor an independent arithmetic test constitutes an accepted Lean proof.

References

[1] Tsanakas, Andreas and Desli, Evangelia (2003), “Risk measures and theories of choice”, British Actuarial Journal, 9(4), pp. 959–991. Discusses exponential premium calculation, expected utility and the monetary properties and limitations of different risk measures. Open academic record.

[2] Bäuerle, Nicole and Glauner, Alexander (2021), “Minimizing spectral risk measures applied to Markov decision processes”, Mathematical Methods of Operations Research. Introduces the entropic certainty equivalent as γ−1log⁡E[eγX]\gamma^{-1}\log\mathbb E[e^{\gamma X}]γ−1logE[eγX] when discussing risk-sensitive decision processes.

[3] Bäuerle, Nicole and Glauner, Alexander (2022), “Markov decision processes with recursive risk measures”, European Journal of Operational Research, 296(3), pp. 953–966. Develops recursive risk-sensitive Bellman equations and optimal Markov policies under suitable assumptions; the present mission only proves the simpler one-period finite-scenario predecessor.

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Actuarial Mathematics XIX: Finite-Horizon Reserve Loss and Hattendorff Innovation BridgeTextbook

Motivation and connection to discrete Hattendorff's theorem

A prospective insurance reserve is an actuarial estimate of future net obligations conditional on the policy being in force. A realised claim can differ from this estimate because death may occur earlier or later than expected. For a fully discrete life insurance contract, Hattendorff's theorem allocates the variance of the insurer's loss to individual policy years. A decisive preliminary identity is that the realised insurer loss at issue, after subtracting the opening reserve, equals a sum of discounted net amounts at risk multiplied by centred mortality innovations.

Shiu and Xiong [1] express loss at issue in their equation (1), derive a one-year reserve finite-difference identity in equation (3), and sum the resulting reserve changes in equations (4)–(5). This mission makes the corresponding finite-horizon, pathwise reserve-loss identity precise, including a terminal prospective reserve for policies still in force when the chosen horizon ends. It is the cashflow side of the finite-scenario innovation analysis proposed in Mission XVI.

The central distinction is important: the mission proves a deterministic identity for each possible curtate death year, provided the annual conditional rates and reserve recurrence are consistent. It does not itself construct the mortality probability distribution, derive conditional rates from a measure, prove annual orthogonality, or establish the final variance formula. Those tasks belong to the probabilistic components in XVI and their eventual integration.

Contract timing and cashflow variables

Let K∈NK\in\mathbb NK∈N denote curtate future lifetime. The event K=tK=tK=t means the insured dies during policy year ttt, with the associated benefit paid at time t+1t+1t+1. Define the real-valued indicators

St(K)=1{K≥t},Dt(K)=1{K=t}.S_t(K)=\mathbf1_{\{K\ge t\}}, \qquad D_t(K)=\mathbf1_{\{K=t\}}.St​(K)=1{K≥t}​,Dt​(K)=1{K=t}​.

These satisfy the disjoint partition

St(K)=Dt(K)+St+1(K).S_t(K)=D_t(K)+S_{t+1}(K).St​(K)=Dt​(K)+St+1​(K).

Let n∈Nn\in\mathbb Nn∈N be the finite valuation horizon, v∈Rv\in\mathbb Rv∈R a per-year discount factor, πt\pi_tπt​ the premium at the start of policy year ttt, bt+1b_{t+1}bt+1​ the death benefit at its end, and VtV_tVt​ the prospective reserve at time ttt on the in-force basis.

The finite-horizon net insurer loss, including the reserve required at the horizon for a policy still in force, is

Ln(K)=∑0≤t<n ⁣[vt+1bt+1Dt(K)−vtπtSt(K)]+vnVnSn(K).\boxed{ L_n(K)= \sum_{0\le t<n}\! \left[v^{t+1}b_{t+1}D_t(K) -v^t\pi_t S_t(K)\right] +v^nV_nS_n(K). }Ln​(K)=0≤t<n∑​[vt+1bt+1​Dt​(K)−vtπt​St​(K)]+vnVn​Sn​(K).​

The first term values year-end death benefits, the second subtracts premiums paid at the beginning of each covered year only while the policy remains in force, and the third carries forward the continuing liability.

For n=0n=0n=0 no premium or death benefit is included and L0(K)=V0L_0(K)=V_0L0​(K)=V0​. If K≥nK\ge nK≥n, the insurer has not paid a death benefit during the chosen horizon, and the value includes vnVnv^nV_nvnVn​. Therefore the mission does not assume that everyone dies before the selected horizon, nor does it discard an outstanding terminal liability.

One-year reserve recurrence

Let qtq_tqt​ denote the conditional probability of death during policy year ttt, given the policy is still in force at its start, and let ptp_tpt​ denote conditional survival through that year. Their one-year normalisation is

pt+qt=1.p_t+q_t=1.pt​+qt​=1.

Let the annual prospective reserve balance be

Vt+πt=v(ptVt+1+qtbt+1).\boxed{ V_t+\pi_t =v\left(p_tV_{t+1}+q_tb_{t+1}\right). }Vt​+πt​=v(pt​Vt+1​+qt​bt+1​).​

This is the discrete one-year recurrence appearing in [1, equation (3)] before multiplication by vtv^tvt and rearrangement. The source has an annual premium paid at the beginning and a death benefit at the end. The rates pt,qtp_t,q_tpt​,qt​, benefit bt+1b_{t+1}bt+1​, premium πt\pi_tπt​ and reserve sequence VtV_tVt​ are inputs to the formal statement. Their actuarial origin is not silently assumed.

The formalisation deliberately permits arbitrary real quantities for the algebra. The usual probability interpretation additionally requires 0≤pt,qt≤10\le p_t,q_t\le10≤pt​,qt​≤1, and the conventional financial interpretation requires a valid positive discount factor. These stronger conditions are not needed for the pathwise identity itself once the two recurrence equalities are assumed.

Net amount at risk and annual mortality surprise

The year-ttt realised mortality surprise is

It(K)=Dt(K)−qtSt(K).I_t(K)=D_t(K)-q_tS_t(K).It​(K)=Dt​(K)−qt​St​(K).

This equals 1−qt1-q_t1−qt​ on death in year ttt, −qt-q_t−qt​ when the insured survives through year ttt, and zero after the policy has ended. It is a pointwise cashflow expression here; statistical centring requires a later assumption that the supplied qtq_tqt​ is the correct conditional death probability.

Define the discounted net amount at risk and its annual contribution:

ρt=vt+1(bt+1−Vt+1),ρtIt(K).\rho_t=v^{t+1}(b_{t+1}-V_{t+1}), \qquad \rho_tI_t(K).ρt​=vt+1(bt+1​−Vt+1​),ρt​It​(K).

The finite innovation value is

Zn(K)=∑0≤t<nρtIt(K).Z_n(K)=\sum_{0\le t<n}\rho_tI_t(K).Zn​(K)=0≤t<n∑​ρt​It​(K).

Unlike the more general mortality innovation mission, this draft explicitly connects the coefficient ρt\rho_tρt​ to the death benefit and prospective reserve rather than treating it as an arbitrary monetary sequence.

One-year cancellation and the finite-horizon theorem

To see the mechanism, consider the change in the reserve-adjusted insurer loss when the horizon increases from ttt to t+1t+1t+1:

Lt+1(K)−Lt(K)=vt+1bt+1Dt(K)−vtπtSt(K)+vt+1Vt+1St+1(K)−vtVtSt(K).\begin{aligned} L_{t+1}(K)-L_t(K) ={}&v^{t+1}b_{t+1}D_t(K) -v^t\pi_tS_t(K)\\ &+v^{t+1}V_{t+1}S_{t+1}(K) -v^tV_tS_t(K). \end{aligned}Lt+1​(K)−Lt​(K)=​vt+1bt+1​Dt​(K)−vtπt​St​(K)+vt+1Vt+1​St+1​(K)−vtVt​St​(K).​

Substituting St+1=St−DtS_{t+1}=S_t-D_tSt+1​=St​−Dt​, the one-year reserve balance, and pt+qt=1p_t+q_t=1pt​+qt​=1 reduces that entire expression to

Lt+1(K)−Lt(K)=vt+1(bt+1−Vt+1)(Dt(K)−qtSt(K)).\boxed{ L_{t+1}(K)-L_t(K) =v^{t+1}(b_{t+1}-V_{t+1}) \left(D_t(K)-q_tS_t(K)\right). }Lt+1​(K)−Lt​(K)=vt+1(bt+1​−Vt+1​)(Dt​(K)−qt​St​(K)).​

Sum this identity from t=0t=0t=0 to n−1n-1n−1. All intermediate reserve balances cancel, leaving the capstone:

Ln(K)−V0=∑0≤t<nvt+1(bt+1−Vt+1)It(K)=Zn(K).\boxed{ L_n(K)-V_0 =\sum_{0\le t<n} v^{t+1}(b_{t+1}-V_{t+1})I_t(K) =Z_n(K). }Ln​(K)−V0​=0≤t<n∑​vt+1(bt+1​−Vt+1​)It​(K)=Zn​(K).​

This equality holds for every KKK and finite nnn provided the year-by-year normalisation and reserve balance hold on the relevant years. It includes n=0n=0n=0 without a special artificial convention and it retains the terminal liability already included in LnL_nLn​. Neither V0=0V_0=0V0​=0 nor Vn=0V_n=0Vn​=0 is required.

When later coupled to a genuine mortality distribution and the statistical identities in Mission XVI, the representation provides the missing bridge for a finite-horizon discrete Hattendorff variance theorem. Such a coupling must explicitly reconcile the probability model, its conditional rates, and the definition of weighted variance. No published theorem is treated as a proved dependency merely because it has appeared as an Open Prove2Me target.

Formal proof graph and publication safeguards

Six definitions introduce the in-force and death-year indicators, the realised finite loss with terminal reserve, an annual reserve balance predicate, a centred mortality surprise and the discounted net-at-risk innovation sum. Twelve supporting theorems establish time-zero and after-death indicators, the disjoint event partition, the zero-horizon loss and innovation, realised death/survival shock cases, finite-sum successor identities and the pivotal one-year reserve-adjusted loss identity. The capstone proves the finite pathwise equality for every curtate death year under annual assumptions for all years t<nt<nt<n.

All source declarations use correct leading Lean imports. Every local definition import is required by the declaration it uses; the dependency graph must remain acyclic. Preliminary private remote elaboration checks only statement syntax and types. It is not an accepted Lean proof, nor does it show that not-yet-published definition modules are individually importable.

References

[1] Shiu, Elias S. W. and Xiong, Xiaoyi (2021), “An elementary derivation of Hattendorff's theorem”, European Actuarial Journal, 11, pp. 319–323, equations (1), (3), (4) and (5). In particular, their one-year reserve recurrence and summation-by-parts argument motivate the loss-to-innovation representation.

[2] Gerber, Hans U. (1997), Life Insurance Mathematics, third edition, Springer, Chapter 6, §6.7, allocation of the overall life-insurance loss to individual policy years.

[3] Gerber, Hans U., Leung, Bartholomew P. K. and Shiu, Elias S. W. (2003), “Indicator Function and Hattendorff Theorem”, North American Actuarial Journal, 7(1), pp. 38–47. Supports the indicator-based perspective and the relationship between mortality surprises and annual loss allocation.

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Actuarial Mathematics XV: Finite-Action Excess-of-Loss Reinsurance and Bellman ValuationTextbook

Motivation and research scope

An insurer can transfer part of an unusually large claim to a reinsurer using an excess-of-loss contract. The insurer chooses a retention amount and remains liable for each claim only up to that amount, while the reinsurer covers the excess. A retention strategy trades off the cost of reinsurance protection against the amount of insurance loss retained.

Brachetta and Ceci (2019) investigate optimal excess-of-loss retention under a stochastic environment which affects claim frequency, claim severity and reinsurance premiums [1]. Their actual results use a marked point process, an exogenous diffusion factor, terminal exponential utility, a Hamilton–Jacobi–Bellman equation and a continuous-time verification theorem. This mission is not a purported proof of that stochastic HJB result.

Instead, it creates a rigorous finite-scenario, finite-action precursor: exact excess-of-loss claim sharing, weighted retained-claim valuation and the Bellman optimisation operator for a finite collection of actions. The direct source for discrete finite-horizon optimality is Puterman, Markov Decision Processes, Chapter 4 [2], which develops dynamic programming and the existence of deterministic optimal actions. A genuine stochastic reinsurance-control model can later replace the discrete scenario assumptions, construct the controlled wealth process and address the full HJB theorem of [1].

Excess-of-loss retention and ceded claims

Let z∈Rz\in\mathbb Rz∈R be a gross claim amount and a∈Ra\in\mathbb Ra∈R be the retention threshold. The insured-life/non-life interpretation requires z≥0z\ge0z≥0 and a≥0a\ge0a≥0, but the Lean functions themselves are defined algebraically on all real numbers.

The insurer retains

r(z,a)=min⁡(z,a)r(z,a)=\min(z,a)r(z,a)=min(z,a)

and cedes to the reinsurer

c(z,a)=z−min⁡(z,a).c(z,a)=z-\min(z,a).c(z,a)=z−min(z,a).

Consequently the claim is allocated without double counting:

r(z,a)+c(z,a)=z.r(z,a)+c(z,a)=z.r(z,a)+c(z,a)=z.

The supporting theorems show that retained loss cannot exceed either the original claim or the retention limit, that ceded loss is nonnegative, and that raising the retention threshold cannot reduce the retained loss. For nonnegative claims, setting a=0a=0a=0 leaves no retained loss. If z≤az\le az≤a, no excess is ceded.

The division of claim amounts follows the surplus decomposition in Brachetta and Ceci [1, §2], where the retained claim is expressed by the minimum of the claim size and the control.

Finite-scenario expected retained loss and cost

Let Ω\OmegaΩ be a finite set of claim scenarios. For scenario ω\omegaω, let zωz_\omegazω​ be the gross claim and wωw_\omegawω​ a probability weight. Probability interpretation requires

wω≥0,∑ω∈Ωwω=1.w_\omega\ge0,\qquad \sum_{\omega\in\Omega}w_\omega=1.wω​≥0,ω∈Ω∑​wω​=1.

The expected retained claim amount for retention aaa is

Ew[r(Z,a)]=∑ω∈Ωwωmin⁡(zω,a).\mathbb E_w[r(Z,a)] =\sum_{\omega\in\Omega}w_\omega\min(z_\omega,a).Ew​[r(Z,a)]=ω∈Ω∑​wω​min(zω​,a).

Let q(a)q(a)q(a) be the reinsurance premium charged for that retention. The one-period expected insurance and reinsurance cost is

C(a)=q(a)+Ew[r(Z,a)].C(a)=q(a)+\mathbb E_w[r(Z,a)].C(a)=q(a)+Ew​[r(Z,a)].

This simple expected-cost criterion captures the basic trade-off: a lower retention reduces claims retained, generally at the cost of a higher reinsurance premium. The theorem definitions impose no monotonicity on the premium function qqq; if actuarial monotonicity is required, it must be included as a separate hypothesis.

The finite expected-loss function is nonnegative under nonnegative scenarios, retentions and weights. It is increasing in retention when the weights are nonnegative. These are algebraic checks, not a claim that minimising this expected cost is equivalent to maximising exponential terminal utility in [1]. The source article uses the latter, more sophisticated objective.

Discrete optimal decisions and Bellman operator

To prepare for multi-year optimal reinsurance, let SSS be a finite state space, AAA a nonempty finite admissible action set, and P(s,a,t)P(s,a,t)P(s,a,t) the one-step transition weight from state sss to ttt when action aaa is selected. Let r(s,a)r(s,a)r(s,a) be the one-period reward, vvv a deterministic discount factor and N(t)N(t)N(t) a next-period value.

The return associated with one action is

Q(s,a)=r(s,a)+v∑t∈SP(s,a,t)N(t).Q(s,a)=r(s,a)+v\sum_{t\in S}P(s,a,t)N(t).Q(s,a)=r(s,a)+vt∈S∑​P(s,a,t)N(t).

The finite-action Bellman operator is

(TN)(s)=max⁡a∈AQ(s,a).(TN)(s)=\max_{a\in A}Q(s,a).(TN)(s)=a∈Amax​Q(s,a).

Since AAA is nonempty and finite, the maximum is attained. The capstone formally targets

Q(s,a)≤(TN)(s)for every a∈A,(TN)(s)=Q(s,a⋆)for some a⋆∈A.\begin{aligned} Q(s,a)&\le(TN)(s)\quad\text{for every }a\in A,\\ (TN)(s)&=Q(s,a^\star) \quad\text{for some }a^\star\in A. \end{aligned}Q(s,a)(TN)(s)​≤(TN)(s)for every a∈A,=Q(s,a⋆)for some a⋆∈A.​

This is the finite-horizon principle of selecting an optimal discrete action, not continuous-time HJB verification. Puterman [2, Chapter 4] discusses the Bellman recursion and the existence of deterministic Markov policies for finite-horizon decision problems. To model reinsurance with this operator, later theorems must specialise AAA to admissible retention limits, define state-dependent premium and claim distributions, and prove row-stochasticity and any desired utility assumptions.

The draft intentionally does not claim that arbitrary matrix entries PPP define a valid probability law. The finite Bellman maximum and the two capstone inequalities are algebraically meaningful for arbitrary real weights; a controlled Markov-process interpretation requires additional conditions.

Formal definitions and proof structure

Five definitions introduce gross claim retention, ceded claim, finite weighted retained loss, one-year reinsurance cost and the finite-action Bellman operator. Twelve supporting theorems cover the claim split, nonnegative and monotone retention results, expected retained-loss monotonicity, stage cost and Bellman lower bounds. The capstone packages upper domination and attainment of the Bellman maximum.

All local imports appear before other Lean commands. Every theorem is currently a proposed proof obligation; the source-elaboration checks are private and do not constitute accepted proofs. Definitions that are not yet published cannot be assumed importable in the production theorem preview.

This is a foundations mission for a later reinsurance-control programme. A credible subsequent research mission will need the full conditional marked-point-process model, wealth dynamics, admissible adapted controls, exponential utility and the analytic regularity assumptions of [1] before attempting its backward-PDE verification result.

References

[1] Brachetta, Matteo and Ceci, Claudia (2019), “Optimal Excess-of-Loss Reinsurance for Stochastic Factor Risk Models”, Risks, 7(2), article 48. The claim process and retention control are in §2, the HJB formulation in §3, optimal strategies in §4 and the verification argument in §5. This article motivates the reinsurance problem but its continuous-time verification theorem is outside the present draft.

[2] Puterman, Martin L. (1994), Markov Decision Processes: Discrete Stochastic Dynamic Programming, Chapter 4, “Finite-Horizon Markov Decision Processes”, Wiley, pp. 74–118. Includes finite-horizon policy evaluation, optimality equations, deterministic Markov policies and backward induction. This is the direct source for the discrete Bellman stage.

[3] Brachetta and Ceci (2019), open preprint, arXiv:1904.05422. Independent accessible source for the original stochastic-factor control problem and its distinct continuous-time assumptions.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XIII: Annual Loss Allocation and Finite Hattendorff IdentityTextbook

Motivation and actuarial context

A prospective life insurance reserve describes the expected remaining loss on a policy at a valuation date. An alternative way to understand the insurer's total future loss is to allocate it between individual policy years. Each year produces an insurance cashflow and a change in the reserve needed to support future benefits. When properly centred by the reserve balance, the resulting annual gains have expectation zero. Hattendorff's theorem connects this allocation to the striking result that losses for distinct years are uncorrelated and the variance of total discounted loss is the sum of their individual discounted variances.

The classical finite annual result is covered by Gerber, Life Insurance Mathematics, third edition, §6.7, particularly equations (6.7.3) and (6.7.6)–(6.7.10) [1]. A modern actuarial derivation is developed in the European Actuarial Journal article An elementary derivation of Hattendorff's theorem [2]. The connection to martingale increments is emphasised by Norberg [3] and by Gerber, Leung and Shiu [4].

This mission formalises a finite-scenario annual-loss allocation and Hattendorff-style variance identity. It makes the distinction between a proved algebraic decomposition and the deeper stochastic theorem explicit: annual orthogonality is a hypothesis of the capstone, with its derivation from conditional mortality and reserve dynamics reserved for a subsequent extension. Thus the mission does not claim that an arbitrary pair of yearly cashflows is uncorrelated.

Finite mortality scenarios and expected values

Let Ω\OmegaΩ be a finite sample space, and let wωw_\omegawω​ denote the probability assigned to scenario ω\omegaω. A valid scenario probability law has nonnegative weights summing to one. The mission defines the finite weighted expectation

Ew[X]=∑ω∈ΩwωX(ω).\mathbb E_w[X]=\sum_{\omega\in\Omega}w_\omega X(\omega).Ew​[X]=ω∈Ω∑​wω​X(ω).

Its supporting results establish expected values of constants and linear combinations. For scenario cashflows XXX and YYY, weighted variance and covariance are defined by

Var⁡w(X)=∑ωwω(X(ω)−Ew[X])2,Cov⁡w(X,Y)=∑ωwω(X(ω)−Ew[X])(Y(ω)−Ew[Y]).\begin{aligned} \operatorname{Var}_w(X) &=\sum_\omega w_\omega \left(X(\omega)-\mathbb E_w[X]\right)^2,\\ \operatorname{Cov}_w(X,Y) &=\sum_\omega w_\omega \left(X(\omega)-\mathbb E_w[X]\right) \left(Y(\omega)-\mathbb E_w[Y]\right). \end{aligned}Varw​(X)Covw​(X,Y)​=ω∑​wω​(X(ω)−Ew​[X])2,=ω∑​wω​(X(ω)−Ew​[X])(Y(ω)−Ew​[Y]).​

The definitions work for arbitrary real arrays of weights, while the actuarial probability interpretation assumes valid scenario probabilities. Finite sums avoid moment-integrability issues without imposing an artificial condition such as independence between years.

Annual insurer gains and reserve changes

Let Ck(ω)C_k(\omega)Ck​(ω) be the net insurer cash outgo during policy year kkk, measured at that year's start, and let RkR_kRk​ be the deterministic opening prospective reserve under a given in-force valuation basis. With per-year discount factor vvv, define the annual gain or loss component

Gk(ω)=Ck(ω)+vRk+1−Rk.G_k(\omega)=C_k(\omega)+vR_{k+1}-R_k.Gk​(ω)=Ck​(ω)+vRk+1​−Rk​.

The term vRk+1vR_{k+1}vRk+1​ represents the discounted liability carried into the next year, while RkR_kRk​ is the reserve released from the opening position. The sign convention is insurer loss, so positive values represent net outgo or an adverse change.

If the annual reserve balance is

Ew[Ck]+vRk+1=Rk,\mathbb E_w[C_k]+vR_{k+1}=R_k,Ew​[Ck​]+vRk+1​=Rk​,

then linearity gives

Ew[Gk]=0.\mathbb E_w[G_k]=0.Ew​[Gk​]=0.

This is the first actuarial component of Hattendorff's framework: properly reserved annual losses are centred under the valuation basis. The finite scenario weights need to sum to one, and the reserve balance must be assumed or established. Merely defining GkG_kGk​ does not give it zero mean.

Discounted loss allocation and telescoping

The total discounted annual gain through nnn years is

Ln(ω)=∑0≤k<nvkGk(ω).L_n(\omega)=\sum_{0\le k<n}v^kG_k(\omega).Ln​(ω)=0≤k<n∑​vkGk​(ω).

Expanding the annual gain definition and telescoping the reserve terms gives the pathwise identity

Ln(ω)=∑0≤k<nvkCk(ω)+vnRn−R0.\boxed{ L_n(\omega)= \sum_{0\le k<n}v^k C_k(\omega) +v^n R_n-R_0. }Ln​(ω)=0≤k<n∑​vkCk​(ω)+vnRn​−R0​.​

The terminal reserve is retained explicitly. It must not be assumed zero for an arbitrary incomplete policy horizon. This exact finite-period formula corresponds to the annual allocation of loss and reserve changes discussed in [1, §6.7, equation (6.7.3)], with the horizon and terminal liability clearly stated.

The empty-term case has L0=0L_0=0L0​=0. Increasing the horizon from nnn to n+1n+1n+1 adds precisely vnGnv^nG_nvnGn​. These boundary and recursion lemmas form a useful independent verification layer for the finite sum.

Orthogonality and the variance decomposition

When distinct annual gains have zero covariance,

Cov⁡w(Gi,Gj)=0(i≠j,  i,j<n),\operatorname{Cov}_w(G_i,G_j)=0 \qquad (i\ne j,\;i,j<n),Covw​(Gi​,Gj​)=0(i=j,i,j<n),

their discounted aggregate variance has no cross-year terms:

Var⁡w(Ln)=∑0≤k<nv2kVar⁡w(Gk).\boxed{ \operatorname{Var}_w(L_n) =\sum_{0\le k<n}v^{2k}\operatorname{Var}_w(G_k). }Varw​(Ln​)=0≤k<n∑​v2kVarw​(Gk​).​

Importantly, uncorrelated does not mean independent. Annual losses are linked by the same insured life, survival history and reserve process. Hattendorff's theorem establishes the required uncorrelatedness from the correct conditional insurance model; the zero-covariance condition is an explicit hypothesis in this mission's finite-scenario algebraic capstone. This distinction is important for the formalisation and is consistent with [1, equations (6.7.6)–(6.7.8)] and the martingale explanation in [3–4].

The supporting theorem on variance of a sum, variance scaling and covariance symmetry makes the algebra behind the annual allocation explicit. Zero-mean gain and zero-covariance assumptions must be separately justified when moving from this finite abstract setting to a particular mortality model.

Capstone and subsequent formal development

The capstone assumes a finite scenario law whose weights sum to one, a sequence of yearly cashflows CkC_kCk​, deterministic reserves RkR_kRk​, a reserve balance for each year k<nk<nk<n, and pairwise zero covariance of the resulting annual gains. It then proves three statements together: each year's gain is centred, the discounted variance splits additively by year, and the discounted sum telescopes to net cashflows plus the terminal reserve less opening reserve.

Five definitions establish weighted expectation, annual reserve gain, discounted aggregate gain, variance and covariance. Thirteen supporting theorem targets handle elementary expectation algebra, finite-year telescoping, zero-mean reserve gains, covariance symmetry and orthogonal variance decomposition. A capstone combines these results.

This is explicitly the finite algebraic and reserve-accounting stage, not a complete proof of Hattendorff's theorem for arbitrary life insurance contracts. A later mission should construct the curtate-lifetime annual innovations using the published reserve recursions of Mission XI, establish the conditional mean-zero property from survival information and derive cross-year orthogonality without assuming it. Only that later bridge will discharge the substantive stochastic obligation. No independence claim is made.

Every item is a proposed Lean statement. The isolated-module imports appear before other Lean commands, and no unpublished definition is treated as already available to the live compiler.

References

[1] Gerber, Hans U. (1997), Life Insurance Mathematics, third edition, Springer, Chapter 6, §6.7, Allocation of the Overall Loss to Policy Years, equations (6.7.3)–(6.7.10). Publisher book record.

[2] An elementary derivation of Hattendorff's theorem, European Actuarial Journal (2021), DOI: 10.1007/s13385-020-00256-9. Develops the annual insurer-loss formula using the prospective reserve recurrence.

[3] Norberg, Ragnar (1992), “Hattendorff's theorem and Thiele's differential equation generalized”, Scandinavian Actuarial Journal, pp. 2–14. Places the annual uncorrelated-loss principle in a broader stochastic and martingale setting.

[4] Gerber, Hans U., Leung, Bartholomew P. K. and Shiu, Elias S. W. (2003), “Indicator Function and Hattendorff Theorem”, North American Actuarial Journal, 7(1), pp. 38–47. Relates the actuarial theorem to uncorrelated martingale increments.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XIV: Multiple-Decrement Annual Reserve PremiumsTextbook

Motivation and actuarial context

A traditional life-insurance model may have one way of exiting the insured state, namely death. Many actuarial contracts instead allow multiple mutually exclusive decrements. A policyholder might exit through death, disability, withdrawal or retirement, and different causes may trigger different benefits. A net premium reserve must therefore allow one-year payments that vary by the cause of exit, as well as the liability continuing for policies that do not exit.

Gerber, Life Insurance Mathematics, third edition, Chapter 7 §7.5 [1], derives the multiple-decrement reserve and its one-year recursion, followed by a decomposition of premium into reserve accumulation and the expected cost of the net amounts at risk. The same models are related to the broader multiple-state framework developed in Dickson, Hardy and Waters (2009), Chapter 8, including §8.8 on multiple decrements [2].

This mission formalises the one-year multiple-decrement reserve balance and premium decomposition for a finite set of causes. It is a deliberately local actuarial model: it handles one policy year and deterministic opening and closing reserves, without assuming that the complete lifetime-dependent reserve functions from Missions XI or XII have already been published.

One-year decrement law

Let JJJ be a finite set of mutually exclusive causes of exit. Fix a policy in force at the start of the year. Let ppp denote the conditional probability of surviving in force to the following year, and qjq_jqj​ the conditional probability of decrement cause j∈Jj\in Jj∈J during the year.

The one-year decrement law is valid when

p≥0,qj≥0,p+∑j∈Jqj=1.p\ge0,\qquad q_j\ge0,\qquad p+\sum_{j\in J}q_j=1.p≥0,qj​≥0,p+j∈J∑​qj​=1.

The possible decrement causes are alternative outcomes of the same year. Their probabilities are added because the causes are mutually exclusive; they are not independent risks. The survival probability refers to remaining in force, rather than necessarily being alive in every possible post-decrement state.

The formal model treats JJJ as any finite type. No nonempty-type hypothesis is required: if JJJ is empty, the unit-probability law forces p=1p=1p=1 and reduces to certain survival, without exit benefits.

Benefit payments and the annual reserve balance

Let bjb_jbj​ be the benefit payable at the end of the year following exit for cause jjj. The conditional expected exit benefit before discounting is

B=∑j∈Jqjbj.B=\sum_{j\in J}q_jb_j.B=j∈J∑​qj​bj​.

Let RRR be the reserve immediately before the current premium, let R+R_+R+​ denote the reserve required at the next annual valuation for surviving policies, and let vvv be the annual discount factor. Assume the year-end reserve for policies which exit is zero after payment of the cause-specific benefit. Under this timing, the expected present value of the following-year liability is

v(pR++∑j∈Jqjbj).v\left(pR_+ +\sum_{j\in J}q_jb_j\right).v​pR+​+j∈J∑​qj​bj​​.

The required premium Π\PiΠ is defined by the annual reserve balance

R+Π=v(pR++∑j∈Jqjbj).\boxed{R+\Pi=v\left(pR_+ +\sum_{j\in J}q_jb_j\right).}R+Π=v​pR+​+j∈J∑​qj​bj​​.​

Equivalently, the formula defines

Π=v(pR++B)−R.\Pi=v\left(pR_++B\right)-R.Π=v(pR+​+B)−R.

This is the discrete conditional one-year multiple-decrement generalisation of the annual life-reserve recursion in [1, equation (7.5.2)]. It does not assert that the reserves RRR and R+R_+R+​ were derived from a complete prospective valuation, nor that an arbitrary premium chosen externally automatically satisfies the balance. Those tasks require a separate multi-year model.

Savings and risk premium components

The one-year required premium can be separated into two economically interpretable parts. The savings premium grows the opening reserve towards the next reserve:

Πsav=vR+−R.\Pi^{\mathrm{sav}}=vR_+-R.Πsav=vR+​−R.

The risk premium finances benefits above or below the amount of reserve that would otherwise remain at the next annual valuation:

Πrisk=v∑j∈Jqj(bj−R+).\Pi^{\mathrm{risk}}= v\sum_{j\in J}q_j(b_j-R_+).Πrisk=vj∈J∑​qj​(bj​−R+​).

Since the decrement law satisfies ∑jqj=1−p\sum_jq_j=1-p∑j​qj​=1−p,

Πsav+Πrisk=vR+−R+v∑jqj(bj−R+)=v(pR++∑jqjbj)−R=Π.\begin{aligned} \Pi^{\mathrm{sav}}+\Pi^{\mathrm{risk}} &=vR_+-R+ v\sum_jq_j(b_j-R_+)\\ &=v\left(pR_++\sum_jq_jb_j\right)-R\\ &=\Pi. \end{aligned}Πsav+Πrisk​=vR+​−R+vj∑​qj​(bj​−R+​)=v(pR+​+j∑​qj​bj​)−R=Π.​

Thus the principal premium decomposition is

Π=Πsav+Πrisk.\boxed{\Pi=\Pi^{\mathrm{sav}}+\Pi^{\mathrm{risk}}.}Π=Πsav+Πrisk.​

This follows the savings and risk-premium interpretation of [1, equations (7.5.3)–(7.5.5)]. A negative risk premium is possible algebraically when cause benefits are lower than the continuing reserve. The formal theorem does not assume all monetary amounts are nonnegative.

Boundary cases and formal theorem graph

If p=0p=0p=0, every in-force policy exits during the year, and the continuing reserve term vanishes:

Π=vB−R.\Pi=vB-R.Π=vB−R.

If no decrement can occur, p=1p=1p=1 and qj=0q_j=0qj​=0 for every cause, the required premium reduces to the savings component alone,

Π=Πsav=vR+−R.\Pi=\Pi^{\mathrm{sav}}=vR_+-R.Π=Πsav=vR+​−R.

If every cause of exit pays exactly the same amount as the following-year reserve, bj=R+b_j=R_+bj​=R+​, the risk component is zero. Scaling all monetary benefits and reserve amounts by a common factor scales the premium by that factor.

The draft introduces five definitions: a valid annual decrement law, expected cause benefit, required annual premium, savings premium and risk premium. Eleven supporting theorems establish probability conditions, zero and scaled benefits, reserve balance, zero-survival and no-decrement limits, risk-free exits and the premium decomposition. The capstone combines the one-year reserve balance with the savings/risk identity.

The definitions and theorem types are independent of unconfirmed Prove2Me actuarial declarations from earlier missions. Imports of local definitions are explicitly placed at the beginning of each Lean file, and the proposed statements do not treat a Draft declaration as a published theorem. The proofs of the individual statements remain to be supplied after captain and moderator review.

References

[1] Gerber, Hans U. (1997), Life Insurance Mathematics, third edition, Springer, Chapter 7, Multiple Decrements, §7.5, The Net Premium Reserve, equations (7.5.1)–(7.5.5). In particular (7.5.2) is the annual multiple-decrement recursion and (7.5.3)–(7.5.5) separate the savings and risk portions.

[2] Dickson, David C. M., Hardy, Mary R. and Waters, Howard R. (2009), Actuarial Mathematics for Life Contingent Risks, first edition, Chapter 8, Cambridge University Press, §8.8, Multiple Decrement Models.

[3] Dickson, Hardy and Waters (2009), Chapter 7, Policy Values, annual policy-value recursions. The one-cause formula provides the earlier special case from which the multiple-cause generalisation develops.

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Functional AnalysisNumerical AnalysisOptimization·Captain: mikedeng1

A Forward-Backward Splitting Method for Monotone Inclusions Without Cocoercivity 3: With Linesearch and Locally Lipschitz B the Method Converges to a Zero in Finite DimensionsResearch Paper

Motivation

Many problems in optimization, variational inequalities and saddle-point computation can be written as a monotone inclusion: find xxx with 0∈A(x)+B(x)0 \in A(x) + B(x)0∈A(x)+B(x), where AAA is a set-valued maximally monotone operator (a subdifferential, a normal cone) and BBB is single-valued (a gradient, a skew saddle operator). Splitting methods treat AAA only through its resolvent and BBB only through forward evaluations. The classical forward-backward method needs BBB to be cocoercive, which rules out saddle-point operators; Tseng's forward-backward-forward method removes this but needs two evaluations of BBB per step.

Malitsky and Tam (arXiv:1808.04162, SIAM J. Optim. 30(2), 2020) introduced the forward-reflected-backward method, which needs only monotonicity and Lipschitz continuity of BBB and one new evaluation of BBB per iteration. Its step size in Section 2 depends on a global Lipschitz constant LLL of BBB. Such a constant is often unknown, expensive to estimate, overly conservative, or nonexistent when BBB is only locally Lipschitz. Section 3 of the paper replaces the fixed step by a linesearch (backtracking) and proves convergence for locally Lipschitz BBB in finite dimensions. This mission formalizes that result.

Setting

Let HHH be a finite-dimensional real inner product space. An operator A:H⇉HA : H \rightrightarrows HA:H⇉H is monotone if ⟨x−y,u−v⟩≥0\langle x - y, u - v\rangle \ge 0⟨x−y,u−v⟩≥0 whenever u∈A(x)u \in A(x)u∈A(x), v∈A(y)v \in A(y)v∈A(y), and maximally monotone if moreover its graph is not properly contained in the graph of another monotone operator. For t>0t > 0t>0 the resolvent JtA=(I+tA)−1J_{tA} = (I + tA)^{-1}JtA​=(I+tA)−1 is the map with t−1(w−JtAw)∈A(JtAw)t^{-1}(w - J_{tA}w) \in A(J_{tA}w)t−1(w−JtA​w)∈A(JtA​w) for every www. A map B:H→HB : H \to HB:H→H is monotone if ⟨x−y,B(x)−B(y)⟩≥0\langle x - y, B(x) - B(y)\rangle \ge 0⟨x−y,B(x)−B(y)⟩≥0, and locally Lipschitz if every point has a neighbourhood on which BBB is Lipschitz. The zero set is (A+B)−1(0)={x:−B(x)∈A(x)}(A+B)^{-1}(0) = \{x : -B(x) \in A(x)\}(A+B)−1(0)={x:−B(x)∈A(x)}.

Fix δ∈(0,1)\delta \in (0,1)δ∈(0,1) and σ∈(0,1)\sigma \in (0,1)σ∈(0,1). Given xkx_kxk​, xk−1x_{k-1}xk−1​ and the previous step λk−1\lambda_{k-1}λk−1​, the trial point at step ttt is

xk+1(t)=JtA(xk−tB(xk)−λk−1(B(xk)−B(xk−1))).x_{k+1}(t) = J_{tA}\big(x_k - tB(x_k) - \lambda_{k-1}(B(x_k) - B(x_{k-1}))\big).xk+1​(t)=JtA​(xk​−tB(xk​)−λk−1​(B(xk​)−B(xk−1​))).

Algorithm 1 starts from arbitrary x0,x−1∈Hx_0, x_{-1} \in Hx0​,x−1​∈H and λ−1>0\lambda_{-1} > 0λ−1​>0. In each iteration it chooses ρ∈{1,σ−1}\rho \in \{1, \sigma^{-1}\}ρ∈{1,σ−1}, sets λk=ρλk−1σi\lambda_k = \rho\lambda_{k-1}\sigma^iλk​=ρλk−1​σi with iii the smallest nonnegative integer for which

λk∥B(xk+1)−B(xk)∥≤δ2∥xk+1−xk∥,xk+1=xk+1(λk).(30)\lambda_k \|B(x_{k+1}) - B(x_k)\| \le \frac{\delta}{2}\|x_{k+1} - x_k\|, \qquad x_{k+1} = x_{k+1}(\lambda_k). \tag{30}λk​∥B(xk+1​)−B(xk​)∥≤2δ​∥xk+1​−xk​∥,xk+1​=xk+1​(λk​).(30)

The choice of ρ\rhoρ may change from one iteration to the next; ρ=σ−1\rho = \sigma^{-1}ρ=σ−1 allows the step to grow.

Formalization targets

Goal: Theorem 3.4

If AAA is maximally monotone, BBB is monotone and locally Lipschitz, and (A+B)−1(0)≠∅(A+B)^{-1}(0) \ne \emptyset(A+B)−1(0)=∅, then every sequence generated by Algorithm 1 satisfies

∃ xˉ∈(A+B)−1(0):xk→xˉ.\exists\, \bar x \in (A+B)^{-1}(0): \qquad x_k \to \bar x .∃xˉ∈(A+B)−1(0):xk​→xˉ.

The statement fixes no constant: it holds for every δ,σ∈(0,1)\delta, \sigma \in (0,1)δ,σ∈(0,1), every λ−1>0\lambda_{-1} > 0λ−1​>0, every initial pair and every sequence of choices of ρ\rhoρ.

Milestones

  1. Lemma 3.2 (any real Hilbert space, BBB only locally Lipschitz): at any iteration state, some iii satisfies (30), so the linesearch terminates.
  2. Lemma 3.3: for a zero xxx there is ε>0\varepsilon > 0ε>0 with
∥xk+1−x∥2+2λk⟨B(xk+1)−B(xk),x−xk+1⟩+(12+ε)∥xk+1−xk∥2≤∥xk−x∥2+2λk−1⟨B(xk)−B(xk−1),x−xk⟩+12∥xk−xk−1∥2,\|x_{k+1}-x\|^2+2\lambda_k\langle B(x_{k+1})-B(x_k),x-x_{k+1}\rangle+\big(\tfrac12+\varepsilon\big)\|x_{k+1}-x_k\|^2 \le \|x_k-x\|^2+2\lambda_{k-1}\langle B(x_k)-B(x_{k-1}),x-x_k\rangle+\tfrac12\|x_k-x_{k-1}\|^2,∥xk+1​−x∥2+2λk​⟨B(xk+1​)−B(xk​),x−xk+1​⟩+(21​+ε)∥xk+1​−xk​∥2≤∥xk​−x∥2+2λk−1​⟨B(xk​)−B(xk−1​),x−xk​⟩+21​∥xk​−xk−1​∥2,

stated for k≥1k \ge 1k≥1 (see Formalization scope). 3. The iterates are bounded and ∥xk−xk+1∥→0\|x_k - x_{k+1}\| \to 0∥xk​−xk+1​∥→0. 4. (33): there is L>0L > 0L>0 with ∥B(xk+1)−B(xk)∥≤L∥xk+1−xk∥\|B(x_{k+1}) - B(x_k)\| \le L\|x_{k+1} - x_k\|∥B(xk+1​)−B(xk​)∥≤L∥xk+1​−xk​∥ for all kkk. 5. The step sizes (λk)(\lambda_k)(λk​) are bounded away from zero.

Significance

The theorem makes the forward-reflected-backward method usable without any knowledge of a Lipschitz constant, and extends it to operators that are only locally Lipschitz, such as gradients of C1C^1C1 functions without globally Lipschitz gradient or saddle operators of smooth non-quadratic convex-concave functions. The linesearch costs one resolvent and one evaluation of BBB per trial, and the adaptive factor ρ=σ−1\rho = \sigma^{-1}ρ=σ−1 lets the steps recover after a conservative phase. The same template (an energy inequality where the linesearch test stands in for the Lipschitz bound, followed by a lower bound on the step sizes) recurs in adaptive and backtracking variants of many first-order methods.

The result is proved in the paper; to our knowledge it has no machine-checked proof. The mission produces a formal account of Algorithm 1 including the minimality of the backtracking index, which is where informal accounts of linesearch methods tend to be imprecise. It also records one correction: Lemma 3.3 as printed asserts (32) for all k∈Nk \in \mathbb Nk∈N, but at k=0k = 0k=0 the bound concerns initial data that Algorithm 1 never tests, and it fails there. Theorem 3.4 is unaffected.

Difficulty

Two steps do not transfer directly from the constant-step analysis. First, termination of the linesearch requires the limit behaviour of resolvents as the step tends to zero (JtA(y)→Pdom A‾(y)J_{tA}(y) \to P_{\overline{\mathrm{dom}\,A}}(y)JtA​(y)→PdomA​(y), Bauschke–Combettes, Theorem 23.47), combined with continuity of BBB at the current point; local Lipschitz continuity enters only here and in the last step. Second, the step sizes must be bounded below. The obvious argument combines the accepted test (30) with the Lipschitz bound (33) along the iterates, but (33) concerns accepted points, while a rejected trial step concerns a trial point that is not an iterate. One must show that the rejected trial points also stay in a fixed bounded set, on which BBB is Lipschitz. Finite dimensionality is used exactly to pass from local Lipschitz continuity to Lipschitz continuity on bounded sets.

Formalization scope

HHH is a type with [NormedAddCommGroup H] [InnerProductSpace ℝ H] [FiniteDimensional ℝ H]; it is never specialised to EuclideanSpace ℝ (Fin n). The operator vocabulary (monotone, maximally monotone, resolvent) is the published module ThreeOpSplitting.Accel.MonotoneOperators; local Lipschitz continuity is Mathlib's LocallyLipschitz. Conventions committed to:

  • Resolvent as hypothesis. The resolvent is a family J : ℝ → H → H with IsResolventFamily A J; for maximally monotone AAA it exists (Minty) and is unique on t>0t > 0t>0. The goal keeps maximal monotonicity of AAA as well.
  • Index shift. Lean's x j is xj−1x_{j-1}xj−1​ and lam j is λj−1\lambda_{j-1}λj−1​, so lam 0 =λ−1=\lambda_{-1}=λ−1​. Algorithm 1's initialization also names a λ0\lambda_0λ0​ that the iteration never uses; it is not a parameter.
  • Run predicate. IsLinesearchRun J B δ σ lam x requires at every iteration some ρ∈{1,σ−1}\rho \in \{1, \sigma^{-1}\}ρ∈{1,σ−1} and an index iii such that λk=ρλk−1σi\lambda_k = \rho\lambda_{k-1}\sigma^iλk​=ρλk−1​σi, xk+1x_{k+1}xk+1​ is the trial point at λk\lambda_kλk​, (30) holds, and (30) fails at every smaller index. Every sequence of ρ\rhoρ choices is admitted.
  • Mode of convergence. Norm convergence, Filter.Tendsto x atTop (nhds xs).
  • Lemma 3.3 for k≥1k \ge 1k≥1. A disclosed correction of the printed "for all k∈Nk \in \mathbb Nk∈N".
  • Hypothesis relaxations in milestones. Lemma 3.3 uses only monotonicity of AAA and no completeness; the boundedness milestone drops finite dimensionality. Both are stronger than the page.

Trivializing encodings are ruled out: the resolvent is tied to AAA by IsResolventFamily rather than left free; the minimality clause prevents arbitrarily small accepted steps; ρ\rhoρ is not fixed; convergence is in norm, not weak; and a global Lipschitz hypothesis on BBB, which would reduce the goal to mission 1 of this series in finite dimension, is not assumed. The hypotheses are satisfiable (a sanity file checks A≡{0}A \equiv \{0\}A≡{0}, J=idJ = \mathrm{id}J=id, B=0B = 0B=0).

A complete development needs: nonexpansiveness and continuity in the step of resolvents of maximally monotone operators, including the small-step limit to the projection onto dom A‾\overline{\mathrm{dom}\,A}domA; Lipschitz continuity on compact sets of locally Lipschitz maps; the telescoping argument of Theorem 2.5; and a finite-dimensional closedness argument for the graph of A+BA + BA+B. The resolvent facts are reusable well beyond this mission. Proofs of individual milestones, and of the resolvent lemmas as separate items, are welcome.

Selected references

  • Y. Malitsky, M. K. Tam, A Forward-Backward Splitting Method for Monotone Inclusions Without Cocoercivity, SIAM J. Optim. 30(2):1451–1472, 2020. arXiv:1808.04162v4, doi:10.1137/18M1207260
  • H. H. Bauschke, P. L. Combettes, Convex Analysis and Monotone Operator Theory in Hilbert Spaces, 2nd ed., Springer, 2017. doi:10.1007/978-3-319-48311-5
  • P. Tseng, A modified forward-backward splitting method for maximal monotone mappings, SIAM J. Control Optim. 38(2):431–446, 2000. doi:10.1137/S0363012998338806
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Linear OptimizationOperations ResearchOptimization·Captain: mikedeng1

Production Scheduling for Strategic Open Pit Mine Planning: A Mixed-Integer Programming Approach 3: Variable-Right-Hand-Side Production Cuts along a Precedence Chain Are ValidResearch Paper

Motivation

Strategic open pit mine planning decides which parts of an ore body are excavated, in which period, and where each block of material is sent: to a processing plant, a stockpile or a waste dump. Rivera Letelier, Espinoza, Goycoolea, Moreno and Muñoz (Operations Research 68(5), 2020) state the problem as a mixed-integer program, the precedence-constrained production scheduling problem with clusters (PCPSP-C), which extends the formulation of Bienstock and Zuckerberg (IPCO 2010) to clusters of blocks that are extracted together. The integer versions of this program have large integrality gaps on production scheduling instances (§5, p. 1432), so the authors derive problem-specific cutting planes. This mission concerns the variable-right-hand-side (VRHS) production cuts of §5.2. They combine the precedence order of the clusters with the capacity of a single destination: if a solution sends many blocks to a capacitated destination, the predecessors of those blocks must be fully extracted.

The VRHS cuts are introduced first on a one-period, two-destination set, the mode-knapsack set MK (§5.2.1), and then generalised to the full multi-period clustered model (§5.2.2). Disaggregated formulations with destination choices go back to Boland et al. (Comput. Oper. Res. 2009); cutting planes for the precedence-constrained knapsack structure of open pit scheduling were studied by Bley et al. (Comput. Oper. Res. 2010).

All page references are journal pages of the published Operations Research article.

Setting

An instance has finite sets B\mathcal BB of blocks, D\mathcal DD of destinations and C\mathcal CC of clusters, the latter a partition of B\mathcal BB, and periods T={1,…,T}\mathcal T=\{1,\dots,T\}T={1,…,T}. Block bbb lies in cluster c(b)c(b)c(b) and has weight qb≥0q_b\ge 0qb​≥0. A precedence relation b1≺b2b_1\prec b_2b1​≺b2​ on blocks induces one on clusters (c1≺c2c_1\prec c_2c1​≺c2​ if some block of c1c_1c1​ precedes some block of c2c_2c2​), assumed to be a strict partial order. The arc set A\mathcal AA is its transitive reduction: (c,c′)∈A(c,c')\in\mathcal A(c,c′)∈A when c′c'c′ is an immediate predecessor of ccc. The reverse closure of a cluster is rcl(c)={c}∪{c′:c≺c′}rcl(c)=\{c\}\cup\{c':c\prec c'\}rcl(c)={c}∪{c′:c≺c′}, the cluster and everything that requires it; for a set SSS of clusters, q(S)=∑c∈S∑b∈cqbq(S)=\sum_{c\in S}\sum_{b\in c}q_bq(S)=∑c∈S​∑b∈c​qb​.

Variables xc,tx_{c,t}xc,t​ give the fraction of cluster ccc extracted in period ttt, and yb,d,ty_{b,d,t}yb,d,t​ the fraction of block bbb sent to destination ddd in period ttt. The constraints (2)–(7) of p. 1427 are

xc(b),t=∑dyb,d,t,∑txc,t≤1,∑t′≤txc,t′≤∑t′≤txc′,t′  ((c,c′)∈A),Gy≤g,y≥0,x_{c(b),t}=\sum_{d}y_{b,d,t},\qquad \sum_{t}x_{c,t}\le 1,\qquad \sum_{t'\le t}x_{c,t'}\le\sum_{t'\le t}x_{c',t'}\ \ ((c,c')\in\mathcal A),\qquad Gy\le g,\qquad y\ge 0,xc(b),t​=d∑​yb,d,t​,t∑​xc,t​≤1,t′≤t∑​xc,t′​≤t′≤t∑​xc′,t′​  ((c,c′)∈A),Gy≤g,y≥0,

together with an integrality condition: full integrality (10), xc,t∈{0,1}x_{c,t}\in\{0,1\}xc,t​∈{0,1}, defines the PCPSP-F, and partial integrality (11), "∑t′≤txc,t′>0\sum_{t'\le t}x_{c,t'}>0∑t′≤t​xc,t′​>0 implies ∑t′≤txc′,t′=1\sum_{t'\le t}x_{c',t'}=1∑t′≤t​xc′,t′​=1 for (c,c′)∈A(c,c')\in\mathcal A(c,c′)∈A", defines the PCPSP-P. The general rows Gy≤gGy\le gGy≤g include the destination capacity rows (9), ∑bqb yb,d,t≤Utd\sum_b q_b\,y_{b,d,t}\le U^d_t∑b​qb​yb,d,t​≤Utd​. The cuts use the cumulative variables wc,t=∑t′=1txc,t′w_{c,t}=\sum_{t'=1}^{t}x_{c,t'}wc,t​=∑t′=1t​xc,t′​ (17).

The mode-knapsack set MK (p. 1433) fixes a DAG G=(B,A)G=(\mathcal B,\mathcal A)G=(B,A), weights qb>0q_b>0qb​>0 and a capacity U>0U>0U>0, and consists of the vectors (x,yP,yW)(x,y^P,y^W)(x,yP,yW) with

∑bqbybP≤U,ybP+ybW=xb,xb≤1,xb>0⇒xb′=1 ((b,b′)∈A),yP,yW≥0.\sum_b q_b y^P_b\le U,\qquad y^P_b+y^W_b=x_b,\qquad x_b\le 1,\qquad x_b>0\Rightarrow x_{b'}=1\ ((b,b')\in\mathcal A),\qquad y^P,y^W\ge 0.b∑​qb​ybP​≤U,ybP​+ybW​=xb​,xb​≤1,xb​>0⇒xb′​=1 ((b,b′)∈A),yP,yW≥0.

Formalization targets

Goal: Theorem 7 (VRHS cuts), p. 1434

Fix d∈Dd\in\mathcal Dd∈D, t∈Tt\in\mathcal Tt∈T and clusters c1≺c2≺⋯≺cnc_1\prec c_2\prec\dots\prec c_nc1​≺c2​≺⋯≺cn​ with q(rcl(c1)∖rcl(cn))<Utd<q(rcl(c1))q(rcl(c_1)\setminus rcl(c_n))<U^d_t<q(rcl(c_1))q(rcl(c1​)∖rcl(cn​))<Utd​<q(rcl(c1​)). Let Δk=rcl(ck)∖rcl(ck+1)\Delta_k=rcl(c_k)\setminus rcl(c_{k+1})Δk​=rcl(ck​)∖rcl(ck+1​), δk=q(Δk)\delta_k=q(\Delta_k)δk​=q(Δk​) for k<nk<nk<n, and Δn=rcl(cn)\Delta_n=rcl(c_n)Δn​=rcl(cn​), δn=Utd−q(rcl(c1)∖rcl(cn))\delta_n=U^d_t-q(rcl(c_1)\setminus rcl(c_n))δn​=Utd​−q(rcl(c1​)∖rcl(cn​)). For constants 0≤αb≤10\le\alpha_b\le 10≤αb​≤1 (b∈cnb\in c_nb∈cn​), the inequality

∑k=1n−1∑c∈Δk∑b∈cqbyb,d,t+∑b∈cnαbqbyb,d,t+∑c∈rcl(cn)∖{cn}∑b∈cqbyb,d,t≤∑k=1nδkwck,t(32)\sum_{k=1}^{n-1}\sum_{c\in\Delta_k}\sum_{b\in c}q_b y_{b,d,t}+\sum_{b\in c_n}\alpha_b q_b y_{b,d,t}+\sum_{c\in rcl(c_n)\setminus\{c_n\}}\sum_{b\in c}q_b y_{b,d,t}\le\sum_{k=1}^{n}\delta_k w_{c_k,t}\tag{32}k=1∑n−1​c∈Δk​∑​b∈c∑​qb​yb,d,t​+b∈cn​∑​αb​qb​yb,d,t​+c∈rcl(cn​)∖{cn​}∑​b∈c∑​qb​yb,d,t​≤k=1∑n​δk​wck​,t​(32)

is valid for the PCPSP-F, and, when ∑b∈cnαbqb≤Utd−q(rcl(c1)∖rcl(cn))\sum_{b\in c_n}\alpha_b q_b\le U^d_t-q(rcl(c_1)\setminus rcl(c_n))∑b∈cn​​αb​qb​≤Utd​−q(rcl(c1​)∖rcl(cn​)) (33), for the PCPSP-P. The goal is the conjunction of the two validity claims.

Milestones

  • (29)–(30), p. 1434: under either integrality condition, wc,t<1w_{c,t}<1wc,t​<1 implies yb,d,t=0y_{b,d,t}=0yb,d,t​=0 for every block of a cluster in rcl(c)∖{c}rcl(c)\setminus\{c\}rcl(c)∖{c}, and yb,d,t≤wc(b),ty_{b,d,t}\le w_{c(b),t}yb,d,t​≤wc(b),t​. The third condition (31) of the page is the capacity row (9) itself.
  • (35), p. 1435: ∑c∈Δk∑b∈cqbyb,d,t≤δkwck,t\sum_{c\in\Delta_k}\sum_{b\in c}q_b y_{b,d,t}\le\delta_k w_{c_k,t}∑c∈Δk​​∑b∈c​qb​yb,d,t​≤δk​wck​,t​ for k=1,…,n−1k=1,\dots,n-1k=1,…,n−1.
  • (36), p. 1435: under (33), ∑b∈cnαbqbyb,d,t≤δnwcn,t\sum_{b\in c_n}\alpha_b q_b y_{b,d,t}\le\delta_n w_{c_n,t}∑b∈cn​​αb​qb​yb,d,t​≤δn​wcn​,t​.
  • Theorem 5, p. 1434: in MK, every block bbb with qb≤Uq_b\le Uqb​≤U gives the valid inequality ∑b′∈rcl(b)qb′yb′P≤Uxb\sum_{b'\in rcl(b)}q_{b'}y^P_{b'}\le U x_b∑b′∈rcl(b)​qb′​yb′P​≤Uxb​.

Significance

A valid inequality removes fractional points of the linear relaxation while keeping every feasible schedule. The VRHS cuts are among the production cuts that the paper evaluates in its computational study (§8), alongside the extraction cuts and the hourglass cuts. Their right-hand side is not a constant but a combination of extraction variables along a chain, which is what lets them couple the destination capacity with the precedence order; the paper's Theorem 5 shows the mechanism on MK, Theorem 7 in the full model. The partial integrality regime, under which the second half of Theorem 7 holds, is the one used by commercial mine planning software (p. 1427).

The results are proved in the paper by case analysis on the first index kkk with wck,t<1w_{c_k,t}<1wck​,t​<1. None of them has a machine-checked proof. Formalizing them makes explicit which rows of the formulation each cut uses (the destination capacity (9) and the integrality condition), and what role the coefficient condition (33) plays in the partially integral case.

Difficulty

The proof uses that Δ1,…,Δn−1\Delta_1,\dots,\Delta_{n-1}Δ1​,…,Δn−1​ partition rcl(c1)∖rcl(cn)rcl(c_1)\setminus rcl(c_n)rcl(c1​)∖rcl(cn​) and are disjoint from rcl(cn)rcl(c_n)rcl(cn​), which requires rcl(ck+1)⊆rcl(ck)rcl(c_{k+1})\subseteq rcl(c_k)rcl(ck+1​)⊆rcl(ck​) along the chain. It uses that wc,t≤wck,tw_{c,t}\le w_{c_k,t}wc,t​≤wck​,t​ for every c∈rcl(ck)c\in rcl(c_k)c∈rcl(ck​), and that wc,t<1w_{c,t}<1wc,t​<1 forces all strict successors of ccc to be unextracted; both chain the constraints (4) and (11) along covering arcs of a finite strict order, since the formulation constrains only the arcs of A\mathcal AA, not all of ≺\prec≺. A natural first attempt, arguing directly from ≺\prec≺, therefore does not apply. The counting step needs x≥0x\ge 0x≥0, which is not a constraint of the formulation but follows from xc(b),t=∑dyb,d,tx_{c(b),t}=\sum_d y_{b,d,t}xc(b),t​=∑d​yb,d,t​, y≥0y\ge 0y≥0 and the nonemptiness of clusters. In the partial integrality case a fractional wcn,tw_{c_n,t}wcn​,t​ is possible, and the bound on the cnc_ncn​ term must come from (33) rather than from integrality.

Formalization scope

Blocks, destinations and clusters are finite types; periods are Fin T, index ttt standing for period t+1t+1t+1. An instance carries the block-to-cluster map, the block precedence, values, discount rate, weights, capacities and mmm side rows Gy≤gGy\le gGy≤g. Cluster precedence is derived from block precedence; A\mathcal AA is its covering relation, and constraints (4) and (11) range over A\mathcal AA only. The chain c1,…,cnc_1,\dots,c_nc1​,…,cn​ is a function on N\mathbb NN read at 1,…,n1,\dots,n1,…,n with n≥1n\ge 1n≥1, and condition 1 of Theorem 7 is stated for consecutive pairs. In (32), yyy is taken at the single period ttt and www is cumulative.

The standing assumptions of §2.1 are hypotheses of every PCPSP-C statement: clusters cover B\mathcal BB (so each is nonempty), ≺\prec≺ is a strict partial order on clusters, r>0r>0r>0, and qb≥0q_b\ge 0qb​≥0. A cut "valid for the PCPSP-F (PCPSP-P)" is stated as: at every point feasible for the formulation with full (partial) integrality whose destination capacity rows (9) hold, the inequality holds. The capacity rows enter as an explicit hypothesis because the paper assumes they are among the rows of Gy≤gGy\le gGy≤g; without them the cut is false. Validity is never asserted for the LP relaxation, where (29) and (32) fail, so the integrality condition cannot be dropped. Conditions 2 and 3 of Theorem 7 are kept as on the page, although the proof does not use condition 3. In MK, the DAG property, q>0q>0q>0 and U>0U>0U>0 are hypotheses; an arc (b,b′)(b,b')(b,b′) means that extracting bbb forces b′b'b′, and rcl(b)rcl(b)rcl(b) collects bbb and the blocks from which bbb is reachable.

The development needs only finite sums, finite sets and orders from Mathlib. Contributions are welcome on the chaining lemma for covering relations of finite strict orders, on the nonnegativity and monotonicity of www, and on the partition {Δk}\{\Delta_k\}{Δk​} of rcl(c1)∖rcl(cn)rcl(c_1)\setminus rcl(c_n)rcl(c1​)∖rcl(cn​), which the goal and the milestones share.

Selected references

  • O. Rivera Letelier, D. Espinoza, M. Goycoolea, E. Moreno, G. Muñoz, Production Scheduling for Strategic Open Pit Mine Planning: A Mixed-Integer Programming Approach, Operations Research 68(5):1425–1444, 2020. https://doi.org/10.1287/opre.2019.1965
  • D. Bienstock, M. Zuckerberg, Solving LP Relaxations of Large-Scale Precedence Constrained Problems, Proc. 14th IPCO, LNCS 6080, 1–14, 2010. https://doi.org/10.1007/978-3-642-13036-6_1
  • N. Boland, I. Dumitrescu, G. Froyland, A. M. Gleixner, LP-based disaggregation approaches to solving the open pit mining production scheduling problem with block processing selectivity, Computers & Operations Research 36(4):1064–1089, 2009. https://doi.org/10.1016/j.cor.2007.12.006
  • A. Bley, N. Boland, C. Fricke, G. Froyland, A strengthened formulation and cutting planes for the open pit mine production scheduling problem, Computers & Operations Research 37(9):1641–1647, 2010. https://doi.org/10.1016/j.cor.2009.12.008
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Functional AnalysisNumerical AnalysisOptimization·Captain: mikedeng1

A Forward-Backward Splitting Method for Monotone Inclusions Without Cocoercivity 1: The Forward-Reflected-Backward Method Converges Weakly to a Zero of A + BResearch Paper

Monotone inclusions and the cost of splitting

Many problems in convex optimization, variational inequalities and saddle-point computation can be written as a monotone inclusion: find xxx in a real Hilbert space HHH with

0∈(A+B)(x),0 \in (A+B)(x),0∈(A+B)(x),

where AAA is a set-valued maximally monotone operator (a subdifferential, a normal cone, a constraint) and BBB is a single-valued monotone operator (a gradient, or the skew operator of a saddle-point problem). Splitting methods solve such problems using AAA and BBB separately: a backward step evaluates the resolvent JλA=(I+λA)−1J_{\lambda A}=(I+\lambda A)^{-1}JλA​=(I+λA)−1, and a forward step evaluates BBB.

The classical forward-backward method xk+1=JλA(xk−λB(xk))x_{k+1}=J_{\lambda A}(x_k-\lambda B(x_k))xk+1​=JλA​(xk​−λB(xk​)) converges when BBB is cocoercive, but can fail when BBB is merely monotone and Lipschitz, which is the case for saddle-point operators such as B(z1,z2)=(z2,−z1)B(z_1,z_2)=(z_2,-z_1)B(z1​,z2​)=(z2​,−z1​). Tseng's forward-backward-forward method (Tseng 2000) removes the cocoercivity assumption at the price of two evaluations of BBB per iteration. Malitsky and Tam (arXiv:1808.04162; SIAM J. Optim. 30(2), 2020) propose the forward-reflected-backward method, which needs one evaluation of BBB and one resolvent of AAA per iteration, reusing the previous value of BBB.

Timeline of the relevant results:

  • 1967: Opial's lemma on weak convergence of sequences in Hilbert space (Opial 1967).
  • 1979: Lions and Mercier analyse forward-backward splitting with cocoercive BBB (Lions–Mercier 1979).
  • 1980: Popov's modified Arrow–Hurwicz method for saddle points, with one operator evaluation per step (Popov 1980).
  • 2000: Tseng's forward-backward-forward method for monotone and Lipschitz BBB.
  • 2015: Malitsky's projected reflected gradient method for variational inequalities (Malitsky 2015), the special case A=NCA=N_CA=NC​, BBB affine.
  • 2018–2020: Malitsky and Tam, the forward-reflected-backward method, Theorem 2.5.

Setting

HHH is a real Hilbert space with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩. A set-valued operator A:H⇉HA:H\rightrightarrows HA:H⇉H is monotone if ⟨x−y,u−v⟩≥0\langle x-y,u-v\rangle\ge 0⟨x−y,u−v⟩≥0 whenever u∈A(x)u\in A(x)u∈A(x), v∈A(y)v\in A(y)v∈A(y), and maximally monotone if its graph is not properly contained in the graph of another monotone operator. Its resolvent JλA=(I+λA)−1J_{\lambda A}=(I+\lambda A)^{-1}JλA​=(I+λA)−1 is, for λ>0\lambda>0λ>0 and AAA maximally monotone, an everywhere defined single-valued map, characterised by λ−1(w−JλAw)∈A(JλAw)\lambda^{-1}(w-J_{\lambda A}w)\in A(J_{\lambda A}w)λ−1(w−JλA​w)∈A(JλA​w). A map B:H→HB:H\to HB:H→H is LLL-Lipschitz if ∥B(x)−B(y)∥≤L∥x−y∥\|B(x)-B(y)\|\le L\|x-y\|∥B(x)−B(y)∥≤L∥x−y∥, and monotone if ⟨x−y,B(x)−B(y)⟩≥0\langle x-y,B(x)-B(y)\rangle\ge0⟨x−y,B(x)−B(y)⟩≥0.

The zero set is (A+B)−1(0)={x:−B(x)∈A(x)}(A+B)^{-1}(0)=\{x : -B(x)\in A(x)\}(A+B)−1(0)={x:−B(x)∈A(x)}. Given initial points x0,x−1∈Hx_0,x_{-1}\in Hx0​,x−1​∈H and step sizes (λk)k≥−1(\lambda_k)_{k\ge-1}(λk​)k≥−1​, the forward-reflected-backward method is

xk+1=JλkA(xk−λkB(xk)−λk−1(B(xk)−B(xk−1)))∀k∈N.(13)x_{k+1}=J_{\lambda_k A}\big(x_k-\lambda_k B(x_k)-\lambda_{k-1}(B(x_k)-B(x_{k-1}))\big)\qquad\forall k\in\mathbb N. \tag{13}xk+1​=Jλk​A​(xk​−λk​B(xk​)−λk−1​(B(xk​)−B(xk−1​)))∀k∈N.(13)

A sequence (xk)(x_k)(xk​) converges weakly to xˉ\bar xxˉ if ⟨xk,v⟩→⟨xˉ,v⟩\langle x_k,v\rangle\to\langle\bar x,v\rangle⟨xk​,v⟩→⟨xˉ,v⟩ for every v∈Hv\in Hv∈H; a sequential weak cluster point is the weak limit of a subsequence.

Formalization targets

Goal: Theorem 2.5 (p. 6)

If AAA is maximally monotone, BBB is monotone and LLL-Lipschitz, (A+B)−1(0)≠∅(A+B)^{-1}(0)\ne\varnothing(A+B)−1(0)=∅, and (λk)⊆[ε,1−2ε2L](\lambda_k)\subseteq[\varepsilon,\tfrac{1-2\varepsilon}{2L}](λk​)⊆[ε,2L1−2ε​] for some ε>0\varepsilon>0ε>0, then every sequence generated by (13) satisfies

xk⇀xˉfor some xˉ∈(A+B)−1(0).x_k\rightharpoonup\bar x\quad\text{for some }\bar x\in(A+B)^{-1}(0).xk​⇀xˉfor some xˉ∈(A+B)−1(0).

Milestones

In attack order:

  1. Proposition 2.3, the basic inequality (19) for one resolvent step.
  2. Lemma 2.4, the energy inequality (20).
  3. The telescoped bound after (24).
  4. Boundedness of (xk)(x_k)(xk​) and ∥xk−xk+1∥→0\|x_k-x_{k+1}\|\to0∥xk​−xk+1​∥→0.
  5. Weak cluster points lie in the zero set.
  6. Convergence of the energy (26).
  7. Its limit equals lim⁡∥xk−xˉ∥2\lim\|x_k-\bar x\|^2lim∥xk​−xˉ∥2.
  8. Lemma 2.2, an Opial-type criterion for weak convergence.

Corollary 2.6, the constant-step case λ∈(0,12L)\lambda\in(0,\tfrac1{2L})λ∈(0,2L1​), is included as a companion theorem.

Significance

Theorem 2.5 shows that monotone inclusions with a Lipschitz, non-cocoercive single-valued part can be solved by a splitting method with the per-iteration cost of forward-backward splitting: one forward and one backward evaluation. For saddle-point problems, where each evaluation of BBB is a pair of matrix–vector products, this halves the operator cost of Tseng's method. The method contains the projected reflected gradient method and, for A=0A=0A=0, Popov's method and the optimistic gradient method used in training generative adversarial networks (Remark 2.1). The analysis of this section is reused for the linear rate, the linesearch, the inertial variant and the three-operator variant of later sections (missions 2–5 of this series).

The theorem is proved in the paper. Formalizing it requires a machine-checked Opial-type lemma and a machine-checked demiclosedness argument for maximally monotone operators perturbed by a continuous monotone map, both reusable well beyond this mission. To our knowledge no machine-checked proof of convergence of the forward-reflected-backward method exists.

Difficulty

The energy inequality of Lemma 2.4 is algebra plus monotonicity and the Lipschitz estimate, and it yields boundedness and ∥xk+1−xk∥→0\|x_{k+1}-x_k\|\to0∥xk+1​−xk​∥→0. The difficulty lies in passing from these facts to weak convergence of the whole sequence. Norm convergence is false in general, so a Cauchy-sequence argument is unavailable. The energy is not Fejér monotone in ∥xk−x∥\|x_k-x\|∥xk​−x∥ alone, because of the cross term 2λk−1⟨B(xk)−B(xk−1),x−xk⟩2\lambda_{k-1}\langle B(x_k)-B(x_{k-1}),x-x_k\rangle2λk−1​⟨B(xk​)−B(xk−1​),x−xk​⟩, so the standard Fejér/Opial lemma does not apply directly. Identifying weak cluster points as zeros requires the weak-strong closedness of the graph of A+BA+BA+B, which in turn rests on maximal monotonicity of the sum: this is not a consequence of monotonicity of the two parts, and the inclusion (25) can be passed to the limit only because the step sizes stay above ε\varepsilonε.

Formalization scope

The Lean development uses a real inner product space H (InnerProductSpace ℝ H), complete wherever the page needs it, and the published operator vocabulary ThreeOpSplitting.Accel.MonotoneOperators (monotone and maximally monotone set-valued operators, monotone and Lipschitz single-valued maps, resolvents). Conventions:

  • Resolvents are hypotheses. The iteration is driven by a family J:R→H→HJ:\mathbb R\to H\to HJ:R→H→H with γ−1(w−J(γ)w)∈A(J(γ)w)\gamma^{-1}(w-J(\gamma)w)\in A(J(\gamma)w)γ−1(w−J(γ)w)∈A(J(γ)w) for all γ>0\gamma>0γ>0, w∈Hw\in Hw∈H; for maximally monotone AAA such a family exists and is unique. The goal keeps maximal monotonicity of AAA as a hypothesis as well.
  • Index shift. Lean's x j is xj−1x_{j-1}xj−1​ and lam j is λj−1\lambda_{j-1}λj−1​; the initial points are arbitrary.
  • Step range. Every λj\lambda_jλj​, j≥−1j\ge-1j≥−1, lies in [ε,(1−2ε)/(2L)][\varepsilon,(1-2\varepsilon)/(2L)][ε,(1−2ε)/(2L)], including λ−1\lambda_{-1}λ−1​ as on p. 4. L>0L>0L>0 is assumed, since the range divides by LLL.
  • Weak convergence is convergence of ⟨xk,v⟩\langle x_k,v\rangle⟨xk​,v⟩ for every vvv; cluster points are sequential weak cluster points (subsequences along strictly increasing index maps).
  • Several milestones are stated in a stronger form than the page, with AAA only monotone, HHH not complete, or a conclusion for every zero rather than the cluster point. Each item's note says which.

Three formalizations would trivialize the goal and are excluded:

  • an unconstrained resolvent map;
  • norm convergence or convergence of a subsequence in place of weak convergence of the whole sequence;
  • a step range shrunk or pinned to a constant.

A complete development needs the Opial-type Lemma 2.2, which in turn needs weak sequential compactness of bounded sets in Hilbert space, and maximal monotonicity of A+BA+BA+B for continuous monotone BBB (Bauschke–Combettes, Corollaries 20.25 and 24.4(i)) with its demiclosedness (Proposition 20.33). These are general results of monotone operator theory, and contributions of them as separate theorems are welcome.

Selected references

  • Y. Malitsky and M. K. Tam, A Forward-Backward Splitting Method for Monotone Inclusions Without Cocoercivity, SIAM J. Optim. 30(2), 2020; arXiv:1808.04162v4. https://arxiv.org/abs/1808.04162v4 (DOI https://doi.org/10.1137/18M1207260)
  • H. H. Bauschke and P. L. Combettes, Convex Analysis and Monotone Operator Theory in Hilbert Spaces, 2nd ed., Springer, 2017. https://doi.org/10.1007/978-3-319-48311-5
  • P. Tseng, A modified forward-backward splitting method for maximal monotone mappings, SIAM J. Control Optim. 38(2), 2000. https://doi.org/10.1137/S0363012998338806
  • Y. Malitsky, Projected reflected gradient methods for monotone variational inequalities, SIAM J. Optim. 25(1), 2015. https://doi.org/10.1137/14097238X
  • L. D. Popov, A modification of the Arrow–Hurwicz method for search of saddle points, Math. Notes 28, 1980. https://doi.org/10.1007/BF01141092
  • P.-L. Lions and B. Mercier, Splitting algorithms for the sum of two nonlinear operators, SIAM J. Numer. Anal. 16(6), 1979. https://doi.org/10.1137/0716071
  • Z. Opial, Weak convergence of the sequence of successive approximations for nonexpansive mappings, Bull. Amer. Math. Soc. 73, 1967. https://doi.org/10.1090/S0002-9904-1967-11761-0
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Three Conjectures in Extremal Spectral Graph Theory 2: For Large n, K₂ + Pₙ₋₂ Is the Unique Planar Graph on n Vertices of Maximum Spectral Radius (Boots–Royle / Cao–Vince Conjecture)Research Paper

Motivation

The spectral radius of a graph, the largest eigenvalue of its adjacency matrix, measures how densely and how unevenly the edges of the graph are distributed. Asking which graph in a class maximizes it is a spectral analogue of the extremal question "which graph in the class has the most edges". For planar graphs the question has a long history in spectral graph theory, going back at least to Schwenk and Wilson. It also arose in geography, where the spectral radius serves as a measure of the connectivity of planar networks. To compare real networks with a theoretical upper bound, geographers wanted the planar graph of maximum spectral radius (arXiv:1606.01916v2, p. 3).

Timeline, as recorded by Tait and Tobin (pp. 1–3):

  • 1978, Schwenk and Wilson: early study of the eigenvalues of planar graphs.
  • 1991, Boots and Royle, and independently 1993, Cao and Vince: conjecture that the planar graph on n≥9n \ge 9n≥9 vertices of maximum spectral radius is P2+Pn−2P_2 + P_{n-2}P2​+Pn−2​ (Conjecture 1 of the paper). The conjecture is false for n∈{7,8}n \in \{7, 8\}n∈{7,8}, so some lower bound on nnn is necessary (p. 2).
  • 1988–2000: successive improvements of the upper bound on the spectral radius of planar graphs, by Hong (1988, 1995, 1998), Cao and Vince (1993), Guiduli (1996) and Ellingham and Zha (2000). These bounds do not identify the extremal graph.
  • 2010, Dvořák and Mohar: an upper bound on the spectral radius of planar graphs of given maximum degree.
  • Guiduli and Hayes were reported by Ellingham and Zha to have proved the conjecture for large nnn. The preprint never appeared (p. 3).
  • 2017, Tait and Tobin: proof of the conjecture for all sufficiently large nnn (Theorem 15).

Setting

All graphs are finite and simple. A graph on nnn vertices has vertex set {0,1,…,n−1}\{0, 1, \dots, n-1\}{0,1,…,n−1}. Its adjacency matrix A(G)A(G)A(G) is the n×nn \times nn×n real matrix with entry 111 in position (u,w)(u, w)(u,w) when u∼wu \sim wu∼w and 000 otherwise. Its eigenvalues are real, and the largest is the spectral radius λ1(G)\lambda_1(G)λ1​(G).

A graph is planar if it can be drawn in the plane with vertices as distinct points and edges as simple arcs joining their ends, such that an arc meets no vertex other than its ends and two arcs meet only at common ends.

For graphs GGG and HHH on disjoint vertex sets, the join G+HG + HG+H is the graph on the union of the two vertex sets that keeps every edge of GGG and of HHH and adds every edge between a vertex of GGG and a vertex of HHH. Write K2K_2K2​ for a single edge, PmP_mPm​ for the path on mmm vertices, and K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​ for their join: two adjacent vertices, both joined to every vertex of a path on the remaining n−2n - 2n−2 vertices. The paper also writes it P2+Pn−2P_2 + P_{n-2}P2​+Pn−2​.

A planar graph GGG on nnn vertices is a planar spectral maximizer if λ1(G′)≤λ1(G)\lambda_1(G') \le \lambda_1(G)λ1​(G′)≤λ1​(G) for every planar graph G′G'G′ on the same nnn vertices.

The milestones refer to a leading eigenvector v\mathbf vv of a maximizer, scaled so that every entry is positive and the largest entry is 111, and to a vertex xxx with vx=1\mathbf v_x = 1vx​=1. For a parameter ε>0\varepsilon > 0ε>0 they use the sets L={z:vz>ε}L = \{z : \mathbf v_z > \varepsilon\}L={z:vz​>ε} and S=V(G)∖LS = V(G) \setminus LS=V(G)∖L, the edge counts e(X)e(X)e(X) (edges inside XXX) and e(X,Y)e(X, Y)e(X,Y) (edges between XXX and YYY), and a second vertex www with vw>1−24ε\mathbf v_w > 1 - 24\varepsilonvw​>1−24ε that is adjacent to all but 94εn94\varepsilon n94εn vertices of SSS.

Formalization targets

Goal: Theorem 15

∃N0 ∀n≥N0 ∀G on n vertices:G is a planar spectral maximizer  ⟺  G≅K2+Pn−2.\exists N_0\ \forall n \ge N_0\ \forall G \text{ on } n \text{ vertices}: \quad G \text{ is a planar spectral maximizer} \iff G \cong K_2 + P_{n-2}.∃N0​ ∀n≥N0​ ∀G on n vertices:G is a planar spectral maximizer⟺G≅K2​+Pn−2​.

The threshold N0N_0N0​ is not fixed. The paper proves the statement only for nnn beyond an unspecified bound, and the conjecture's bound n≥9n \ge 9n≥9 remains open. The equivalence encodes "the unique maximizer is K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​": every maximizer is isomorphic to it, and it is itself a maximizer.

Milestones, in the order of the proof

  1. If HHH is a proper spanning subgraph of a connected graph GGG, then λ1(H)<λ1(G)\lambda_1(H) < \lambda_1(G)λ1​(H)<λ1​(G) (§1.2, already proved on the platform).
  2. A planar graph on n≥3n \ge 3n≥3 vertices has no K3,3K_{3,3}K3,3​ subgraph and at most 3n−63n - 63n−6 edges, and each of its bipartite subgraphs has at most 2n−42n - 42n−4 edges (p. 8).
  3. Lemma 8: 2n−4<λ1<6n\sqrt{2n-4} < \lambda_1 < \sqrt{6n}2n−4​<λ1​<6n​.
  4. The counts ∣L∣≤32n−4/ε|L| \le 3\sqrt{2n-4}/\varepsilon∣L∣≤32n−4​/ε, e(S,L)≤2n−4e(S, L) \le 2n - 4e(S,L)≤2n−4, e(S)≤3n−6e(S) \le 3n - 6e(S)≤3n−6, e(L)≤92n−4/εe(L) \le 9\sqrt{2n-4}/\varepsilone(L)≤92n−4​/ε (p. 8).
  5. Lemma 9: ∑z∈Lvz≤ε2n−4+18/ε\sum_{z \in L} \mathbf v_z \le \varepsilon\sqrt{2n-4} + 18/\varepsilon∑z∈L​vz​≤ε2n−4​+18/ε and ∑z∈Svz≤(1+3ε)2n−4\sum_{z \in S} \mathbf v_z \le (1 + 3\varepsilon)\sqrt{2n-4}∑z∈S​vz​≤(1+3ε)2n−4​.
  6. Eq. (7): ∑y∼u, y∈Svy≥(vu−ε)2n−4−18/ε\sum_{y \sim u,\, y \in S} \mathbf v_y \ge (\mathbf v_u - \varepsilon)\sqrt{2n-4} - 18/\varepsilon∑y∼u,y∈S​vy​≥(vu​−ε)2n−4​−18/ε for u∈Lu \in Lu∈L.
  7. Lemma 10: vz>1/6n\mathbf v_z > 1/\sqrt{6n}vz​>1/6n​ for every vertex zzz.
  8. ∣{y∈S:y≁x}∣≤14εn|\{y \in S : y \not\sim x\}| \le 14\varepsilon n∣{y∈S:y∼x}∣≤14εn (p. 10).
  9. Lemma 11: a vertex w∈Lw \in Lw∈L, w≠xw \ne xw=x, with vw>1−24ε\mathbf v_w > 1 - 24\varepsilonvw​>1−24ε and ∣{y∈S:y≁w}∣≤94εn|\{y \in S : y \not\sim w\}| \le 94\varepsilon n∣{y∈S:y∼w}∣≤94εn.
  10. Lemma 12: vu<1/10\mathbf v_u < 1/10vu​<1/10 for every u∉{x,w}u \notin \{x, w\}u∈/{x,w}.
  11. Lemma 13: x∼wx \sim wx∼w.
  12. Lemma 14: every vertex other than xxx and www is adjacent to both.
  13. A planar graph with two distinct vertices adjacent to all other vertices is a spanning subgraph of K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​ (proof of Theorem 15, p. 13).

Significance

The result. Theorem 15 settles the Boots–Royle / Cao–Vince conjecture for all large nnn. It identifies the planar graph of maximum spectral radius exactly, so the theoretical upper bound that the geographic application asks for is λ1(K2+Pn−2)\lambda_1(K_2 + P_{n-2})λ1​(K2​+Pn−2​). Along the way, Lemmas 8–14 describe the eigenvector of the extremal graph: two vertices carry almost all of the eigenvector weight, and every other entry is below 1/101/101/10. The same method proves the outerplanar analogue (Theorem 7, the companion mission of this series).

Formalizing it. The theorem is proved on paper and has no machine-checked proof. Formalizing it needs several pieces that are absent from Mathlib or the platform and are reusable: the edge bound 3n−63n - 63n−6 and the bipartite bound 2n−42n - 42n−4 for topologically planar graphs, the non-planarity of K3,3K_{3,3}K3,3​ and K5K_5K5​ and of their subdivisions, Rayleigh-quotient comparison of spectral radii, and the face structure of maximal planar graphs. Each milestone is a self-contained target.

Difficulty

Counting edges does not separate the candidates. A maximizer can be taken to be a maximal planar graph, so it has exactly 3n−63n - 63n−6 edges. Every maximal planar graph on nnn vertices has the same number of edges, and the standard lower bound λ1≥2∣E∣/n\lambda_1 \ge 2|E|/nλ1​≥2∣E∣/n is the same for all of them. The extremal graph is pinned down only through its eigenvector. One has to show that the weight concentrates on two vertices, which are then forced to be adjacent to each other (Lemma 13) and to every other vertex (Lemma 14). Lemma 13 is the step specific to planarity. It uses the triangular faces of a maximal planar graph to find an edge switch that keeps the graph planar. In the formal setting, planarity is topological, so every planarity fact of the argument (the edge counts, the K3,3K_{3,3}K3,3​ and K5K_5K5​ obstructions, the faces of a triangulation) has to be derived from the drawing.

Formalization scope

  • Graphs are SimpleGraph (Fin n). "GGG is K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​" is a graph isomorphism G ≃g bookPath n, where bookPath n lives on Fin 2 ⊕ Fin (n - 2). It is not an equality on a fixed labelling.
  • λ1\lambda_1λ1​ is the published WangKangXue.SpectralTuran.specRad, the largest eigenvalue of the real adjacency matrix.
  • Planarity is the published topological RobertsonSeymour1986.GM5.IsPlanar: a drawing by simple arcs. It is not replaced by K5K_5K5​/K3,3K_{3,3}K3,3​-minor-freeness or by an edge count, either of which would change the class the maximum ranges over.
  • Extremality is IsSpecMax IsPlanar G: GGG is planar and λ1(G′)≤λ1(G)\lambda_1(G') \le \lambda_1(G)λ1​(G′)≤λ1​(G) for every planar G′G'G′ on Fin n. Every milestone from Lemma 8 to Lemma 14 assumes it. These lemmas are false for an arbitrary planar graph, so a statement that drops the hypothesis, or replaces it by a property implying the conclusion, is not acceptable.
  • The eigenvector is universally quantified: every v\mathbf vv with Av=λ1vA\mathbf v = \lambda_1 \mathbf vAv=λ1​v, all entries positive, all entries at most 111, and every xxx with vx=1\mathbf v_x = 1vx​=1. Such a vector exists because the maximizer is connected (Perron–Frobenius). A statement that only asserts the existence of some eigenvector is weaker and is ruled out.
  • Quantifiers. "For nnn sufficiently large" is ∃N ∀n≥N\exists N\ \forall n \ge N∃N ∀n≥N, and NNN may depend on ε\varepsilonε. Milestones 4–8 hold for every ε>0\varepsilon > 0ε>0. Lemmas 11–14 hold for 0<ε<ε00 < \varepsilon < \varepsilon_00<ε<ε0​ with an unspecified ε0\varepsilon_0ε0​, because the paper chooses ε\varepsilonε small. The quantifier on ε\varepsilonε is always outermost, so ε\varepsilonε never depends on nnn or GGG. Lemmas 12–14 hold for every vertex www satisfying the conclusion of Lemma 11 (the predicate IsSecondHub), with the constants 242424 and 949494.
  • Added hypotheses. n≥3n \ge 3n≥3 in the planar facts and in Lemma 8, where the paper's standing "nnn large enough" is needed only to that extent. The page names the vertex of Lemma 12 vvv, the same letter as the eigenvector; it is renamed uuu. Lemma 14's set AAA is stated in unfolded form.
  • Infrastructure that a complete development needs: Euler's formula for topologically planar graphs, the non-planarity of K3,3K_{3,3}K3,3​ and K5K_5K5​, Perron–Frobenius for connected graphs, and the Rayleigh quotient. Proofs of the planar facts (milestone 2) are reusable well beyond this mission. Contributions toward any of them are welcome.

Selected references

  • M. Tait and J. Tobin, Three conjectures in extremal spectral graph theory, J. Combin. Theory Ser. B (2017). Preprint arXiv:1606.01916v2. https://arxiv.org/abs/1606.01916, DOI https://doi.org/10.1016/j.jctb.2017.04.006
  • B. N. Boots and G. F. Royle, A conjecture on the maximum value of the principal eigenvalue of a planar graph, Geographical Analysis 23(3) (1991), 276–282.
  • D. Cao and A. Vince, The spectral radius of a planar graph, Linear Algebra Appl. 187 (1993), 251–257.
  • A. J. Schwenk and R. J. Wilson, On the eigenvalues of a graph, in: Selected Topics in Graph Theory, Academic Press, 1978, 307–336.
  • Hong Yuan, A bound on the spectral radius of graphs, Linear Algebra Appl. 108 (1988), 135–139.
  • M. N. Ellingham and X. Zha, The spectral radius of graphs on surfaces, J. Combin. Theory Ser. B 78(1) (2000), 45–56.
  • Z. Dvořák and B. Mohar, Spectral radius of finite and infinite planar graphs and of graphs of bounded genus, J. Combin. Theory Ser. B 100(6) (2010), 729–739.

Bibliographic data as given in the bibliography of Tait and Tobin (pp. 21–23).

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Three Conjectures in Extremal Spectral Graph Theory 1: For Large n, K₁ + Pₙ₋₁ Is the Unique Outerplanar Graph on n Vertices of Maximum Spectral Radius (Cvetković–Rowlinson Conjecture)Research Paper

Motivation

The spectral radius λ1(G)\lambda_1(G)λ1​(G) of a graph GGG, the largest eigenvalue of its adjacency matrix, is a standard measure of how densely and how centrally a graph is connected. A classical theme of spectral graph theory asks, for a natural family of graphs, which member of the family on nnn vertices maximizes λ1\lambda_1λ1​. For planar graphs this question was raised by geographers comparing road and transport networks, and for outerplanar graphs it was posed by Cvetković and Rowlinson in their 1990 survey of the largest eigenvalue of a graph, where they relate it to the study of subfamilies of Hamiltonian graphs.

Conjecture (Cvetković–Rowlinson, 1990). The outerplanar graph on nnn vertices of maximum spectral radius is K1+Pn−1K_1 + P_{n-1}K1​+Pn−1​.

Timeline:

  • 1990. Cvetković and Rowlinson state the conjecture (Linear and Multilinear Algebra 28).
  • 1990. Rowlinson makes partial progress, on the index of certain outerplanar graphs (Ars Combinatoria 29).
  • 1993. Cao and Vince work on the spectral radius of planar graphs and the related conjecture (Linear Algebra Appl. 187).
  • 2001. Zhou, Lin and Hu study the spectral radius of Hamiltonian planar and outerplanar graphs (Tsinghua Science and Technology 6).
  • 2017. Tait and Tobin prove the conjecture for all sufficiently large nnn (arXiv:1606.01916, J. Combin. Theory Ser. B, doi:10.1016/j.jctb.2017.04.006), Theorem 7.

This mission formalizes Section 2 of Tait and Tobin.

Setting

All graphs are finite and simple. An nnn-vertex graph GGG has vertex set V(G)={0,…,n−1}V(G) = \{0, \dots, n-1\}V(G)={0,…,n−1}, adjacency matrix A(G)A(G)A(G), and spectral radius λ1(G)\lambda_1(G)λ1​(G), the largest eigenvalue of the real symmetric matrix A(G)A(G)A(G). Write dud_udu​ for the degree of a vertex uuu and N(u)N(u)N(u) for its neighbourhood.

A plane drawing of GGG places the vertices at distinct points of R2\mathbb R^2R2 and each edge as a simple arc between its ends; an arc passes through no other vertex, and two arcs meet only at a common end. The union of the vertex points and arcs is a compact set, so its complement has exactly one unbounded connected component, the outer face. A graph is outerplanar if it has a plane drawing in which every vertex lies on the boundary of the outer face.

The join G+HG + HG+H of two graphs is their disjoint union together with all edges between them. The fan K1+Pn−1K_1 + P_{n-1}K1​+Pn−1​ is a single vertex joined to every vertex of a path on n−1n-1n−1 vertices; it is outerplanar and has 2n−32n-32n−3 edges.

An outerplanar graph GGG on nnn vertices is a spectral maximizer if λ1(G′)≤λ1(G)\lambda_1(G') \le \lambda_1(G)λ1​(G′)≤λ1​(G) for every outerplanar graph G′G'G′ on the same nnn vertices.

Several milestones refer to a Perron vector: an eigenvector v\mathbf vv of A(G)A(G)A(G) for λ1\lambda_1λ1​ with all entries positive, normalized so that its maximum entry is 111, together with a vertex xxx with vx=1\mathbf v_x = 1vx​=1. For a connected graph such a vector exists by the Perron–Frobenius theorem.

Formalization targets

Goal: Theorem 7

There is NNN such that for every n≥Nn \ge Nn≥N and every graph GGG on nnn vertices,

G is an outerplanar spectral maximizer  ⟺  G≅K1+Pn−1.G \text{ is an outerplanar spectral maximizer} \iff G \cong K_1 + P_{n-1}.G is an outerplanar spectral maximizer⟺G≅K1​+Pn−1​.

The forward direction is the paper's Theorem 7; the converse says that the fan is the maximizer, as the conjecture reads. The threshold NNN is left unspecified, as in the paper.

Milestones

The milestones follow the proof in Section 2, in order:

  1. a strict subgraph of a connected graph has strictly smaller λ1\lambda_1λ1​ (already proved on the platform);
  2. an outerplanar graph on n≥2n \ge 2n≥2 vertices has at most 2n−32n-32n−3 edges and no K2,3K_{2,3}K2,3​ subgraph;
  3. Lemma 3: for n≥3n \ge 3n≥3 a spectral maximizer has λ1>n−1\lambda_1 > \sqrt{n-1}λ1​>n−1​;
  4. Lemma 4: du>vun−11nd_u > \mathbf v_u n - 11\sqrt ndu​>vu​n−11n​ for every vertex uuu;
  5. Lemma 5: for nnn large, dx>n−11nd_x > n - 11\sqrt ndx​>n−11n​ and vu<C1/n\mathbf v_u < C_1/\sqrt nvu​<C1​/n​ for every u≠xu \ne xu=x, with an absolute constant C1C_1C1​;
  6. Lemma 6: for nnn large, ∑z∈Bvz<C2/n\sum_{z\in B}\mathbf v_z < C_2/\sqrt n∑z∈B​vz​<C2​/n​, where B=V(G)∖(N(x)∪{x})B = V(G)\setminus(N(x)\cup\{x\})B=V(G)∖(N(x)∪{x});
  7. for nnn large, B=∅B = \emptysetB=∅: xxx is adjacent to every other vertex;
  8. an outerplanar graph with a vertex adjacent to all others is a spanning subgraph of K1+Pn−1K_1 + P_{n-1}K1​+Pn−1​.

Significance

The theorem settles, for all large nnn, a conjecture that had been open since 1990 and had resisted several partial attacks. The same paper settles, in the same framework, the planar analogue (the Boots–Royle and Cao–Vince conjecture, K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​) and a conjecture on spectral irregularity. The outerplanar case is the shortest of the three.

On the formal side, the result is proved on paper but has no machine-checked proof. Completing the mission produces a formal theory of outerplanar plane drawings (edge bound, K2,3K_{2,3}K2,3​-freeness, outerplanarity of the fan), eigenvector estimates for extremal graphs, and the full extremal theorem. The edge bound and the K2,3K_{2,3}K2,3​ exclusion are reusable for any later work on outerplanar or series–parallel graphs. Determining the exact threshold NNN, or proving the statement for every n≥2n \ge 2n≥2, would be a strengthening beyond the paper.

Difficulty

There are two separate difficulties. The first is topological: the facts about outerplanar graphs that the spectral argument uses (at most 2n−32n-32n−3 edges, no K2,3K_{2,3}K2,3​ subgraph, no cycle in G−xG - xG−x when xxx dominates, outerplanarity of the fan) are folklore on paper but require a Jordan-curve-type argument about plane drawings, of which Mathlib currently contains very little. The second is spectral: the edge-switching step that proves B=∅B = \emptysetB=∅ compares λ1\lambda_1λ1​ of two graphs through the Rayleigh quotient, and needs a positive Perron vector and the variational characterization of the largest eigenvalue for symmetric matrices. A purely combinatorial edge-maximization argument does not work: the fan is not the only outerplanar graph with 2n−32n-32n−3 edges, so maximizing the number of edges does not identify the spectral maximizer.

Formalization scope

  • Graphs are SimpleGraph (Fin n); λ1\lambda_1λ1​ is the published WangKangXue.SpectralTuran.specRad, the largest eigenvalue of G.adjMatrix ℝ.
  • Outerplanarity is topological: a published RobertsonSeymour1986.GM5.PlaneDrawing with every vertex point in the closure of the unbounded component of the complement of the drawing. It is not replaced by a forbidden-minor characterization; such characterizations are theorems about outerplanarity, and would change which graphs compete in the maximization.
  • Extremality is IsSpecMax IsOuterplanar G: GGG is outerplanar and no outerplanar graph on the same vertex set has larger λ1\lambda_1λ1​. It is never weakened to a comparison with the fan.
  • "GGG is K1+Pn−1K_1 + P_{n-1}K1​+Pn−1​" is a graph isomorphism G ≃g fan n, with the fan on Fin 1 ⊕ Fin (n - 1).
  • Perron-vector statements quantify over every positive eigenvector for λ1\lambda_1λ1​ with maximum entry 111 and every vertex xxx with vx=1\mathbf v_x = 1vx​=1; existential quantification over v\mathbf vv would be weaker.
  • "For some absolute constant" is an existential quantifier placed before the threshold, the graph and the vector; "for nnn sufficiently large" is ∃ N, ∀ n ≥ N.
  • Added hypotheses, each forced by a degenerate case: n≥2n \ge 2n≥2 for the edge bound (the bound 2n−32n-32n−3 is negative below), n≥3n \ge 3n≥3 for Lemma 3 (it fails for n=2n = 2n=2, where the maximizer K2K_2K2​ has λ1=1=n−1\lambda_1 = 1 = \sqrt{n-1}λ1​=1=n−1​).

A complete development needs the Perron–Frobenius theorem for symmetric nonnegative matrices and the Rayleigh quotient characterization of λ1\lambda_1λ1​, both of general use; the theory of outerplanar drawings; and the counting arguments of the lemmas. Contributions to any of these layers are welcome, as are independent proofs of the outerplanar facts from the drawing definition.

Selected references

  • M. Tait and J. Tobin, Three conjectures in extremal spectral graph theory, J. Combin. Theory Ser. B (2017), https://doi.org/10.1016/j.jctb.2017.04.006; preprint arXiv:1606.01916v2, https://arxiv.org/abs/1606.01916
  • D. Cvetković and P. Rowlinson, The largest eigenvalue of a graph: a survey, Linear and Multilinear Algebra 28 (1990), 3–33.
  • P. Rowlinson, On the index of certain outerplanar graphs, Ars Combinatoria 29 (1990), 221–225.
  • D. Cao and A. Vince, The spectral radius of a planar graph, Linear Algebra Appl. 187 (1993), 251–257.
  • J. Zhou, C. Lin and G. Hu, Spectral radius of Hamiltonian planar graphs and outerplanar graphs, Tsinghua Science and Technology 6 (2001), 350–354.
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Operations ResearchOptimization·Captain: mikedeng1

Multistage Adaptive Robust Optimization for the Unit Commitment Problem I: Without Ramping Constraints, Two-Stage and Multistage Robust Unit Commitment Are EquivalentResearch Paper

Motivation

Unit commitment (UC) is the day-ahead decision of an electricity system operator: which generators to switch on in each hour of the next day, and how much each of them should produce. System operators solve UC problems every day, and their cost and reliability are first-order concerns of power-system operations. With a large share of wind and solar generation, the net load (demand minus renewable output) at each node is uncertain at commitment time, and robust optimization is one of the standard ways to commit units that remain operable for every load trajectory in an uncertainty set.

The robust UC literature first adopted the two-stage model (Jiang et al. 2012; Zhao and Zeng 2012; Bertsimas et al. 2013): commitments are chosen first, then the dispatch is chosen after the whole day's net loads are revealed. In reality the operator learns the loads hour by hour, so the dispatch at hour ttt may only use what has been observed up to ttt. Lorca, Sun, Litvinov and Zheng (2016) introduced the multistage robust UC model that imposes this non-anticipativity, and asked when the extra realism matters. Their answer is this mission's goal: it matters only through the ramping constraints.

Setting

There are generators i∈Ngi\in\mathcal N_gi∈Ng​, net-load nodes j∈Ndj\in\mathcal N_dj∈Nd​, lines l∈Nll\in\mathcal N_ll∈Nl​ and hours t∈T={1,…,T}t\in\mathcal T=\{1,\dots,T\}t∈T={1,…,T}.

  • A commitment (x,u,v)(x,u,v)(x,u,v) consists of on/off, start-up and shut-down indicators xit,uit,vit∈{0,1}x_i^t,u_i^t,v_i^t\in\{0,1\}xit​,uit​,vit​∈{0,1}. The set XXX of admissible commitments is cut out by the logical constraints (1b)–(1g): the start-up/shut-down identity xit−xit−1=uit−vitx_i^t-x_i^{t-1}=u_i^t-v_i^txit​−xit−1​=uit​−vit​ and minimum up and down times UTi,DTiUT_i,DT_iUTi​,DTi​.
  • For a commitment xxx and the hour-ttt net loads dt∈RNdd^t\in\mathbb R^{N_d}dt∈RNd​, the dispatch set without ramping ΩtNR(x,dt)\Omega_t^{NR}(x,d^t)ΩtNR​(x,dt) is the set of pt∈RNgp^t\in\mathbb R^{N_g}pt∈RNg​ with generation limits pimin⁡xit≤pit≤pimax⁡xitp_i^{\min}x_i^t\le p_i^t\le p_i^{\max}x_i^tpimin​xit​≤pit​≤pimax​xit​, line limits ∣αl⊤(Bppt−Bddt)∣≤flmax⁡|\alpha_l^\top(B^pp^t-B^dd^t)|\le f_l^{\max}∣αl⊤​(Bppt−Bddt)∣≤flmax​ and energy balance ∑ipit=∑jdjt\sum_ip_i^t=\sum_jd_j^t∑i​pit​=∑j​djt​.
  • The ramping constraints (1i) couple consecutive hours: −RDitxit−SDitvit≤pit−pit−1≤RUitxit−1+SUituit-RD_i^tx_i^t-SD_i^tv_i^t\le p_i^t-p_i^{t-1}\le RU_i^tx_i^{t-1}+SU_i^tu_i^t−RDit​xit​−SDit​vit​≤pit​−pit−1​≤RUit​xit−1​+SUit​uit​.
  • The budget uncertainty set is D=∏tDt\mathcal D=\prod_t\mathcal D^tD=∏t​Dt with
Dt={dt: ∑j∣djt−dˉjt∣d^jt≤ΓNd,  djt∈[dˉjt−Γd^jt, dˉjt+Γd^jt]}.\mathcal D^t=\Big\{d^t:\ \sum_j\frac{|d_j^t-\bar d_j^t|}{\hat d_j^t}\le\Gamma\sqrt{N_d},\ \ d_j^t\in[\bar d_j^t-\Gamma\hat d_j^t,\ \bar d_j^t+\Gamma\hat d_j^t]\Big\}.Dt={dt: j∑​d^jt​∣djt​−dˉjt​∣​≤ΓNd​​,  djt​∈[dˉjt​−Γd^jt​, dˉjt​+Γd^jt​]}.
  • The commitment cost is F(x)=∑t∑i(Gixit+Siuit)F(x)=\sum_t\sum_i(G_ix_i^t+S_iu_i^t)F(x)=∑t​∑i​(Gi​xit​+Si​uit​) and the dispatch cost is ∑t∑iCipit\sum_t\sum_iC_ip_i^t∑t​∑i​Ci​pit​.

The two-stage robust UC (2) minimizes over XXX

F(x)+max⁡d∈D min⁡p∈Ω(x,d) ∑t∑iCipit,F(x)+\max_{d\in\mathcal D}\ \min_{p\in\Omega(x,d)}\ \sum_t\sum_iC_ip_i^t ,F(x)+d∈Dmax​ p∈Ω(x,d)min​ t∑​i∑​Ci​pit​,

where the dispatch ppp is chosen knowing the whole trajectory ddd. The multistage robust UC (5) minimizes over XXX

F(x)+min⁡p(⋅) max⁡d∈D ∑t∑iCipit(d[t]),F(x)+\min_{p(\cdot)}\ \max_{d\in\mathcal D}\ \sum_t\sum_iC_ip_i^t(d^{[t]}),F(x)+p(⋅)min​ d∈Dmax​ t∑​i∑​Ci​pit​(d[t]),

over policies pt(d[t])p^t(d^{[t]})pt(d[t]) that depend only on d[t]=(d1,…,dt)d^{[t]}=(d^1,\dots,d^t)d[t]=(d1,…,dt) and satisfy the dispatch constraints for every d∈Dd\in\mathcal Dd∈D.

Formalization targets

Goal: Theorem 1 (p. 11)

With the ramping constraints deleted from both models,

F(x)+max⁡d∈Dmin⁡p∈ΩNR(x,d)c(p)  =  F(x)+min⁡p(⋅) non-anticipativemax⁡d∈Dc(p(d))for every (x,u,v)∈X,F(x)+\max_{d\in\mathcal D}\min_{p\in\Omega^{NR}(x,d)}c(p)\;=\;F(x)+\min_{p(\cdot)\ \text{non-anticipative}}\max_{d\in\mathcal D}c(p(d))\qquad\text{for every }(x,u,v)\in X,F(x)+d∈Dmax​p∈ΩNR(x,d)min​c(p)=F(x)+p(⋅) non-anticipativemin​d∈Dmax​c(p(d))for every (x,u,v)∈X,

and consequently the two problems have the same optimal value over XXX.

Milestones (the steps of the paper's proof)

Both sides are compared with problem (1P), whose objective is

F(x)+∑t∈T max⁡dt∈Dt min⁡pt∈ΩtNR(x,dt) ∑iCipit.F(x)+\sum_{t\in\mathcal T}\ \max_{d^t\in\mathcal D^t}\ \min_{p^t\in\Omega_t^{NR}(x,d^t)}\ \sum_iC_ip_i^t .F(x)+t∈T∑​ dt∈Dtmax​ pt∈ΩtNR​(x,dt)min​ i∑​Ci​pit​.
  1. Part (i): the dispatch set without ramping is separable over time; the uncertainty set (3) is separable over time; hence the two-stage objective equals the (1P) objective.
  2. Part (ii): the multistage objective equals the nested max-min value of (M~NR)(\widetilde M^{NR})(MNR); one stage of the nested problem splits off the later value; backward induction gives the sum of per-period worst cases; hence the multistage objective equals the (1P) objective.

Companion results (Example 1, Propositions 1–2, pp. 7–9)

On a two-bus, two-hour system with line limit and ramp rates equal to 111, the two-stage model is feasible (Proposition 1), yet under its commitment no causal dispatch policy is feasible (Proposition 2). These show that the hypothesis "without ramping constraints" cannot be dropped.

Significance

The theorem locates exactly where multistage robust UC differs from the two-stage model: in the inter-temporal coupling created by ramping. Without ramping, the hourly dispatch problems decouple and so does the uncertainty set, so seeing the future gives the dispatch no advantage. With ramping, Example 1 shows the two-stage model can certify a commitment that fails in real-time operation. The practical message drawn in the paper is that the multistage model is useful precisely when ramping capability is a scarce resource, which is the situation of systems with high renewable penetration.

The result is proved in the paper. As far as is known it has not been machine-checked. This mission produces a formal model of robust UC (commitment logic, network-constrained dispatch, budget uncertainty, non-anticipative policies) together with a checked proof of the equivalence and of the counterexample. The model is a reusable base for later formal work on robust and multistage power-system models, such as the affine-policy results of the same paper.

Difficulty

The two separability steps are short on paper but must be carried out in the extended reals, where infeasible dispatch problems have value +∞+\infty+∞ and sums of extended reals are not well behaved in general; the argument has to show that no −∞-\infty−∞ arises. The main gap is the multistage side. The paper passes from the policy formulation (5) to the nested max-min formulation (6) by a remark, without proof. Formally, the value of an optimization over non-anticipative policies, which are functions on the whole uncertainty set, has to be identified with a backward max-min recursion over the per-hour sets, in both directions and without any attainment of the minima. A tempting shortcut, defining the multistage model as the nested formula, would prove nothing about policies and is excluded.

Formalization scope

  • Hours are Fin T, 0-based: Lean period ttt is the paper's t+1t+1t+1. Generators, nodes, buses and lines are Fin Ng, Fin Nd, Fin Nb, Fin Nl.
  • The initial status x0x^0x0 and dispatch p0p^0p0, which (1c) and (1i) use at the first hour, are data fields; the paper leaves them implicit.
  • Commitment variables are real-valued with the constraint {0,1}\{0,1\}{0,1} inside XXX. The index ranges of (1d)–(1g) avoid natural-number subtraction.
  • All optimal values are in EReal; an infimum over an empty set is +∞+\infty+∞, the paper's convention for infeasibility.
  • Standing assumptions of the budget set (3), carried as hypotheses: Γ≥0\Gamma\ge0Γ≥0 and d^jt>0\hat d_j^t>0d^jt​>0. They make dˉ∈D\bar d\in\mathcal Ddˉ∈D, so every Dt\mathcal D^tDt is nonempty.
  • Policies are functions of the hour and the whole trajectory; non-anticipativity is the requirement that the dispatch at hour ttt depends only on the net loads up to hour ttt. Without this requirement the multistage model would coincide with the two-stage model by definition and the theorem would be empty.
  • "Equivalent" is formalized as equality of the two objectives at every commitment in XXX, plus equality of the optimal values.
  • Example 1 is formalized on its own: two buses, the commitment ((1,1),(1,1))((1,1),(1,1))((1,1),(1,1)), energy balance, ramp bounds ±1\pm1±1 and the line limit 111 on the net injection at bus AAA. It is not an instance of the budget set (3).

Contributions welcome: proofs of the milestones and the goal, and lemmas on infima and suprema of sums over product sets in EReal, which are reusable beyond this mission.

Selected references

  • Á. Lorca, X. A. Sun, E. Litvinov, T. Zheng, Multistage adaptive robust optimization for the unit commitment problem, Operations Research 64(1), 2016. https://doi.org/10.1287/opre.2015.1456
  • D. Bertsimas, E. Litvinov, X. A. Sun, J. Zhao, T. Zheng, Adaptive robust optimization for the security constrained unit commitment problem, IEEE Transactions on Power Systems 28(1), 2013. https://doi.org/10.1109/TPWRS.2012.2205021
  • R. Jiang, J. Wang, Y. Guan, Robust unit commitment with wind power and pumped storage hydro, IEEE Transactions on Power Systems 27(2) 800–810, 2012.
  • L. Zhao, B. Zeng, Robust unit commitment problem with demand response and wind energy, IEEE Power and Energy Society General Meeting, 2012, 1–8.
  • J. Ostrowski, M. F. Anjos, A. Vannelli, Tight mixed integer linear programming formulations for the unit commitment problem, IEEE Transactions on Power Systems 27(1), 2012 (cited for the form of (1d)–(1g)).
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Control TheoryConvex OptimizationOptimization·Captain: mikedeng1

Analysis and Design of Optimization Algorithms via Integral Quadratic Constraints I: A Feasible LMI and a ρ-Hard IQC Certify the Linear Rate ‖ξₖ − ξ⋆‖ ≤ √cond(P) ρᵏ ‖ξ₀ − ξ⋆‖Research Paper

Motivation

First-order methods such as the gradient method, Nesterov's accelerated method and the Heavy-ball method are usually analysed one at a time, each with its own hand-built potential function. Lessard, Recht and Packard (SIAM J. Optim. 26(1), 2016; read here in arXiv:1408.3595v7) observed that such a method is a linear dynamical system in feedback with the gradient map, and that tools from robust control, the integral quadratic constraints (IQCs) of Megretski and Rantzer (IEEE TAC 42(6), 1997), turn the question "does this method converge linearly, and at what rate?" into the feasibility of a small semidefinite program. The size of that program depends on the algorithm, not on the dimension of the optimization problem.

The paper's main result, Theorem 4, is the certificate behind this approach. It has been the starting point of a line of work on automated and computer-aided analysis of optimization algorithms, including the design of new methods with provably optimal rates.

Setting

An iterative algorithm is a linear system GGG with state ξk∈Rnξ\xi_k \in \mathbb R^{n_\xi}ξk​∈Rnξ​, driven by an input uk∈Rdu_k \in \mathbb R^duk​∈Rd and producing an output yk∈Rdy_k \in \mathbb R^dyk​∈Rd:

ξk+1=Aξk+Buk,yk=Cξk.\xi_{k+1} = A\xi_k + Bu_k, \qquad y_k = C\xi_k .ξk+1​=Aξk​+Buk​,yk​=Cξk​.

The loop is closed by a map φ\varphiφ from sequences to sequences, u=φ(y)u = \varphi(y)u=φ(y). For the gradient method, A=IA = IA=I, B=−αIB = -\alpha IB=−αI, C=IC = IC=I and uk=∇f(yk)u_k = \nabla f(y_k)uk​=∇f(yk​).

Instead of φ\varphiφ itself, one uses a constraint that φ\varphiφ is known to satisfy. A filter Ψ\PsiΨ is a second linear system with state ζk∈Rnζ\zeta_k \in \mathbb R^{n_\zeta}ζk​∈Rnζ​, inputs (yk,uk)(y_k, u_k)(yk​,uk​) and output zk∈Rnzz_k \in \mathbb R^{n_z}zk​∈Rnz​:

ζ0=ζ⋆,ζk+1=AΨζk+BΨyyk+BΨuuk,zk=CΨζk+DΨyyk+DΨuuk.\zeta_0 = \zeta_\star,\qquad \zeta_{k+1} = A_\Psi\zeta_k + B^y_\Psi y_k + B^u_\Psi u_k,\qquad z_k = C_\Psi\zeta_k + D^y_\Psi y_k + D^u_\Psi u_k .ζ0​=ζ⋆​,ζk+1​=AΨ​ζk​+BΨy​yk​+BΨu​uk​,zk​=CΨ​ζk​+DΨy​yk​+DΨu​uk​.

Given a reference point (y⋆,u⋆)(y_\star, u_\star)(y⋆​,u⋆​), the pair (ζ⋆,z⋆)(\zeta_\star, z_\star)(ζ⋆​,z⋆​) is the fixed point of the filter: ζ⋆=AΨζ⋆+BΨyy⋆+BΨuu⋆\zeta_\star = A_\Psi\zeta_\star + B^y_\Psi y_\star + B^u_\Psi u_\starζ⋆​=AΨ​ζ⋆​+BΨy​y⋆​+BΨu​u⋆​ and z⋆=CΨζ⋆+DΨyy⋆+DΨuu⋆z_\star = C_\Psi\zeta_\star + D^y_\Psi y_\star + D^u_\Psi u_\starz⋆​=CΨ​ζ⋆​+DΨy​y⋆​+DΨu​u⋆​. Assume ρ(AΨ)<1\rho(A_\Psi) < 1ρ(AΨ​)<1 (all eigenvalues of AΨA_\PsiAΨ​ have modulus less than one) and let MMM be a symmetric matrix. The map φ\varphiφ satisfies the ρ\rhoρ-hard IQC defined by (Ψ,M,ρ,y⋆,u⋆)(\Psi, M, \rho, y_\star, u_\star)(Ψ,M,ρ,y⋆​,u⋆​) if, for every input sequence yyy, with u=φ(y)u = \varphi(y)u=φ(y) and z=Ψ(y,u)z = \Psi(y,u)z=Ψ(y,u),

∑t=0kρ−2t(zt−z⋆)⊤M(zt−z⋆)≥0for all k≥0.\sum_{t=0}^{k} \rho^{-2t}(z_t - z_\star)^\top M (z_t - z_\star) \ge 0 \qquad \text{for all } k \ge 0 .t=0∑k​ρ−2t(zt​−z⋆​)⊤M(zt​−z⋆​)≥0for all k≥0.

It satisfies the pointwise IQC if each term (zk−z⋆)⊤M(zk−z⋆)(z_k - z_\star)^\top M (z_k - z_\star)(zk​−z⋆​)⊤M(zk​−z⋆​) is nonnegative.

Eliminating yyy, the systems GGG and Ψ\PsiΨ combine into one linear system with state xk=(ξk,ζk)x_k = (\xi_k, \zeta_k)xk​=(ξk​,ζk​):

xk+1=A^xk+B^uk,zk=C^xk+D^uk,A^=[A0BΨyCAΨ], B^=[BBΨu], C^=[DΨyCCΨ], D^=DΨu.x_{k+1} = \hat A x_k + \hat B u_k,\quad z_k = \hat C x_k + \hat D u_k,\qquad \hat A = \begin{bmatrix} A & 0 \\ B^y_\Psi C & A_\Psi\end{bmatrix},\ \hat B = \begin{bmatrix} B \\ B^u_\Psi\end{bmatrix},\ \hat C = \begin{bmatrix} D^y_\Psi C & C_\Psi\end{bmatrix},\ \hat D = D^u_\Psi .xk+1​=A^xk​+B^uk​,zk​=C^xk​+D^uk​,A^=[ABΨy​C​0AΨ​​], B^=[BBΨu​​], C^=[DΨy​C​CΨ​​], D^=DΨu​.

The condition number of a symmetric positive definite PPP is cond⁡(P)=λmax⁡(P)/λmin⁡(P)\operatorname{cond}(P) = \lambda_{\max}(P)/\lambda_{\min}(P)cond(P)=λmax​(P)/λmin​(P), and ∥⋅∥\|\cdot\|∥⋅∥ is the Euclidean norm.

Formalization targets

Goal: Theorem 4

Let (ξ⋆,ζ⋆,y⋆,u⋆,z⋆)(\xi_\star, \zeta_\star, y_\star, u_\star, z_\star)(ξ⋆​,ζ⋆​,y⋆​,u⋆​,z⋆​) be a fixed point of GGG and Ψ\PsiΨ (ξ⋆=Aξ⋆+Bu⋆\xi_\star = A\xi_\star + Bu_\starξ⋆​=Aξ⋆​+Bu⋆​, y⋆=Cξ⋆y_\star = C\xi_\stary⋆​=Cξ⋆​, and the filter equations above), let 0<ρ≤10 < \rho \le 10<ρ≤1, and suppose φ\varphiφ satisfies the ρ\rhoρ-hard IQC defined by (Ψ,M,ρ,y⋆,u⋆)(\Psi, M, \rho, y_\star, u_\star)(Ψ,M,ρ,y⋆​,u⋆​). If there are P≻0P \succ 0P≻0 and λ≥0\lambda \ge 0λ≥0 with

[A^⊤PA^−ρ2PA^⊤PB^B^⊤PA^B^⊤PB^]+λ[C^D^]⊤M[C^D^]⪯0,(3.9)\begin{bmatrix}\hat A^\top P\hat A - \rho^2 P & \hat A^\top P\hat B \\ \hat B^\top P\hat A & \hat B^\top P \hat B\end{bmatrix} + \lambda \begin{bmatrix}\hat C & \hat D\end{bmatrix}^\top M \begin{bmatrix}\hat C & \hat D\end{bmatrix} \preceq 0, \tag{3.9}[A^⊤PA^−ρ2PB^⊤PA^​A^⊤PB^B^⊤PB^​]+λ[C^​D^​]⊤M[C^​D^​]⪯0,(3.9)

then every trajectory of the interconnection, ξk+1=Aξk+B φ(Cξ)k\xi_{k+1} = A\xi_k + B\,\varphi(C\xi)_kξk+1​=Aξk​+Bφ(Cξ)k​, satisfies

∥ξk−ξ⋆∥≤cond⁡(P) ρk ∥ξ0−ξ⋆∥for all k.\|\xi_k - \xi_\star\| \le \sqrt{\operatorname{cond}(P)}\,\rho^k\,\|\xi_0 - \xi_\star\| \qquad \text{for all } k .∥ξk​−ξ⋆​∥≤cond(P)​ρk∥ξ0​−ξ⋆​∥for all k.

Milestones

The milestones follow the paper's proof: the elimination (3.6) of yyy; the one-step inequality (3.10) obtained from the LMI at a fixed point of (3.7); its weighted telescoped sum; the decay (xk−x⋆)⊤P(xk−x⋆)≤ρ2k(x0−x⋆)⊤P(x0−x⋆)(x_k - x_\star)^\top P (x_k - x_\star) \le \rho^{2k}(x_0 - x_\star)^\top P (x_0 - x_\star)(xk​−x⋆​)⊤P(xk​−x⋆​)≤ρ2k(x0​−x⋆​)⊤P(x0​−x⋆​) in the PPP-weighted norm; and the passage to the Euclidean norm with the factor cond⁡(P)\sqrt{\operatorname{cond}(P)}cond(P)​. Two companion statements are included: a pointwise IQC implies the ρ\rhoρ-hard IQC for every ρ>0\rho > 0ρ>0 (the remark after Theorem 4), and Proposition 2 (for ρ≥0\rho \ge 0ρ≥0), the Lyapunov characterisation ρ(T)<ρ  ⟺  ∃P≻0, T⊤PT−ρ2P≺0\rho(T) < \rho \iff \exists P \succ 0,\ T^\top P T - \rho^2 P \prec 0ρ(T)<ρ⟺∃P≻0, T⊤PT−ρ2P≺0.

Significance

Theorem 4 reduces a statement about all functions in a class, for instance all strongly convex functions with Lipschitz gradients in every dimension, to a semidefinite feasibility problem with a handful of variables. The paper uses it to recover the known rates of the gradient method and to compute numerically certified rates for Nesterov's method, and the same template underlies later rate certificates for proximal, operator-splitting and distributed methods. The pointwise remark is what lets the sector IQC of gradients be plugged in directly.

The theorem is proved in the paper; nothing about it is open. To our knowledge neither the IQC framework nor Theorem 4 has a machine-checked proof. A formal development gives the first verified version of the certificate, and with it a route by which a numerically found LMI solution, once checked exactly, yields a verified convergence rate for a concrete algorithm.

Difficulty

The argument is short; the difficulty is in the bookkeeping. The IQC is a statement about every input sequence, while the conclusion concerns one trajectory of the closed loop, so the proof has to instantiate the IQC at the trajectory's own output y=Cξy = C\xiy=Cξ and match the filter state it produces with the ζ\zetaζ-component of the combined state. The weights ρ−2t\rho^{-2t}ρ−2t must line up with the telescoping of the one-step inequality, and the final step needs the eigenvalue bounds λmin⁡(P)∥v∥2≤v⊤Pv≤λmax⁡(P)∥v∥2\lambda_{\min}(P)\|v\|^2 \le v^\top P v \le \lambda_{\max}(P)\|v\|^2λmin​(P)∥v∥2≤v⊤Pv≤λmax​(P)∥v∥2 together with the fact that ζ0=ζ⋆\zeta_0 = \zeta_\starζ0​=ζ⋆​ removes the filter state from the initial error. Block matrices indexed by sums of index types make each of these steps heavier in Lean than on paper.

Formalization scope

Vectors are Fin n → ℝ, matrices are Matrix (Fin a) (Fin b) ℝ, and sequences are ℕ → Fin n → ℝ indexed from 000. The norm is written out as v⊤v\sqrt{v^\top v}v⊤v​, because Mathlib's norm on Fin n → ℝ is the sup norm, under which the constant cond⁡(P)\sqrt{\operatorname{cond}(P)}cond(P)​ would be wrong. The combined state lives on Fin nξ ⊕ Fin nζ and the LMI on (Fin nξ ⊕ Fin nζ) ⊕ Fin d, assembled with Matrix.fromBlocks, fromRows and fromCols; "⪯0\preceq 0⪯0" is positive semidefiniteness of the negated matrix. cond⁡(P)\operatorname{cond}(P)cond(P) is the largest over the smallest eigenvalue of the Hermitian matrix PPP, and ρ(AΨ)<1\rho(A_\Psi) < 1ρ(AΨ​)<1 is stated over the complex spectrum.

The page allows 0≤ρ0 \le \rho0≤ρ; since the weights ρ−2t\rho^{-2t}ρ−2t are undefined at ρ=0\rho = 0ρ=0, every statement that uses them assumes ρ>0\rho > 0ρ>0. Proposition 2 is printed without a sign condition and is false for ρ<0\rho < 0ρ<0; it is stated for ρ≥0\rho \ge 0ρ≥0. The IQC hypothesis quantifies over every input sequence and every kkk, with the filter started at ζ⋆\zeta_\starζ⋆​; replacing it by the IQC along the single closed-loop trajectory, starting the filter at 000, or reading ∥⋅∥\|\cdot\|∥⋅∥ as the sup norm would each change the theorem, and none is the formalization. The trajectory in the goal is universally quantified ("for any ξ0\xi_0ξ0​"); its existence is not assumed. The hypotheses ρ(AΨ)<1\rho(A_\Psi) < 1ρ(AΨ​)<1 and M=M⊤M = M^\topM=M⊤ are kept as on the page although the proof does not use them. A sanity instance outside the proposal (the scalar gradient method with the sector IQC, ρ=1/2\rho = 1/2ρ=1/2, P=1P = 1P=1, λ=1/4\lambda = 1/4λ=1/4) checks in Lean that all hypotheses of the goal can hold at once.

The development needs only Mathlib's linear algebra: block matrices, PosDef/PosSemidef, the spectral theorem for Hermitian matrices, and finite sums. The Euclidean-norm lemma (decay in a PPP-norm implies decay in the Euclidean norm with factor cond⁡(P)\sqrt{\operatorname{cond}(P)}cond(P)​) and Proposition 2 are reusable beyond this mission. Proofs of any milestone, and of Proposition 2 in either direction, are welcome.

Selected references

  • L. Lessard, B. Recht, A. Packard, Analysis and Design of Optimization Algorithms via Integral Quadratic Constraints, SIAM J. Optim. 26(1):57–95, 2016. https://doi.org/10.1137/15M1009597 (arXiv version used: https://arxiv.org/abs/1408.3595v7)
  • A. Megretski, A. Rantzer, System Analysis via Integral Quadratic Constraints, IEEE Trans. Automat. Control 42(6):819–830, 1997. https://doi.org/10.1109/9.587335
  • Y. Nesterov, Introductory Lectures on Convex Optimization: A Basic Course, Kluwer, 2004. https://doi.org/10.1007/978-1-4419-8853-9
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Isoperimetric Inequalities in Simplicial Complexes 1: For a Finite d-Complex with a Complete Skeleton, the Spectral Gap Is at Most the Cheeger Constant, λ(X) ≤ h(X)Research Paper

Motivation

For a finite graph, the Cheeger constant measures how hard it is to cut the vertex set into two pieces, and the spectral gap of the graph Laplacian measures how fast random walks mix. The two Cheeger inequalities (Dodziuk 1984; Alon and Milman 1985; Alon 1986) bound each quantity by a function of the other, and they underlie the theory of expander graphs, with uses in derandomization, error-correcting codes and the analysis of Markov chains.

High-dimensional expanders extend this theory from graphs to simplicial complexes. Linial and Meshulam (2006) and Gromov (2010) introduced combinatorial and topological notions of expansion for complexes; the spectral side is Eckmann's discrete Hodge theory (1944), in which each dimension carries its own Laplacian. Parzanchevski, Rosenthal and Tessler (arXiv:1207.0638, Combinatorica 2015) defined a ddd-dimensional Cheeger constant h(X)h(X)h(X) through partitions of the vertices into d+1d+1d+1 blocks and proved the analogue of the upper Cheeger inequality, λ(X)≤h(X)\lambda(X)\le h(X)λ(X)≤h(X), for complexes with a complete skeleton. This mission formalizes that theorem.

Setting

Let V={0,1,…,n−1}V=\{0,1,\dots,n-1\}V={0,1,…,n−1} and d≥1d\ge1d≥1. A finite ddd-complex with a complete skeleton XXX on VVV consists of all subsets of VVV with at most ddd elements together with a set XdX^dXd of (d+1)(d+1)(d+1)-element subsets, the ddd-cells. A set of j+1j+1j+1 vertices is a jjj-cell; Xd−1X^{d-1}Xd−1 is therefore the set of all ddd-element subsets.

Each cell is oriented by the increasing order of its vertices, σ=[σ0,…,σj]\sigma=[\sigma_0,\dots,\sigma_j]σ=[σ0​,…,σj​] with σ0<⋯<σj\sigma_0<\dots<\sigma_jσ0​<⋯<σj​. The space Ωj\Omega^{j}Ωj of jjj-forms consists of the real functions on jjj-cells, with inner product

⟨f,g⟩=∑σ∈Xjf(σ)g(σ).\langle f,g\rangle=\sum_{\sigma\in X^{j}}f(\sigma)g(\sigma).⟨f,g⟩=σ∈Xj∑​f(σ)g(σ).

The co-boundary ∂d∗:Ωd−1→Ωd\partial_d^*:\Omega^{d-1}\to\Omega^d∂d∗​:Ωd−1→Ωd and the boundaries ∂d:Ωd→Ωd−1\partial_d:\Omega^d\to\Omega^{d-1}∂d​:Ωd→Ωd−1, ∂d−1:Ωd−1→Ωd−2\partial_{d-1}:\Omega^{d-1}\to\Omega^{d-2}∂d−1​:Ωd−1→Ωd−2 are

(∂d∗f)(τ)=∑i=0d(−1)if(τ∖τi),(∂jg)(σ)=∑v∼σg([v,σ0,…,σj−1]),(\partial_d^*f)(\tau)=\sum_{i=0}^d(-1)^i f(\tau\setminus\tau_i),\qquad (\partial_j g)(\sigma)=\sum_{v\sim\sigma}g([v,\sigma_0,\dots,\sigma_{j-1}]),(∂d∗​f)(τ)=i=0∑d​(−1)if(τ∖τi​),(∂j​g)(σ)=v∼σ∑​g([v,σ0​,…,σj−1​]),

where v∼σv\sim\sigmav∼σ means that v∉σv\notin\sigmav∈/σ and {v}∪σ\{v\}\cup\sigma{v}∪σ is a cell, and [v,σ0,… ][v,\sigma_0,\dots][v,σ0​,…] equals (−1)k(-1)^k(−1)k times the increasingly oriented cell when vvv has kkk smaller vertices in σ\sigmaσ. The upper Laplacian is Δ+=∂d∂d∗\Delta^+=\partial_d\partial_d^*Δ+=∂d​∂d∗​ on Ωd−1\Omega^{d-1}Ωd−1, and Zd−1=ker⁡∂d−1Z_{d-1}=\ker\partial_{d-1}Zd−1​=ker∂d−1​ is the space of (d−1)(d-1)(d−1)-cycles.

The spectral gap is the least eigenvalue of Δ+\Delta^+Δ+ on the cycles (Definition 2.1):

λ(X)=min⁡Spec⁡(Δ+∣Zd−1).\lambda(X)=\min\operatorname{Spec}\big(\Delta^+|_{Z_{d-1}}\big).λ(X)=minSpec(Δ+∣Zd−1​​).

For sets A0,…,Ad⊆VA_0,\dots,A_d\subseteq VA0​,…,Ad​⊆V, let F(A0,…,Ad)F(A_0,\dots,A_d)F(A0​,…,Ad​) be the set of ddd-cells with exactly one vertex in each AiA_iAi​. The Cheeger constant is (Definition 1.1)

h(X)=min⁡V=∐i=0dAin⋅∣F(A0,…,Ad)∣∣A0∣⋅∣A1∣⋯∣Ad∣,h(X)=\min_{V=\coprod_{i=0}^dA_i}\frac{n\cdot|F(A_0,\dots,A_d)|}{|A_0|\cdot|A_1|\cdots|A_d|},h(X)=V=∐i=0d​Ai​min​∣A0​∣⋅∣A1​∣⋯∣Ad​∣n⋅∣F(A0​,…,Ad​)∣​,

the minimum over partitions of VVV into nonempty sets A0,…,AdA_0,\dots,A_dA0​,…,Ad​. For d=1d=1d=1, Z0Z_0Z0​ is the space of functions summing to zero, Δ+\Delta^+Δ+ is the graph Laplacian, and hhh is the usual Cheeger constant min⁡A n∣E(A,Aˉ)∣/(∣A∣∣Aˉ∣)\min_{A}\,n|E(A,\bar A)|/(|A||\bar A|)minA​n∣E(A,Aˉ)∣/(∣A∣∣Aˉ∣).

Formalization targets

Goal: Theorem 1.2 (Cheeger Inequality)

λ(X)≤h(X)\lambda(X)\le h(X)λ(X)≤h(X)

for every finite ddd-complex XXX with a complete skeleton on n≥d+1n\ge d+1n≥d+1 vertices.

Milestones

  1. The chain-complex identity ∂d−1∂d=0\partial_{d-1}\partial_d=0∂d−1​∂d​=0 (p. 6).
  2. The form fff of (4.1), built from a partition, is a (d−1)(d-1)(d−1)-cycle (p. 12).
  3. ∂d∗\partial_d^*∂d∗​ is the adjoint of ∂d\partial_d∂d​: ⟨∂dg,f⟩=⟨g,∂d∗f⟩\langle\partial_dg,f\rangle=\langle g,\partial_d^*f\rangle⟨∂d​g,f⟩=⟨g,∂d∗​f⟩ (p. 6).
  4. Rayleigh's principle (4.2): λ(X)⟨f,f⟩≤⟨Δ+f,f⟩=⟨∂d∗f,∂d∗f⟩\lambda(X)\langle f,f\rangle\le\langle\Delta^+f,f\rangle=\langle\partial_d^*f,\partial_d^*f\rangleλ(X)⟨f,f⟩≤⟨Δ+f,f⟩=⟨∂d∗​f,∂d∗​f⟩ for f∈Zd−1f\in Z_{d-1}f∈Zd−1​ (p. 12).
  5. ⟨f,f⟩=n∏i=0d∣Ai∣\langle f,f\rangle=n\prod_{i=0}^d|A_i|⟨f,f⟩=n∏i=0d​∣Ai​∣ for the form (4.1) (p. 13).
  6. (4.3): ∣(∂d∗f)(σ)∣|(\partial_d^*f)(\sigma)|∣(∂d∗​f)(σ)∣ equals nnn for σ∈F(A0,…,Ad)\sigma\in F(A_0,\dots,A_d)σ∈F(A0​,…,Ad​) and 000 for the other ddd-cells (p. 13).
  7. ⟨∂d∗f,∂d∗f⟩=n2∣F(A0,…,Ad)∣\langle\partial_d^*f,\partial_d^*f\rangle=n^2|F(A_0,\dots,A_d)|⟨∂d∗​f,∂d∗​f⟩=n2∣F(A0​,…,Ad​)∣ (p. 14).

Milestones 2 and 5–7 hold for every partition, not only a minimizing one.

Significance

The result. Theorem 1.2 shows that a large spectral gap forces every partition of the vertices into d+1d+1d+1 blocks to be crossed by many ddd-cells, so spectral information certifies combinatorial expansion of a complex. The paper uses it with the spectral analysis of Gundert and Wagner to show that Linial–Meshulam random complexes X(d,n,Clog⁡n/n)X(d,n,C\log n/n)X(d,n,Clogn/n) have Cheeger constant of order log⁡n\log nlogn for large CCC (Corollary 1.3). The paper also shows that the converse direction fails: a triangulation of the Möbius strip has h(X)=114h(X)=1\tfrac14h(X)=141​ but λ(X)=0\lambda(X)=0λ(X)=0, so no lower bound of the form C⋅h(X)m≤λ(X)C\cdot h(X)^m\le\lambda(X)C⋅h(X)m≤λ(X) holds.

Formalizing it. The theorem is proved in the paper; to our knowledge no machine-checked proof exists. A formal proof requires a signed simplicial chain complex with explicit orientations, the adjoint relation between boundary and co-boundary, and a Rayleigh-quotient bound for a symmetric operator on an invariant subspace. These are the basic tools for any further formal work on spectral high-dimensional expansion, including the Mixing Lemma of the same paper (the companion mission of this series).

Difficulty

The graph proof plugs a two-valued test function into the Rayleigh quotient. In dimension ddd the test vector must be a (d−1)(d-1)(d−1)-cycle, and an indicator of a block is not one. The paper's form (4.1) assigns to a (d−1)(d-1)(d−1)-cell whose vertices meet ddd distinct blocks the size of the missing block, with the sign of a permutation of the blocks. Showing that this form is a cycle and that its co-boundary has absolute value exactly nnn on F(A0,…,Ad)F(A_0,\dots,A_d)F(A0​,…,Ad​) and 000 elsewhere is a case analysis over how the vertices of a cell fall into blocks, and every case depends on the orientation signs. A convention error in any of the operators or in the form makes one of these identities fail. A second, smaller difficulty is that λ(X)\lambda(X)λ(X) is a minimum over the spectrum on a subspace, so the Rayleigh bound must be proved for Δ+\Delta^+Δ+ restricted to Zd−1Z_{d-1}Zd−1​, which it preserves.

Formalization scope

  • Vertices are Fin n; a complex is a structure holding its ddd-cells as Finset (Finset (Fin n)), each of size d+1d+1d+1; the complete skeleton is built into the type. Complexes without ddd-cells are allowed.
  • Forms are EuclideanSpace ℝ over the subtype of kkk-element vertex sets, so no form is supported on sets of the wrong size. Ωd\Omega^dΩd is modelled on all (d+1)(d+1)(d+1)-element sets; ∂d∗\partial_d^*∂d∗​ vanishes off XdX^dXd and ∂d\partial_d∂d​ ignores values there.
  • Orientation is by the order of Fin n; the sign of vertex vvv in cell τ\tauτ is (−1)#{w∈τ:w<v}(-1)^{\#\{w\in\tau:w<v\}}(−1)#{w∈τ:w<v}. Boundary and co-boundary are both defined by their formulas; their adjointness is milestone 3.
  • The spectral gap is not defined by sInf. The goal states that some eigenvalue μ\muμ of Δ+\Delta^+Δ+ on Zd−1Z_{d-1}Zd−1​ (a nonzero cycle fff with Δ+f=μf\Delta^+f=\mu fΔ+f=μf) is at most the Cheeger ratio of every partition, which is equivalent to λ(X)≤h(X)\lambda(X)\le h(X)λ(X)≤h(X). A partition is a family A : Fin (d+1) → Finset (Fin n) of nonempty, pairwise disjoint sets covering the vertices.
  • Added hypotheses: d≥1d\ge1d≥1 (the Laplacians act on Ωd−1\Omega^{d-1}Ωd−1) and n≥d+1n\ge d+1n≥d+1 (presupposed by the paper, since hhh minimizes over partitions into d+1d+1d+1 nonempty sets; for n≤dn\le dn≤d the cycle space is 000).
  • Ruled out: forms supported off the ddd-element sets (they would be spurious cycles with eigenvalue 000), an eigenvalue set read through sInf (empty sets give 000), unsigned boundaries (for which ∂∂≠0\partial\partial\ne0∂∂=0), cocycles ker⁡∂d∗\ker\partial_d^*ker∂d∗​ in place of cycles ker⁡∂d−1\ker\partial_{d-1}ker∂d−1​ (on which Δ+\Delta^+Δ+ is zero), and arbitrary disjoint families in place of partitions (empty blocks give ratio 000).
  • Needed infrastructure: sign bookkeeping for faces of sorted finsets, the spectral theorem for symmetric operators on a finite-dimensional inner product space restricted to an invariant subspace (Mathlib's LinearMap.IsSymmetric), and counting cells by blocks of a partition. The chain-complex and adjointness lemmas are reusable in any formal development of simplicial Hodge theory; contributions there are welcome.

Selected references

  • O. Parzanchevski, R. Rosenthal, R. J. Tessler, Isoperimetric inequalities in simplicial complexes, Combinatorica 35 (2015). arXiv:1207.0638v3, doi:10.1007/s00493-014-3002-x
  • B. Eckmann, Harmonische Funktionen und Randwertaufgaben in einem Komplex, Comment. Math. Helv. 17 (1944), no. 1, 240–255.
  • N. Alon, V. D. Milman, λ₁, isoperimetric inequalities for graphs, and superconcentrators, J. Combin. Theory Ser. B 38 (1985), 73–88. doi:10.1016/0095-8956(85)90092-9
  • N. Linial, R. Meshulam, Homological connectivity of random 2-complexes, Combinatorica 26 (2006), 475–487. doi:10.1007/s00493-006-0027-9
  • A. Gundert, U. Wagner, On Laplacians of random complexes, Proceedings of the 2012 Symposium on Computational Geometry, ACM, 2012, 151–160.
  • M. Gromov, Singularities, expanders and topology of maps. Part 2: From combinatorics to topology via algebraic isoperimetry, Geom. Funct. Anal. 20 (2010), no. 2, 416–526.
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Optimization-Based Algorithms for Tensor Decompositions: Canonical Polyadic Decomposition, Decomposition in Rank-(Lr, Lr, 1) Terms, and a New Generalization 1: Block Structure of the Gramian JᴴJResearch Paper

Motivation

Tensor decompositions express a multiway array as a sum of simple terms. The canonical polyadic decomposition (CPD) writes an NNN-th order tensor T∈CI1×⋯×IN\mathcal T\in\mathbb C^{I_1\times\cdots\times I_N}T∈CI1​×⋯×IN​ as a sum of RRR outer products of vectors; block term decompositions replace each rank-one term by a term of higher multilinear rank. These models are used in signal processing, blind source separation and telecommunications, and are computed numerically by minimizing a least-squares misfit.

Sorber, Van Barel and De Lathauwer (SIAM J. Optim. 23(2), 2013) introduce the (rank-Lr∘L_r\circLr​∘ rank-1) block term decomposition (BTD), which contains both the CPD and the rank-(Lr,Lr,1)(L_r,L_r,1)(Lr​,Lr​,1) BTD as special cases, and develop optimization algorithms for it: nonlinear conjugate gradient and quasi-Newton methods built on the complex gradient, and Gauss–Newton and Levenberg–Marquardt methods built on the Jacobian. For the second family the central object is the Gramian JHJJ^{\mathrm H}JJHJ of the Jacobian JJJ of the residual. Theorem 4.5 of the paper gives its exact block structure, and that structure is what lets the methods run without ever forming JJJ.

Setting

Fix N=P+QN = P + QN=P+Q modes with dimensions I1,…,INI_1,\dots,I_NI1​,…,IN​, a number of terms RRR, and block sizes L1,…,LRL_1,\dots,L_RL1​,…,LR​; put R′=∑rLrR' = \sum_r L_rR′=∑r​Lr​. The BTD approximates T\mathcal TT by

∑r=1R(∑r′ar′(1)∘⋯∘ar′(P))∘(cr(1)∘⋯∘cr(Q)),\sum_{r=1}^R\Big(\sum_{r'} a^{(1)}_{r'}\circ\cdots\circ a^{(P)}_{r'}\Big)\circ\big(c^{(1)}_r\circ\cdots\circ c^{(Q)}_r\big),r=1∑R​(r′∑​ar′(1)​∘⋯∘ar′(P)​)∘(cr(1)​∘⋯∘cr(Q)​),

where the inner sum runs over the LrL_rLr​ columns of block rrr. Here A(p)=[a1(p)⋯aR′(p)]∈CIp×R′A^{(p)} = [a^{(p)}_1\cdots a^{(p)}_{R'}]\in\mathbb C^{I_p\times R'}A(p)=[a1(p)​⋯aR′(p)​]∈CIp​×R′ and C(q)=[c1(q)⋯cR(q)]∈CIP+q×RC^{(q)} = [c^{(q)}_1\cdots c^{(q)}_R]\in\mathbb C^{I_{P+q}\times R}C(q)=[c1(q)​⋯cR(q)​]∈CIP+q​×R.

The paper reads this as a structured CPD in R′R'R′ rank-one terms. The first PPP factor matrices are the A(p)A^{(p)}A(p), and the last QQQ are

A(P+q)=C(q)⋅E,A^{(P+q)} = C^{(q)}\cdot E,A(P+q)=C(q)⋅E,

where E=diag(11×L1,…,11×LR)∈RR×R′E = \mathrm{diag}(1_{1\times L_1},\dots,1_{1\times L_R})\in\mathbb R^{R\times R'}E=diag(11×L1​​,…,11×LR​​)∈RR×R′ copies column rrr of C(q)C^{(q)}C(q) into the LrL_rLr​ columns of block rrr. The residual tensor is

FBTD=∑c=1R′ac(1)∘⋯∘ac(N)−T,\mathcal F_{\mathrm{BTD}} = \sum_{c=1}^{R'} a^{(1)}_c\circ\cdots\circ a^{(N)}_c - \mathcal T,FBTD​=c=1∑R′​ac(1)​∘⋯∘ac(N)​−T,

and the unknowns are z=(vecA(1),…,vecA(P),vecC(1),…,vecC(Q))z = (\mathrm{vec}A^{(1)},\dots,\mathrm{vec}A^{(P)},\mathrm{vec}C^{(1)},\dots,\mathrm{vec}C^{(Q)})z=(vecA(1),…,vecA(P),vecC(1),…,vecC(Q)). The Jacobian J=∂ vec(FBTD)/∂zTJ = \partial\,\mathrm{vec}(\mathcal F_{\mathrm{BTD}})/\partial z^{\mathrm T}J=∂vec(FBTD​)/∂zT is the complex (holomorphic) derivative: FBTD\mathcal F_{\mathrm{BTD}}FBTD​ is a polynomial in zzz, not in zˉ\bar zzˉ.

Three auxiliary matrices enter the answer. The first is Wσ=∗m∉σA(m)HA(m)W^\sigma = \ast_{m\notin\sigma}A^{(m)\mathrm H}A^{(m)}Wσ=∗m∈/σ​A(m)HA(m), the Hadamard product of the Gramians of the factor matrices outside a mode set σ\sigmaσ, with entries wr1r2σw^\sigma_{r_1r_2}wr1​r2​σ​. The second is F(q)=E⊗IIP+qF^{(q)} = E\otimes\mathbb I_{I_{P+q}}F(q)=E⊗IIP+q​​, which satisfies vec(C(q)E)T=vec(C(q))TF(q)\mathrm{vec}(C^{(q)}E)^{\mathrm T} = \mathrm{vec}(C^{(q)})^{\mathrm T}F^{(q)}vec(C(q)E)T=vec(C(q))TF(q) (Proposition 4.1). The third is the block diagonal Σ=diag(II1R′,…,IIPR′,F(1),…,F(Q))\Sigma = \mathrm{diag}(\mathbb I_{I_1R'},\dots,\mathbb I_{I_PR'},F^{(1)},\dots,F^{(Q)})Σ=diag(II1​R′​,…,IIP​R′​,F(1),…,F(Q)).

Formalization targets

Goal: Theorem 4.5

For every tensor T\mathcal TT and every zzz,

JHJ=Σ⋅[Π(n1,n2)]n1,n2=1N⋅ΣT,J^{\mathrm H}J = \Sigma\cdot\big[\Pi^{(n_1,n_2)}\big]_{n_1,n_2=1}^N\cdot\Sigma^{\mathrm T},JHJ=Σ⋅[Π(n1​,n2​)]n1​,n2​=1N​⋅ΣT, Π(n1,n2)≜(∂ vecF∂ vec(A(n1))T)H(∂ vecF∂ vec(A(n2))T)={W{n}⊗IInn=n1=n2,[wr1r2{n1,n2} ar2(n1)ar1(n2)H]r1,r2otherwise.\Pi^{(n_1,n_2)} \triangleq \Big(\tfrac{\partial\,\mathrm{vec}\mathcal F}{\partial\,\mathrm{vec}(A^{(n_1)})^{\mathrm T}}\Big)^{\mathrm H}\Big(\tfrac{\partial\,\mathrm{vec}\mathcal F}{\partial\,\mathrm{vec}(A^{(n_2)})^{\mathrm T}}\Big) = \begin{cases}W^{\{n\}}\otimes\mathbb I_{I_n} & n=n_1=n_2,\\ \big[w^{\{n_1,n_2\}}_{r_1r_2}\,a^{(n_1)}_{r_2}a^{(n_2)\mathrm H}_{r_1}\big]_{r_1,r_2} & \text{otherwise.}\end{cases}Π(n1​,n2​)≜(∂vec(A(n1​))T∂vecF​)H(∂vec(A(n2​))T∂vecF​)={W{n}⊗IIn​​[wr1​r2​{n1​,n2​}​ar2​(n1​)​ar1​(n2​)H​]r1​,r2​​​n=n1​=n2​,otherwise.​

The goal has two parts, and both are required. The first is that the Gramian of the CPD Jacobian equals the explicit block matrix. The second is the factorization through Σ\SigmaΣ.

Milestones

  1. The columns of the CPD Jacobian are rank-one tensors: ∂F/∂air(n)=ar(1)∘⋯∘ei(n)∘⋯∘ar(N)\partial\mathcal F/\partial a^{(n)}_{ir} = a^{(1)}_r\circ\cdots\circ e^{(n)}_i\circ\cdots\circ a^{(N)}_r∂F/∂air(n)​=ar(1)​∘⋯∘ei(n)​∘⋯∘ar(N)​.
  2. Diagonal blocks: inner products wr1r2{n}δijw^{\{n\}}_{r_1r_2}\delta_{ij}wr1​r2​{n}​δij​, hence the block wr1r2{n}IInw^{\{n\}}_{r_1r_2}\mathbb I_{I_n}wr1​r2​{n}​IIn​​.
  3. Off-diagonal blocks: inner products wr1r2{n1,n2}air2(n1)ajr1(n2)‾w^{\{n_1,n_2\}}_{r_1r_2}a^{(n_1)}_{ir_2}\overline{a^{(n_2)}_{jr_1}}wr1​r2​{n1​,n2​}​air2​(n1​)​ajr1​(n2​)​​, hence the rank-one block wr1r2{n1,n2}ar2(n1)ar1(n2)Hw^{\{n_1,n_2\}}_{r_1r_2}a^{(n_1)}_{r_2}a^{(n_2)\mathrm H}_{r_1}wr1​r2​{n1​,n2​}​ar2​(n1​)​ar1​(n2​)H​.
  4. Proposition 4.1: the vec identity for C(q)EC^{(q)}EC(q)E and the chain rule (4.3b) for the Jacobian columns of C(q)C^{(q)}C(q).
  5. The blocks of JHJJ^{\mathrm H}JJHJ that involve some C(q)C^{(q)}C(q) are ΠF(q)T\Pi F^{(q)\mathrm T}ΠF(q)T, F(q)ΠF^{(q)}\PiF(q)Π and F(q1)ΠF(q2)TF^{(q_1)}\Pi F^{(q_2)\mathrm T}F(q1​)ΠF(q2​)T, i.e. JHJ=Σ (JCPDHJCPD) ΣTJ^{\mathrm H}J = \Sigma\,(J_{\mathrm{CPD}}^{\mathrm H}J_{\mathrm{CPD}})\,\Sigma^{\mathrm T}JHJ=Σ(JCPDH​JCPD​)ΣT.

Significance

With Theorem 4.5, JHJJ^{\mathrm H}JJHJ is determined by the factor matrices and the small Gramians A(n)HA(n)A^{(n)\mathrm H}A^{(n)}A(n)HA(n). For a hypercubical CPD this takes O(NR2)O(NR^2)O(NR2) extra memory instead of the O(N2R2I2)O(N^2R^2I^2)O(N2R2I2) of a dense Gramian. Theorem 4.6 of the paper then turns the same structure into a matrix–vector product in O(NR2I)O(NR^2I)O(NR2I) operations, which is what inexact Gauss–Newton and Levenberg–Marquardt steps solved by preconditioned conjugate gradients require. The block-diagonal part Π(n,n)=W{n}⊗I\Pi^{(n,n)} = W^{\{n\}}\otimes\mathbb IΠ(n,n)=W{n}⊗I also gives the block Jacobi preconditioner of the paper's §4.2. For the CPD, expressions for the Gramian were already studied in chemometrics (the paper cites G. Tomasi's 2006 thesis for this); Theorem 4.5 states the block structure in closed form and extends it to the structured BTD through Σ\SigmaΣ.

The result is proved in the paper. As far as a search of Prove2Me and Mathlib shows, nothing about CPD or BTD Jacobians has been formalized. This mission produces a machine-checked proof of the block structure, starting from an explicit model of the decomposition and an honest complex derivative. That model (outer products, the structured CPD, EEE, Σ\SigmaΣ, the Hadamard-Gramian products) can be reused for the paper's cogradient theorem and for other tensor algorithms.

Difficulty

The identity is finite-dimensional, but no single step reduces it to a known lemma. First, JJJ is a genuine derivative of a multilinear polynomial map in ∑nInR′\sum_n I_nR'∑n​In​R′ complex variables, so each entry has to be computed from the derivative of a sum of products. Second, JHJJ^{\mathrm H}JJHJ is a sum over all ∏nIn\prod_n I_n∏n​In​ multi-indices. Turning it into the product of Gramians in WσW^\sigmaWσ means exchanging a sum of products with a product of sums while one or two modes are held fixed, with the conjugates landing on crossed column indices (ar2(n1)a^{(n_1)}_{r_2}ar2​(n1​)​, aˉr1(n2)\bar a^{(n_2)}_{r_1}aˉr1​(n2​)​). Third, the structured factor matrices A(P+q)=C(q)EA^{(P+q)} = C^{(q)}EA(P+q)=C(q)E are not unknowns. The derivative with respect to C(q)C^{(q)}C(q) has to go through the chain rule and the vec–Kronecker identity, and Σ\SigmaΣ's rows and columns are indexed by different sets.

Formalization scope

All objects are defined in TensorBTD.Gramian.Setting, with the following conventions.

  • Modes and columns. The NNN modes are Fin P ⊕ Fin Q (mode ppp is Sum.inl (p-1) and mode P+qP+qP+q is Sum.inr (q-1)), so all indices are 0-based. The R′R'R′ columns are Σ r : Fin R, Fin (L r) in lexicographic order, which is the order of (3.5).
  • Tensors and residuals. A tensor is a function of the multi-index. The residual is defined entrywise as a sum of outer products. The paper's (3.8) is its mode-nnn unfolding.
  • Vectorization and Kronecker products. Vectorized indices are (column, row) pairs, Mathlib's column-major Matrix.vec. This is the paper's Definition 2.5 with its misprint (i+(j−1)J)(i+(j-1)J)(i+(j−1)J) corrected to (i+(j−1)I)(i+(j-1)I)(i+(j−1)I). Kronecker products are Mathlib's ⊗ₖ.
  • Jacobian. The Jacobian is defined column by column as the complex derivative deriv of t↦G(x+teβ)t\mapsto G(x+te_\beta)t↦G(x+teβ​) at 000. It is not defined by its closed form, and it is not a real derivative.
  • The unstructured CPD. Π(n1,n2)\Pi^{(n_1,n_2)}Π(n1​,n2​) differentiates with respect to A(n)A^{(n)}A(n) for every nnn, including n>Pn>Pn>P, where A(n)A^{(n)}A(n) is not an unknown. It is therefore taken as the Jacobian of the unstructured CPD residual in R′R'R′ terms, with all NNN factor matrices free, evaluated at the factor matrices of zzz. This is how the paper's proof uses it.

There are no hypotheses. The paper's assumptions that P,Q≥1P, Q\ge 1P,Q≥1 and its qualifiers "nonzero" and "rank-LrL_rLr​" are not used in Section 4, so they are dropped. This is a generalization: Q=0Q = 0Q=0 gives the plain CPD in R′R'R′ terms.

A goal that took the closed form of Π\PiΠ as the definition, or that defined JJJ entrywise by the outer-product formula of milestone 1, would only state a sum identity. Both are ruled out: JJJ is a derivative, and the goal asserts that the Gramian of the CPD Jacobian equals the closed form. A misprint in the proof's closing paragraph, F(q)Π(p,P+q)F^{(q)}\Pi^{(p,P+q)}F(q)Π(p,P+q) for the (P+q,p)(P+q,p)(P+q,p) block, is corrected in Lean to F(q)Π(P+q,p)F^{(q)}\Pi^{(P+q,p)}F(q)Π(P+q,p).

Useful Mathlib infrastructure includes Matrix.vec, Matrix.kroneckerMap, Matrix.blockDiagonal', Finset.prod_univ_sum and the derivative rules for finite products (HasDerivAt.finset_prod). General lemmas welcome as contributions: derivatives of multilinear maps along coordinate directions, the sum–product exchange over Fintype.piFinset, and the chain rule for a Jacobian composed with a linear map.

Selected references

  • L. Sorber, M. Van Barel, L. De Lathauwer, Optimization-Based Algorithms for Tensor Decompositions: Canonical Polyadic Decomposition, Decomposition in Rank-(Lr,Lr,1)(L_r,L_r,1)(Lr​,Lr​,1) Terms, and a New Generalization, SIAM J. Optim. 23(2), 695–720, 2013. https://doi.org/10.1137/120868323
  • T. G. Kolda, B. W. Bader, Tensor Decompositions and Applications, SIAM Review 51(3), 455–500, 2009. https://doi.org/10.1137/07070111X
  • L. De Lathauwer, Decompositions of a Higher-Order Tensor in Block Terms — Part II: Definitions and Uniqueness, SIAM J. Matrix Anal. Appl. 30(3), 1033–1066, 2008. https://doi.org/10.1137/070690729
  • L. Sorber, M. Van Barel, L. De Lathauwer, Unconstrained Optimization of Real Functions in Complex Variables, SIAM J. Optim. 22(3), 879–898, 2012. https://doi.org/10.1137/110832124
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Distance Covariance in Metric Spaces 2: Without Negative Type Some Law Has Negative Distance Covariance, and Without Strong Negative Type Some Non-Product Law Has ZeroResearch Paper

Motivation

Distance covariance was introduced by Székely, Rizzo and Bakirov (2007) as a measure of dependence between random vectors in Euclidean spaces: it is zero exactly when the vectors are independent, and its empirical version gives a consistent test of independence that needs no moment beyond the first. Lyons (2013) asked for which metric spaces the same holds. His Theorem 3.11 shows that it holds whenever both spaces have strong negative type. This mission formalizes the complementary result, Proposition 3.15 of the same paper: the hypothesis on the space cannot be removed. Without negative type, distance covariance can even be negative; without strong negative type, it can vanish on a law that is not a product. Together with Theorem 3.11, the proposition locates the boundary of metric spaces on which distance covariance is a valid test of independence.

Timeline. 2007: Székely, Rizzo and Bakirov define distance covariance on Rp×Rq\mathbb R^p\times\mathbb R^qRp×Rq and prove the independence characterization there. 2013: Lyons extends the theory to metric spaces of negative type, characterizes the spaces where it remains a test of independence as those of strong negative type, and proves Proposition 3.15. 2018 and 2021: two errata by the author correct several statements of the paper; the first of them adds the standing assumption that all metric spaces are separable. Proposition 3.15 is not affected by the corrections.

Setting

Let (X,d)(\mathcal X,d)(X,d) and (Y,d)(\mathcal Y,d)(Y,d) be separable metric spaces, each with its Borel σ\sigmaσ-field. A finite Borel measure μ\muμ on X\mathcal XX has a finite first moment if ∫d(o,x) dμ(x)<∞\int d(o,x)\,d\mu(x)<\infty∫d(o,x)dμ(x)<∞ for some point ooo. For such μ\muμ put

aμ(x):=∫d(x,x′) dμ(x′),D(μ):=∫d(x,x′) dμ2(x,x′),a_\mu(x):=\int d(x,x')\,d\mu(x'),\qquad D(\mu):=\int d(x,x')\,d\mu^2(x,x'),aμ​(x):=∫d(x,x′)dμ(x′),D(μ):=∫d(x,x′)dμ2(x,x′),

and define the doubly centred distance dμ(x,x′):=d(x,x′)−aμ(x)−aμ(x′)+D(μ)d_\mu(x,x'):=d(x,x')-a_\mu(x)-a_\mu(x')+D(\mu)dμ​(x,x′):=d(x,x′)−aμ​(x)−aμ​(x′)+D(μ). For two probability measures μ1,μ2\mu_1,\mu_2μ1​,μ2​ with finite first moments, D(μ1−μ2)D(\mu_1-\mu_2)D(μ1​−μ2​) is the energy of their difference,

D(μ1−μ2)=∬d dμ12−2∬d d(μ1×μ2)+∬d dμ22.D(\mu_1-\mu_2)=\iint d\,d\mu_1^2-2\iint d\,d(\mu_1\times\mu_2)+\iint d\,d\mu_2^2 .D(μ1​−μ2​)=∬ddμ12​−2∬dd(μ1​×μ2​)+∬ddμ22​.

Let θ\thetaθ be a Borel probability measure on X×Y\mathcal X\times\mathcal YX×Y whose marginals μ\muμ on X\mathcal XX and ν\nuν on Y\mathcal YY have finite first moments. Its distance covariance is

dcov⁡(θ):=∫dμ(x,x′) dν(y,y′) dθ2((x,y),(x′,y′)).\operatorname{dcov}(\theta):=\int d_\mu(x,x')\,d_\nu(y,y')\,d\theta^2\big((x,y),(x',y')\big).dcov(θ):=∫dμ​(x,x′)dν​(y,y′)dθ2((x,y),(x′,y′)).

θ\thetaθ is a product measure if θ=μ×ν\theta=\mu\times\nuθ=μ×ν.

X\mathcal XX has negative type if for every nnn, all points x1,…,xnx_1,\dots,x_nx1​,…,xn​ and all reals α1,…,αn\alpha_1,\dots,\alpha_nα1​,…,αn​ with ∑iαi=0\sum_i\alpha_i=0∑i​αi​=0,

∑i,j≤nαiαj d(xi,xj)≤0.(3.1)\sum_{i,j\le n}\alpha_i\alpha_j\,d(x_i,x_j)\le 0. \tag{3.1}i,j≤n∑​αi​αj​d(xi​,xj​)≤0.(3.1)

On such a space D(μ1−μ2)≤0D(\mu_1-\mu_2)\le 0D(μ1​−μ2​)≤0 for all probability measures with finite first moments, and X\mathcal XX has strong negative type if moreover equality holds only when μ1=μ2\mu_1=\mu_2μ1​=μ2​. Write δ(y)\delta(y)δ(y) for the point mass at yyy.

Formalization targets

Goal: Proposition 3.15

Let Y\mathcal YY have at least two points.

  1. If X\mathcal XX is not of negative type, there is a probability measure θ\thetaθ on X×Y\mathcal X\times\mathcal YX×Y whose marginals have finite first moments and
dcov⁡(θ)<0.\operatorname{dcov}(\theta)<0.dcov(θ)<0.
  1. If X\mathcal XX is not of strong negative type, there is a probability measure θ\thetaθ on X×Y\mathcal X\times\mathcal YX×Y whose marginals have finite first moments, with
dcov⁡(θ)=0andθ≠μ×ν.\operatorname{dcov}(\theta)=0\quad\text{and}\quad \theta\neq\mu\times\nu .dcov(θ)=0andθ=μ×ν.

The space Y\mathcal YY is arbitrary apart from having two points, so the statement fixes nothing about it.

Milestones (all from the proof on p. 17)

  1. For probability measures μ1,μ2\mu_1,\mu_2μ1​,μ2​ with finite first moments and y1≠y2y_1\ne y_2y1​=y2​, the law θ=(μ1×δ(y1)+μ2×δ(y2))/2\theta=\big(\mu_1\times\delta(y_1)+\mu_2\times\delta(y_2)\big)/2θ=(μ1​×δ(y1​)+μ2​×δ(y2​))/2 has dcov⁡(θ)=−d(y1,y2) D(μ1−μ2)/8\operatorname{dcov}(\theta)=-d(y_1,y_2)\,D(\mu_1-\mu_2)/8dcov(θ)=−d(y1​,y2​)D(μ1​−μ2​)/8.
  2. If X\mathcal XX is not of negative type, there are probability measures μ1≠μ2\mu_1\neq\mu_2μ1​=μ2​ with finite first moments and D(μ1−μ2)>0D(\mu_1-\mu_2)>0D(μ1​−μ2​)>0.
  3. If x1≠x2x_1\neq x_2x1​=x2​ then D(δ(x1)−δ(x2))<0D(\delta(x_1)-\delta(x_2))<0D(δ(x1​)−δ(x2​))<0.
  4. If D(μ1−μ2)≥0D(\mu_1-\mu_2)\ge 0D(μ1​−μ2​)≥0 and x1≠x2x_1\ne x_2x1​=x2​, some γ∈(0,1]\gamma\in(0,1]γ∈(0,1] makes τi:=γμi+(1−γ)δ(xi)\tau_i:=\gamma\mu_i+(1-\gamma)\delta(x_i)τi​:=γμi​+(1−γ)δ(xi​) satisfy D(τ1−τ2)=0D(\tau_1-\tau_2)=0D(τ1​−τ2​)=0.
  5. For μ1≠μ2\mu_1\ne\mu_2μ1​=μ2​ with D(μ1−μ2)≥0D(\mu_1-\mu_2)\ge0D(μ1​−μ2​)≥0, x1≠x2x_1\ne x_2x1​=x2​, γ∈(0,1]\gamma\in(0,1]γ∈(0,1] and y1≠y2y_1\ne y_2y1​=y2​, the law (τ1×δ(y1)+τ2×δ(y2))/2\big(\tau_1\times\delta(y_1)+\tau_2\times\delta(y_2)\big)/2(τ1​×δ(y1​)+τ2​×δ(y2​))/2 is not a product measure.

Significance

The result. Theorem 3.11 of the paper shows that strong negative type of both spaces suffices for dcov⁡(θ)=0\operatorname{dcov}(\theta)=0dcov(θ)=0 to characterize independence. Proposition 3.15 shows the hypothesis on each factor is necessary: a single failure of (3.1) already produces a law with negative distance covariance, so dcov⁡\operatorname{dcov}dcov is not even a nonnegative quantity there, and a single pair of distinct laws with D(μ1−μ2)=0D(\mu_1-\mu_2)=0D(μ1​−μ2​)=0 produces a dependent law that the test cannot detect. Consequently, any use of distance covariance on general metric data (graphs, ℓp\ell^pℓp spaces with p>2p>2p>2, spaces of distributions under Wasserstein metrics) has to verify strong negative type first. Since the two-point space Y\mathcal YY is arbitrary, the failure is a property of X\mathcal XX alone.

Formalizing it. The proposition is proved in the paper; no machine-checked proof of it, or of any result about distance covariance, is known to exist. The mission produces a formal definition of distance covariance on separable metric spaces, of negative and strong negative type in the paper's measure-theoretic form, and the computation of dcov⁡\operatorname{dcov}dcov on two-point mixtures. These are the same objects as in the sibling mission on Theorem 3.11, so the two together give a formal account of when distance covariance characterizes independence.

Difficulty

The step the paper calls "a little algebra" is the bulk of the work: dcov⁡\operatorname{dcov}dcov is a four-fold integral of a product of doubly centred distances, each of which is itself built from integrals against a marginal of θ\thetaθ, and every manipulation of it happens inside Bochner integrals over product measures whose integrability has to be derived from first moments alone. In a formal setting nothing about these integrals is automatic. The passage from a violation of the finite-sum condition (3.1) to two probability measures with D(μ1−μ2)>0D(\mu_1-\mu_2)>0D(μ1​−μ2​)>0 is left implicit in the paper. The non-product claim also uses a fact the page does not state: that τ1≠τ2\tau_1\neq\tau_2τ1​=τ2​, which follows from D(μ1−μ2)≥0D(\mu_1-\mu_2)\ge 0D(μ1​−μ2​)≥0 and is false without it.

Formalization scope

All metric spaces carry their Borel σ\sigmaσ-field and are assumed second countable, which for metric spaces is separability; this is the author's own correction, Errata (i), which makes ddd measurable on the product. Measures are Mathlib measures with values in [0,∞][0,\infty][0,∞]; mixture weights such as γ\gammaγ, 1−γ1-\gamma1−γ and 1/21/21/2 enter as extended nonnegative reals, and γ\gammaγ is always restricted to (0,1](0,1](0,1]. Because Mathlib's Bochner integral does not integrate against signed measures, D(μ1−μ2)D(\mu_1-\mu_2)D(μ1​−μ2​) is defined as the bilinear energy expansion displayed above. "Not a product measure" means θ\thetaθ differs from the product of its own marginals, never from some other product.

Several formalizations of this statement would be trivially true and are excluded. A Bochner integral of a non-integrable function is 000 in Lean, so every statement either assumes or concludes the finite first moments that make dcov⁡\operatorname{dcov}dcov and DDD genuine integrals. Negative type is the finite-sum condition (3.1) and strong negative type the measure condition of p. 11, never an embedding property. The product condition is tested against θ\thetaθ's own marginals, not against free factors. Y\mathcal YY is quantified before θ\thetaθ is chosen, and part 2's hypothesis is the full negation of strong negative type, which includes spaces of negative type.

A complete development needs integrability of dμ dνd_\mu\,d_\nudμ​dν​ under θ2\theta^2θ2 from first moments (Lemma 2.1 of the paper), linearity of the energy in each measure, push-forwards of mixtures of product measures, and the intermediate value theorem. The integrability and energy-bilinearity lemmas are reusable for any work on energy distance or distance covariance. Contributions of these general lemmas, as well as of proofs of the individual milestones, are welcome.

Selected references

  • R. Lyons, Distance covariance in metric spaces, Ann. Probab. 41 (2013), 3284–3305, https://doi.org/10.1214/12-AOP803; author's version arXiv:1106.5758 (version of 19 Dec. 2020, with errata). https://arxiv.org/abs/1106.5758
  • R. Lyons, Errata to "Distance covariance in metric spaces", Ann. Probab. 46 (2018), 2400–2405; reproduced as pp. 24–29 of arXiv:1106.5758 (version of 19 Dec. 2020). https://arxiv.org/abs/1106.5758
  • R. Lyons, Second errata to "Distance covariance in metric spaces", Ann. Probab. 49 (2021), 2668–2670; reproduced as pp. 30–32 of arXiv:1106.5758 (version of 19 Dec. 2020). https://arxiv.org/abs/1106.5758
  • G. J. Székely, M. L. Rizzo, N. K. Bakirov, Measuring and testing dependence by correlation of distances, Ann. Statist. 35 (2007), 2769–2794. https://doi.org/10.1214/009053607000000505
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Distance Covariance in Metric Spaces 3: Every Separable Hilbert Space Has Strong Negative TypeResearch Paper

Motivation

Distance covariance is a statistic for testing whether two random variables are independent. Székely, Rizzo and Bakirov introduced it for Euclidean spaces (Ann. Statist. 2007): the population distance covariance of a joint law θ\thetaθ is 000 exactly when θ\thetaθ is a product measure, so a consistent test of independence follows. Lyons (arXiv:1106.5758) extended the statistic to arbitrary metric spaces and showed that the characterization of independence holds on a pair of metric spaces precisely when both have strong negative type (his Theorem 3.11 and Proposition 3.15). That makes strong negative type the property a statistician has to check before using distance covariance on a given space. Functional data, the main case in practice, live in Hilbert spaces.

This mission formalizes Lyons's Theorem 3.16: every separable Hilbert space is of strong negative type. Kosorok (2009, cited by Lyons) had asked whether the characterization of independence extends to Hilbert spaces.

Timeline.

  • 1935–1938: Schoenberg shows that a metric space has negative type exactly when its distance is the squared distance of a subset of a Hilbert space (Trans. AMS 1938).
  • 1982 and 1986: Koldobskiĭ (Theorem 1) and Linde (Theorem 6), as cited by Lyons, prove results on positive definite functions and stable measures in Banach spaces from which Theorem 3.16 follows, together with its analogue for separable LpL^pLp, 1<p<21<p<21<p<2.
  • 2007: Székely, Rizzo and Bakirov treat the Euclidean case.
  • 2013: Lyons gives a direct proof of Theorem 3.16 through a Gaussian version of the Crofton embedding.
  • 2018: the first Errata (Ann. Probab. 46) supply the justification of a continuity claim at the end of that proof (Errata (x)). They also note that Hilbert spaces were tacitly assumed real (Errata (viii)).

Setting

Let (X,d)(\mathscr X,d)(X,d) be a separable metric space with its Borel σ\sigmaσ-field. A Borel probability measure μ\muμ has a finite first moment if ∫d(o,x) dμ(x)<∞\int d(o,x)\,d\mu(x)<\infty∫d(o,x)dμ(x)<∞ for some o∈Xo\in\mathscr Xo∈X. For two such measures write E(μ1,μ2)=∬d(x,x′) dμ1(x) dμ2(x′)E(\mu_1,\mu_2)=\iint d(x,x')\,d\mu_1(x)\,d\mu_2(x')E(μ1​,μ2​)=∬d(x,x′)dμ1​(x)dμ2​(x′) and

D(μ1−μ2)=E(μ1,μ1)−2E(μ1,μ2)+E(μ2,μ2),D(\mu_1-\mu_2)=E(\mu_1,\mu_1)-2E(\mu_1,\mu_2)+E(\mu_2,\mu_2),D(μ1​−μ2​)=E(μ1​,μ1​)−2E(μ1​,μ2​)+E(μ2​,μ2​),

the integral of ddd against the square of the signed measure μ1−μ2\mu_1-\mu_2μ1​−μ2​.

The space has negative type if, for all nnn, all x1,…,xn∈Xx_1,\dots,x_n\in\mathscr Xx1​,…,xn​∈X and all real α1,…,αn\alpha_1,\dots,\alpha_nα1​,…,αn​ with ∑iαi=0\sum_i\alpha_i=0∑i​αi​=0,

∑i,j≤nαiαj d(xi,xj)≤0.(3.1)\sum_{i,j\le n}\alpha_i\alpha_j\,d(x_i,x_j)\le0. \tag{3.1}i,j≤n∑​αi​αj​d(xi​,xj​)≤0.(3.1)

By approximation, negative type gives D(μ1−μ2)≤0D(\mu_1-\mu_2)\le0D(μ1​−μ2​)≤0 for all probability measures with finite first moments. The space has strong negative type if it has negative type and D(μ1−μ2)=0D(\mu_1-\mu_2)=0D(μ1​−μ2​)=0 only when μ1=μ2\mu_1=\mu_2μ1​=μ2​. Strict negative type is the same condition restricted to finitely supported measures.

The proof works on ℓ2(Z+)\ell^2(\mathbb Z^+)ℓ2(Z+) and uses the following objects. ρ\rhoρ is the law on R∞\mathbb R^\inftyR∞ of an IID standard normal sequence Z1,Z2,…Z_1,Z_2,\dotsZ1​,Z2​,…; λ\lambdaλ is Lebesgue measure on R\mathbb RR; c=E∣Z1∣c=\mathbf E|Z_1|c=E∣Z1​∣. For w,u∈R∞w,u\in\mathbb R^\inftyw,u∈R∞ put w(u)=lim sup⁡N∑n≤Nunwnw(u)=\limsup_N\sum_{n\le N}u_nw_nw(u)=limsupN​∑n≤N​un​wn​. The Gaussian Crofton embedding sends uuu to the function

ϕ(u)(w,s)=1[w(u)/c,∞)(s)−1[0,∞)(s)\phi(u)(w,s)=\mathbf 1_{[w(u)/c,\infty)}(s)-\mathbf 1_{[0,\infty)}(s)ϕ(u)(w,s)=1[w(u)/c,∞)​(s)−1[0,∞)​(s)

on R∞×R\mathbb R^\infty\times\mathbb RR∞×R. For probability measures μ1,μ2\mu_1,\mu_2μ1​,μ2​ on ℓ2\ell^2ℓ2, its barycenter at μ=μ1−μ2\mu=\mu_1-\mu_2μ=μ1​−μ2​ is the function βϕ(μ)(w,s)=μ{u ; w(u)≤cs}\beta_\phi(\mu)(w,s)=\mu\{u\,;\,w(u)\le cs\}βϕ​(μ)(w,s)=μ{u;w(u)≤cs}.

Formalization targets

Goal: Theorem 3.16

H a separable real Hilbert space ⟹ H is of strong negative type.H \text{ a separable real Hilbert space}\ \Longrightarrow\ H \text{ is of strong negative type.}H a separable real Hilbert space ⟹ H is of strong negative type.

Milestones, in the order the proof uses them

  1. Z(u)=∑unZnZ(u)=\sum u_nZ_nZ(u)=∑un​Zn​ converges ρ\rhoρ-a.s., is centered normal with variance ∥u∥22\|u\|_2^2∥u∥22​, and E∣Z(u)∣=c∥u∥2\mathbf E|Z(u)|=c\|u\|_2E∣Z(u)∣=c∥u∥2​ (p. 18).
  2. The isometry ∥ϕ(u)−ϕ(u′)∥22=∥ϕ(u)−ϕ(u′)∥1=∥u−u′∥2\|\phi(u)-\phi(u')\|_2^2=\|\phi(u)-\phi(u')\|_1=\|u-u'\|_2∥ϕ(u)−ϕ(u′)∥22​=∥ϕ(u)−ϕ(u′)∥1​=∥u−u′∥2​ (p. 18).
  3. Every Hilbert space has negative type, indeed strict negative type (p. 18).
  4. D(μ1−μ2)=−2∫βϕ(μ1−μ2)2 d(ρ×λ)D(\mu_1-\mu_2)=-2\int\beta_\phi(\mu_1-\mu_2)^2\,d(\rho\times\lambda)D(μ1​−μ2​)=−2∫βϕ​(μ1​−μ2​)2d(ρ×λ): identity (3.4) for the Gaussian embedding (pp. 11, 18).
  5. The Cramér–Wold reduction: agreement of μi{⟨u,v⟩≤s}\mu_i\{\langle u,v\rangle\le s\}μi​{⟨u,v⟩≤s} for all finitely supported vvv forces μ1=μ2\mu_1=\mu_2μ1​=μ2​ (p. 18).
  6. If βϕ(μ)=0\beta_\phi(\mu)=0βϕ​(μ)=0 holds ρ×λ\rho\times\lambdaρ×λ-a.e., then for ρ\rhoρ-a.e. www it vanishes at ((v,w),s)((v,w),s)((v,w),s) for all v∈RKv\in\mathbb R^Kv∈RK and s∈Rs\in\mathbb Rs∈R (p. 19; Errata (x)).
  7. If the conclusion of 6 holds for every KKK, then μ1[⟨u≤L,v⟩≤s]=μ2[⟨u≤L,v⟩≤s]\mu_1[\langle u_{\le L},v\rangle\le s]=\mu_2[\langle u_{\le L},v\rangle\le s]μ1​[⟨u≤L​,v⟩≤s]=μ2​[⟨u≤L​,v⟩≤s] for all LLL, vvv, sss (p. 19).

The goal has no constants. Each milestone states a claim of the paper in the paper's strength.

Significance

The result. With Theorem 3.11, Theorem 3.16 shows that for random elements of separable Hilbert spaces, zero distance covariance is equivalent to independence. Distance-covariance tests are therefore consistent for curves, images and other functional data. It also yields Corollary 3.18: if (X,d)(\mathscr X,d)(X,d) is a separable metric space of negative type, then (X,d1/2)(\mathscr X,d^{1/2})(X,d1/2) has strong negative type, so a test of independence is available on every separable space of negative type after a change of metric. Remark 3.17 shows that separability cannot simply be dropped: a non-separable Hilbert space is of strong negative type exactly when its dimension is a cardinal of measure zero.

The formalization. The theorem is proved, and to our knowledge no proof of it, or of negative type of Hilbert spaces, is machine-checked. A complete development needs four things:

  • the Gaussian series on ℓ2\ell^2ℓ2, built from Mathlib's Measure.infinitePi and gaussianReal;
  • an L1L^1L1/L2L^2L2 isometry for a Crofton-type embedding;
  • the identity between the energy distance and a squared barycenter norm;
  • the fact that a finite Borel measure on ℓ2\ell^2ℓ2 is determined by its one-dimensional projections.

Each of these is reusable outside distance covariance: the first in Gaussian measure theory, the last whenever laws on sequence spaces are compared.

Difficulty

The first idea is to approximate. Euclidean spaces have strict negative type, finite-dimensional projections of a Hilbert space are Euclidean, and probability measures are limits of finitely supported ones. Approximation preserves the inequality D(μ1−μ2)≤0D(\mu_1-\mu_2)\le0D(μ1​−μ2​)≤0, but it does not preserve the equality case. A limit of strictly negative quantities may be 000 even though μ1≠μ2\mu_1\neq\mu_2μ1​=μ2​. Remark 3.3 of the paper exhibits a space of strict but not strong negative type, so this gap is real.

The second idea is to transport the finite-dimensional Crofton embedding, in which ∥x−y∥\|x-y\|∥x−y∥ is the measure of half-spaces separating xxx and yyy. It fails because ℓ2\ell^2ℓ2 has no rotation-invariant Lebesgue measure on its half-spaces. The Gaussian measure ρ\rhoρ replaces it. But w(u)w(u)w(u) is defined only ρ\rhoρ-almost surely, and its exceptional set depends on uuu. As a result, "βϕ(μ)=0\beta_\phi(\mu)=0βϕ​(μ)=0 almost everywhere" does not immediately give information for every direction vvv and level sss. That passage from almost every (v,s)(v,s)(v,s) to every (v,s)(v,s)(v,s) is the step the 2018 Errata had to justify.

Formalization scope

Lean conventions, all disclosed in the items:

  • Spaces. A Hilbert space is a real InnerProductSpace ℝ H with CompleteSpace H, as Errata (viii) prescribes; a complex space has the distances of its realification. Separability is SecondCountableTopology, which matches the standing separability of Errata (i). ℓ2(Z+)\ell^2(\mathbb Z^+)ℓ2(Z+) is lp (fun _ : ℕ => ℝ) 2 with the Borel σ\sigmaσ-field, declared in the Setting file because Mathlib supplies none.
  • Indices start at 000.
  • The energy term. D(μ1−μ2)D(\mu_1-\mu_2)D(μ1​−μ2​) is the three-term energy expansion, since Mathlib does not integrate against signed measures. A signed measure μ1−μ2\mu_1-\mu_2μ1​−μ2​ is always handled through the pair (μ1,μ2)(\mu_1,\mu_2)(μ1​,μ2​).
  • Junk values. lim sup⁡\limsuplimsup is taken in R\mathbb RR, so its junk value on divergent sequences lives on a ρ\rhoρ-null set; statements about w(u)w(u)w(u) are made ρ\rhoρ-a.e. or under integrals. ccc is the integral ∫∣z∣ dN(0,1)\int|z|\,dN(0,1)∫∣z∣dN(0,1). ϕ(u)\phi(u)ϕ(u) is a plain function, and Lp(ρ×λ)L^p(\rho\times\lambda)Lp(ρ×λ) norms are written as integrals, with integrability asserted alongside each one.

Trivializing encodings are ruled out:

  • negative and strong negative type are defined by (3.1) and the equality case of (3.3), never through an embedding or the injectivity of a barycenter map;
  • every item about DDD carries finite-first-moment hypotheses, so no integral silently takes the junk value 000.

Contributions are welcome on any milestone. The reduction of a general separable HHH to ℓ2(Z+)\ell^2(\mathbb Z^+)ℓ2(Z+) (by an isometry onto a closed subspace) is not posed separately and belongs to the goal's proof. Mathlib's Measure.ext_of_charFun, for finite measures on complete second-countable real inner product spaces, is a natural tool for milestone 5. Separability of lp is not yet an instance in Mathlib.

Selected references

  • R. Lyons, Distance covariance in metric spaces, Ann. Probab. 41 (2013), 3284–3305; Errata, Ann. Probab. 46 (2018), 2400–2405; Second Errata, Ann. Probab. 49 (2021), 2668–2670. Author's version of 19 Dec. 2020, including both errata: https://arxiv.org/abs/1106.5758
  • G. J. Székely, M. L. Rizzo, N. K. Bakirov, Measuring and testing dependence by correlation of distances, Ann. Statist. 35 (2007), 2769–2794. https://doi.org/10.1214/009053607000000505
  • I. J. Schoenberg, Metric spaces and positive definite functions, Trans. Amer. Math. Soc. 44 (1938), 522–536. https://doi.org/10.1090/S0002-9947-1938-1501980-0
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Functional AnalysisProbabilityStatistics·Captain: mikedeng1

Distance Covariance in Metric Spaces 1: On Spaces of Strong Negative Type, Zero Distance Covariance Forces a Product MeasureResearch Paper

Motivation

Testing whether two random quantities are independent is one of the basic tasks of statistics. Classical correlation only detects linear dependence. Distance covariance, introduced by Székely, Rizzo and Bakirov (Ann. Statist. 2007) for random vectors in Euclidean spaces, is a dependence measure that vanishes exactly under independence. It only needs the distances between sample points, and its empirical version is a simple V-statistic. These properties made it a standard tool for nonparametric independence testing.

Lyons (Ann. Probab. 41 (2013), arXiv:1106.5758) asked in which metric spaces this characterization of independence survives. The answer is the class of metric spaces of strong negative type, which includes all separable Hilbert spaces. On such spaces, distance covariance gives a test of independence that is consistent against every alternative. This mission formalizes that result, Theorem 3.11 of the paper, together with the chain of results its proof rests on.

Timeline. Schoenberg (1937, 1938) characterized metric spaces of negative type by isometric embeddings of (X,d1/2)(\mathcal X,d^{1/2})(X,d1/2) into Hilbert space. Székely, Rizzo and Bakirov (2007) defined distance covariance on Rp×Rq\mathbb R^p\times\mathbb R^qRp×Rq and proved that it vanishes only under independence. Lyons (2013) extended the theory to general metric spaces and identified strong negative type as the exact condition. The Errata (Ann. Probab. 46 (2018), 2400–2405; included in arXiv:1106.5758, pp. 24–29) added a standing separability assumption and repaired a gap in Lemma 3.8. The Second Errata appeared in Ann. Probab. 49 (2021).

Setting

Let (X,d)(\mathcal X,d)(X,d) and (Y,d)(\mathcal Y,d)(Y,d) be separable metric spaces with their Borel σ\sigmaσ-fields. A finite measure μ\muμ on X\mathcal XX has a finite first moment if ∫d(o,x) dμ(x)<∞\int d(o,x)\,d\mu(x)<\infty∫d(o,x)dμ(x)<∞ for some (equivalently every) o∈Xo\in\mathcal Xo∈X. For such μ\muμ define

aμ(x)=∫d(x,x′) dμ(x′),D(μ)=∫d(x,x′) dμ2(x,x′),a_\mu(x)=\int d(x,x')\,d\mu(x'),\qquad D(\mu)=\int d(x,x')\,d\mu^2(x,x'),aμ​(x)=∫d(x,x′)dμ(x′),D(μ)=∫d(x,x′)dμ2(x,x′), dμ(x,x′)=d(x,x′)−aμ(x)−aμ(x′)+D(μ).d_\mu(x,x')=d(x,x')-a_\mu(x)-a_\mu(x')+D(\mu).dμ​(x,x′)=d(x,x′)−aμ​(x)−aμ​(x′)+D(μ).

For a probability measure θ\thetaθ on X×Y\mathcal X\times\mathcal YX×Y whose marginals μ\muμ and ν\nuν have finite first moments, the distance covariance is

dcov⁡(θ)=∫dμ(x,x′) dν(y,y′) dθ2((x,y),(x′,y′)).\operatorname{dcov}(\theta)=\int d_\mu(x,x')\,d_\nu(y,y')\,d\theta^2\big((x,y),(x',y')\big).dcov(θ)=∫dμ​(x,x′)dν​(y,y′)dθ2((x,y),(x′,y′)).

θ\thetaθ is a product measure if θ=μ×ν\theta=\mu\times\nuθ=μ×ν.

(X,d)(\mathcal X,d)(X,d) has negative type if ∑i,j≤nαiαjd(xi,xj)≤0\sum_{i,j\le n}\alpha_i\alpha_j d(x_i,x_j)\le0∑i,j≤n​αi​αj​d(xi​,xj​)≤0 for all nnn, all points x1,…,xnx_1,\dots,x_nx1​,…,xn​ and all real weights with ∑iαi=0\sum_i\alpha_i=0∑i​αi​=0. For finite measures μ1,μ2\mu_1,\mu_2μ1​,μ2​ with finite first moments, D(μ1−μ2)D(\mu_1-\mu_2)D(μ1​−μ2​) is the integral of ddd against (μ1−μ2)2(\mu_1-\mu_2)^2(μ1​−μ2​)2. On spaces of negative type D(μ1−μ2)≤0D(\mu_1-\mu_2)\le0D(μ1​−μ2​)≤0 for probability measures μ1,μ2\mu_1,\mu_2μ1​,μ2​. The space has strong negative type if, in addition, D(μ1−μ2)=0D(\mu_1-\mu_2)=0D(μ1​−μ2​)=0 only when μ1=μ2\mu_1=\mu_2μ1​=μ2​.

An embedding is a map ϕ:X→H\phi:\mathcal X\to Hϕ:X→H into a real Hilbert space with d(x,x′)=∥ϕ(x)−ϕ(x′)∥2d(x,x')=\|\phi(x)-\phi(x')\|^2d(x,x′)=∥ϕ(x)−ϕ(x′)∥2. Its barycenter map is βϕ(μ)=∫ϕ dμ\beta_\phi(\mu)=\int\phi\,d\muβϕ​(μ)=∫ϕdμ. The tensor embedding (x,y)↦ϕ(x)⊗ψ(y)(x,y)\mapsto\phi(x)\otimes\psi(y)(x,y)↦ϕ(x)⊗ψ(y) takes values in the Hilbert tensor product H⊗KH\otimes KH⊗K. M1(X)M^1(\mathcal X)M1(X) denotes the finite signed measures whose variation has finite first moment. M1,1(X×Y)M^{1,1}(\mathcal X\times\mathcal Y)M1,1(X×Y) denotes those on the product whose variation has marginals of finite first moment.

Formalization targets

Goal: Theorem 3.11

If X\mathcal XX and Y\mathcal YY have strong negative type and the marginals μ,ν\mu,\nuμ,ν of the probability measure θ\thetaθ have finite first moments, then

dcov⁡(θ)=0 ⟹ θ=μ×ν.\operatorname{dcov}(\theta)=0\ \Longrightarrow\ \theta=\mu\times\nu .dcov(θ)=0 ⟹ θ=μ×ν.

Milestones

  1. Lemma 2.1: dμ∈L2(μ×μ)d_\mu\in L^2(\mu\times\mu)dμ​∈L2(μ×μ). The integrability of dμ(x,x′)dν(y,y′)d_\mu(x,x')d_\nu(y,y')dμ​(x,x′)dν​(y,y′) against θ2\theta^2θ2 (p. 4) follows, so dcov⁡(θ)\operatorname{dcov}(\theta)dcov(θ) is a genuine integral.
  2. Schoenberg's theorem (p. 9): a separable space has negative type if and only if it has an embedding into ℓ2(N)\ell^2(\mathbb N)ℓ2(N).
  3. Identity (3.4): D(μ)=−2∥βϕ(μ)∥2D(\mu)=-2\|\beta_\phi(\mu)\|^2D(μ)=−2∥βϕ​(μ)∥2 when μ(X)=0\mu(\mathcal X)=0μ(X)=0. Proposition 3.1: strong negative type holds iff βϕ\beta_\phiβϕ​ is injective on probability measures with finite first moment.
  4. Proposition 3.5: dμ(x,x′)=−2⟨ϕ(x)−βϕ(μ),ϕ(x′)−βϕ(μ)⟩d_\mu(x,x')=-2\langle\phi(x)-\beta_\phi(\mu),\phi(x')-\beta_\phi(\mu)\rangledμ​(x,x′)=−2⟨ϕ(x)−βϕ​(μ),ϕ(x′)−βϕ​(μ)⟩, together with aμ(x)=∥ϕ(x)−βϕ(μ)∥2+D(μ)/2a_\mu(x)=\|\phi(x)-\beta_\phi(\mu)\|^2+D(\mu)/2aμ​(x)=∥ϕ(x)−βϕ​(μ)∥2+D(μ)/2 and D(μ)=2Var⁡(ϕ(X))D(\mu)=2\operatorname{Var}(\phi(X))D(μ)=2Var(ϕ(X)).
  5. Proposition 3.7: dcov⁡(θ)=4∥βϕ⊗ψ(θ−μ×ν)∥2\operatorname{dcov}(\theta)=4\|\beta_{\phi\otimes\psi}(\theta-\mu\times\nu)\|^2dcov(θ)=4∥βϕ⊗ψ​(θ−μ×ν)∥2.
  6. Lemma 3.9 (injectivity of βϕ\beta_\phiβϕ​ on M1(X)M^1(\mathcal X)M1(X)) and Lemma 3.8 in its errata form (injectivity of βϕ⊗ψ\beta_{\phi\otimes\psi}βϕ⊗ψ​ on M1,1(X×Y)M^{1,1}(\mathcal X\times\mathcal Y)M1,1(X×Y)).

The converse, that a product measure has dcov⁡(θ)=0\operatorname{dcov}(\theta)=0dcov(θ)=0 (p. 5), is included as a companion statement.

Significance

The result. Theorem 3.11 makes the empirical distance covariance a consistent test of independence against all alternatives on any pair of separable metric spaces of strong negative type. Examples are separable Hilbert spaces and their subsets, and every space of negative type after replacing ddd by drd^rdr, 0<r<10<r<10<r<1. Its companion, Proposition 3.15 (a separate mission of this series), shows that strong negative type is exactly the right hypothesis. Proposition 3.7 also identifies distance covariance with Brownian covariance and with the original Euclidean definition, through specific choices of embedding.

Formalizing it. The result is proved, with the gap in Lemma 3.8 closed by the Errata (2018). No part of it has a machine-checked proof that we know of. A formalization needs barycenters of Hilbert-space-valued maps against measures, the Hilbert tensor product of two real Hilbert spaces, and Schoenberg's embedding theorem. None of these is in Mathlib in this form, and all are reusable well beyond distance covariance.

Difficulty

The obvious route reads dcov⁡(θ)=0\operatorname{dcov}(\theta)=0dcov(θ)=0 as "the barycenters of θ\thetaθ and of μ×ν\mu\times\nuμ×ν coincide in H⊗KH\otimes KH⊗K" and concludes by injectivity. Strong negative type only gives injectivity of βϕ\beta_\phiβϕ​ on probability measures, while θ−μ×ν\theta-\mu\times\nuθ−μ×ν is a signed measure on a product space. Getting from injectivity on single factors to injectivity on M1,1M^{1,1}M1,1 of the product is where the original proof had a gap: an auxiliary signed measure built from θ\thetaθ was not shown to have a finite first moment. The errata version changes the embeddings so that this can be done. Two smaller obstacles are integrability (the definition of dcov⁡\operatorname{dcov}dcov is meaningful only by Lemma 2.1) and the construction of the Hilbert space in Schoenberg's theorem.

Formalization scope

All spaces are Lean metric spaces with their Borel σ\sigmaσ-fields and SecondCountableTopology. This is the separability the author adds in Errata (i), which makes ddd measurable on the product. Measures are Mathlib Measures. A probability θ\thetaθ on X×Y\mathcal X\times\mathcal YX×Y has marginals θ.map Prod.fst and θ.map Prod.snd. "Product measure" means θ\thetaθ equals the product of these marginals. Hilbert spaces are real (Errata (viii)). Existential embeddings land in ℓ2(N)\ell^2(\mathbb N)ℓ2(N), which suffices for separable spaces. The Hilbert tensor product is the completion of the algebraic tensor product with its inner product. D(μ1−μ2)D(\mu_1-\mu_2)D(μ1​−μ2​) is defined by its bilinear expansion. Injectivity on M1M^1M1 and M1,1M^{1,1}M1,1 is stated for pairs of finite measures, which is equivalent to injectivity on signed measures via the Jordan decomposition.

Every integral here is a Bochner integral, which is 000 for a non-integrable integrand. Each statement therefore carries the finite-first-moment hypotheses of the paper, and integrability itself is a milestone. Negative type and strong negative type are defined by (3.1) and by the condition on D(μ1−μ2)D(\mu_1-\mu_2)D(μ1​−μ2​), not through an embedding or a barycenter map, so Schoenberg's theorem and Proposition 3.1 are not definitional. A statement with a "product measure" whose factors are free, or with dcov defined without the moment hypotheses, would be a different and trivializable theorem.

Welcome contributions: barycenter calculus for Hilbert-valued integrals, tensor-product integrals, Schoenberg's theorem, and proofs of any milestone.

Selected references

  • R. Lyons, Distance covariance in metric spaces, Ann. Probab. 41 (2013), 3284–3305. https://doi.org/10.1214/12-AOP803 ; author's version with both errata: https://arxiv.org/abs/1106.5758
  • R. Lyons, Errata to "Distance covariance in metric spaces", Ann. Probab. 46 (2018), 2400–2405; reproduced in https://arxiv.org/abs/1106.5758 (version of 19 Dec. 2020), pp. 24–29
  • G. J. Székely, M. L. Rizzo, N. K. Bakirov, Measuring and testing dependence by correlation of distances, Ann. Statist. 35 (2007), 2769–2794. https://doi.org/10.1214/009053607000000505
  • I. J. Schoenberg, Metric spaces and positive definite functions, Trans. Amer. Math. Soc. 44 (1938), 522–536. https://doi.org/10.1090/S0002-9947-1938-1501980-0
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ProbabilityStatistics·Captain: mikedeng1

Dynamic Assortment Personalization in High Dimensions 2: The Empirical Type Frequencies Satisfy ‖μ̂ − μ⋆‖_q ≤ min{8√((τ+m)/N), m^{1/q}√((τ+log 2m)/(2N))} with Probability at Least 1 − e^{−τ}Research Paper

Motivation

A retailer that personalizes the set of products it shows to each customer needs to know who its customers are. In the low-rank multinomial-logit model of Kallus and Udell, Dynamic Assortment Personalization in High Dimensions (arXiv:1610.05604), every arriving customer belongs to one of mmm customer types, and the type of each arrival is drawn independently from an unknown type distribution μ⋆\mu^\starμ⋆. Planning a non-personalized assortment, or weighting the per-type preference estimates, requires an estimate of μ⋆\mu^\starμ⋆ from the observed types. When mmm is large (types may be fine-grained customer profiles), the question is how many observations are needed before that estimate is reliable, and in which norm.

Theorem 4 of the paper answers this for the simplest estimator, the empirical frequencies, with an explicit, non-asymptotic bound in every ℓq\ell_qℓq​ norm, 1≤q≤∞1\le q\le\infty1≤q≤∞. The bound has two regimes: one that is good when the sample size NNN is only slightly larger than mmm, and one that is good when NNN is large compared with m2/qm^{2/q}m2/q.

Setting

Customer types are labelled 1,…,m1,\dots,m1,…,m. The type distribution is a vector μ⋆\mu^\starμ⋆ in the probability simplex

Δm={μ∈Rm: μi≥0, ∑i=1mμi=1}.\Delta^m=\Big\{\mu\in\mathbb R^m:\ \mu_i\ge0,\ \sum_{i=1}^m\mu_i=1\Big\}.Δm={μ∈Rm: μi​≥0, i=1∑m​μi​=1}.

The observation model (Sec. 3.2, p. 13) consists of NNN records (it,jt,St)(i_t,j_t,S_t)(it​,jt​,St​), t=1,…,Nt=1,\dots,Nt=1,…,N: the type iti_tit​ of the ttt-th customer, the item jtj_tjt​ the customer chose, and the assortment StS_tSt​ offered. The types i1,…,iNi_1,\dots,i_Ni1​,…,iN​ are independent and identically distributed with P(it=i)=μi⋆\mathbb P(i_t=i)=\mu^\star_iP(it​=i)=μi⋆​. The items and assortments play no role for the type distribution.

The empirical type frequencies (Sec. 3.2.1, p. 14) are

μ^i=1N∑t=1NI[it=i],i=1,…,m.\hat\mu_i=\frac1N\sum_{t=1}^N\mathbb I[i_t=i],\qquad i=1,\dots,m.μ^​i​=N1​t=1∑N​I[it​=i],i=1,…,m.

For v∈Rmv\in\mathbb R^mv∈Rm and q∈[1,∞]q\in[1,\infty]q∈[1,∞] the ℓq\ell_qℓq​ norm is ∥v∥q=(∑i∣vi∣q)1/q\|v\|_q=(\sum_i|v_i|^q)^{1/q}∥v∥q​=(∑i​∣vi​∣q)1/q, and ∥v∥∞=max⁡i∣vi∣\|v\|_\infty=\max_i|v_i|∥v∥∞​=maxi​∣vi​∣; the convention m1/q=1m^{1/q}=1m1/q=1 at q=∞q=\inftyq=∞ is used throughout.

The proof works with the empirical Rademacher complexity of the sample: with It=eitI_t=e_{i_t}It​=eit​​ the indicator vector of the ttt-th type,

R^N=12N∑ϵ∈{−1,+1}N sup⁡∥v∥∞≤1 1N∑t=1Nϵt vTIt.\widehat{\mathfrak R}_N=\frac1{2^N}\sum_{\epsilon\in\{-1,+1\}^N}\ \sup_{\|v\|_\infty\le1}\ \frac1N\sum_{t=1}^N\epsilon_t\,v^TI_t .RN​=2N1​ϵ∈{−1,+1}N∑​ ∥v∥∞​≤1sup​ N1​t=1∑N​ϵt​vTIt​.

Formalization targets

Goal: Theorem 4 (p. 18)

For every τ≥0\tau\ge0τ≥0 and q∈[1,∞]q\in[1,\infty]q∈[1,∞], with probability at least 1−e−τ1-e^{-\tau}1−e−τ,

∥μ^−μ⋆∥q ≤ min⁡{8τ+mN, m1/q2τ+log⁡(2m)N}.\|\hat\mu-\mu^\star\|_q\ \le\ \min\left\{8\sqrt{\frac{\tau+m}{N}},\ \frac{m^{1/q}}{\sqrt2}\sqrt{\frac{\tau+\log(2m)}{N}}\right\}.∥μ^​−μ⋆∥q​ ≤ min{8Nτ+m​​, 2​m1/q​Nτ+log(2m)​​}.

The goal keeps the paper's constants and its single statement over all q∈[1,∞]q\in[1,\infty]q∈[1,∞], including q=∞q=\inftyq=∞.

Milestones (proof of Theorem 4, p. 44)

  1. The coordinatewise tail bound, for η≥0\eta\ge0η≥0:
P(∥μ^−μ⋆∥q>η)≤∑i=1mP(∣μ^i−μi⋆∣>η/m1/q)≤2mexp⁡(−2Nη2/m2/q).\mathbb P(\|\hat\mu-\mu^\star\|_q>\eta)\le\sum_{i=1}^m\mathbb P\big(|\hat\mu_i-\mu^\star_i|>\eta/m^{1/q}\big)\le2m\exp(-2N\eta^2/m^{2/q}).P(∥μ^​−μ⋆∥q​>η)≤i=1∑m​P(∣μ^​i​−μi⋆​∣>η/m1/q)≤2mexp(−2Nη2/m2/q).
  1. The deterministic complexity bound, for every sample:
R^N=1N∑i=1m12N∑ϵ∣∑t=1NI[it=i]ϵt∣≤1N∑i=1mμ^i≤mN.\widehat{\mathfrak R}_N=\frac1N\sum_{i=1}^m\frac1{2^N}\sum_{\epsilon}\Big|\sum_{t=1}^N\mathbb I[i_t=i]\epsilon_t\Big|\le\frac1{\sqrt N}\sum_{i=1}^m\sqrt{\hat\mu_i}\le\sqrt{\frac mN}.RN​=N1​i=1∑m​2N1​ϵ∑​​t=1∑N​I[it​=i]ϵt​​≤N​1​i=1∑m​μ^​i​​≤Nm​​.
  1. The ℓ1\ell_1ℓ1​ tail bound, for η≥0\eta\ge0η≥0:
P(∥μ⋆−μ^∥1>η)≤e m−Nη2/64.\mathbb P(\|\mu^\star-\hat\mu\|_1>\eta)\le e^{\,m-N\eta^2/64}.P(∥μ⋆−μ^​∥1​>η)≤em−Nη2/64.

Significance

The first term of the minimum shows that μ^\hat\muμ^​ is consistent in every ℓq\ell_qℓq​ norm as soon as NNN grows faster than mmm, and gives m/N\sqrt{m/N}m/N​-consistency in ℓ1\ell_1ℓ1​, i.e. in total variation. A coordinatewise argument alone cannot give this: for q=1q=1q=1 it yields a bound that does not vanish unless NNN grows faster than m2m^2m2. The second term is the sharper one in the regime N≫m2/qN\gg m^{2/q}N≫m2/q, for instance in ℓ∞\ell_\inftyℓ∞​, where it gives the familiar log⁡(m)/N\sqrt{\log(m)/N}log(m)/N​ rate. In the paper the estimate of μ⋆\mu^\starμ⋆ enters non-personalized assortment planning, where the expected revenue of an assortment is averaged over types.

On the formalization side, the result is proved in the paper; nothing about it is open. As far as a search of the Prove2Me catalog shows, no machine-checked version of this statement, or of an ℓq\ell_qℓq​ concentration bound for empirical frequencies with these constants, exists. A complete development would also supply, in finite and elementary form, a coordinatewise Hoeffding bound for binomial proportions and an ℓ1\ell_1ℓ1​ deviation bound for categorical samples, both reusable well beyond this mission.

Difficulty

The second term is a union bound and a binomial tail bound. The first term is where the work is. The obvious route, bounding each coordinate separately and summing, costs a factor mmm in the ℓ1\ell_1ℓ1​ norm and gives a useless rate when NNN is comparable to mmm. The proof instead treats ∥μ^−μ⋆∥1\|\hat\mu-\mu^\star\|_1∥μ^​−μ⋆∥1​ as the supremum of an empirical process over the ℓ∞\ell_\inftyℓ∞​ unit ball, controls its mean through the Rademacher complexity (where the absolute value of a sum of Nμ^iN\hat\mu_iNμ^​i​ random signs must be bounded by Nμ^i\sqrt{N\hat\mu_i}Nμ^​i​​), and then needs concentration of the supremum around its mean with constants good enough to produce the stated 888 and 1/641/641/64. The paper's p. 44 citation of a symmetrization result states it with the empirical rather than the expected complexity, so that step has to be redone with care rather than transcribed.

Formalization scope

  • Source. The arXiv preprint arXiv:1610.05604. The PDF has no arXiv stamp, version or date and is pinned by its sha256 2b0104810fa9d656f2b79f8a44f791b2a3da388f3f6707564f4619da2050216a. Its printed page numbers equal the PDF page numbers.
  • Types and samples. Types are Fin m and draws Fin N, both 0-based. A sample is a map x : Fin N → Fin m.
  • Probability. The i.i.d. law is explicit: the probability of an event is the finite sum, over the samples in the event, of ∏tμxt⋆\prod_t\mu^\star_{x_t}∏t​μxt​⋆​. No measure theory is used. Restricting the observations (it,jt,St)(i_t,j_t,S_t)(it​,jt​,St​) to the types is exact, because the types are i.i.d. μ⋆\mu^\starμ⋆ regardless of the items and assortments.
  • Standing assumptions. μ⋆∈Δm\mu^\star\in\Delta^mμ⋆∈Δm (Mathlib's stdSimplex), which forces m≥1m\ge1m≥1, and N≥1N\ge1N≥1, added because μ^\hat\muμ^​ is undefined for an empty sample. The milestones' tail bounds assume η≥0\eta\ge0η≥0, which the paper leaves implicit. For η<0\eta<0η<0 the events are certain and the printed bounds can be smaller than 111.
  • Norms and exponents. ∥⋅∥q\|\cdot\|_q∥⋅∥q​ is Mathlib's PiLp norm on Rm\mathbb R^mRm for q∈[1,∞]q\in[1,\infty]q∈[1,∞], with qqq an extended nonnegative real; m1/qm^{1/q}m1/q and m2/qm^{2/q}m2/q use an exponent defined as 000 at q=∞q=\inftyq=∞ and 1/q1/q1/q otherwise. log⁡\loglog is the natural logarithm.
  • The Rademacher complexity is defined by the paper's supremum over the ℓ∞\ell_\inftyℓ∞​ unit ball, a nonempty index set on which the objective is bounded, so the supremum is genuine.
  • Corrected misprint. On p. 44 the Hoeffding display prints 2mexp⁡(−2nη2/m2/q)2m\exp(-2n\eta^2/m^{2/q})2mexp(−2nη2/m2/q) with nnn, the number of items. The formal statement uses the sample size NNN, which is what the argument produces and what Theorem 4 needs. In the complexity chain, the binomial coefficient printed as (m⌈Nμ^i/2⌉)\binom{m}{\lceil N\hat\mu_i/2\rceil}(⌈Nμ^​i​/2⌉m​) should be (Nμ^i⌈Nμ^i/2⌉)\binom{N\hat\mu_i}{\lceil N\hat\mu_i/2\rceil}(⌈Nμ^​i​/2⌉Nμ^​i​​); that line is not part of the formal statement.
  • Not a trivialization. The probability is taken under the i.i.d. product law of μ⋆\mu^\starμ⋆, not for a fixed sample and not under the uniform law on samples. The events use the paper's strict and non-strict inequalities as printed.
  • Welcome contributions. An elementary Hoeffding bound for the binomial proportion; a bounded-differences (McDiarmid) inequality for functions of finitely many independent finite-valued draws; a symmetrization inequality relating E∥μ^−μ⋆∥1\mathbb E\|\hat\mu-\mu^\star\|_1E∥μ^​−μ⋆∥1​ to the Rademacher complexity; and alternative proofs of the ℓ1\ell_1ℓ1​ term.

Selected references

  • N. Kallus, M. Udell, Dynamic Assortment Personalization in High Dimensions, arXiv preprint, 2016; Operations Research 68(4), 2020. https://arxiv.org/abs/1610.05604
  • P. L. Bartlett, S. Mendelson, Rademacher and Gaussian Complexities: Risk Bounds and Structural Results, Journal of Machine Learning Research 3, 463–482, 2002 (the paper cites it as 2003). https://www.jmlr.org/papers/v3/bartlett02a.html
  • W. Hoeffding, Probability Inequalities for Sums of Bounded Random Variables, Journal of the American Statistical Association 58(301), 13–30, 1963. https://doi.org/10.1080/01621459.1963.10500830
  • C. McDiarmid, On the Method of Bounded Differences, Surveys in Combinatorics, London Mathematical Society Lecture Note Series 141, 148–188, 1989. https://doi.org/10.1017/CBO9781107359949.008
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