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Operations ResearchOptimizationProbability·Captain: mikedeng1

Reliable Facility Location Design Under the Risk of Disruptions 1: With R = J the Compact Level-Assignment Formulation Equals the Scenario-Based Stochastic ProgramResearch Paper

Motivation

Facility location models decide where to open depots, warehouses or service centres and which customers each one serves. Classical models assume that an open facility always works. In practice facilities are disrupted by weather, strikes, power loss or supplier failure, and a network designed for normal operation can become very expensive when its nearest facilities go down. Reliable facility location models place facilities so that the sum of the fixed cost and the expected transportation cost, taken over random facility failures, is minimal.

Cui, Ouyang and Shen (UCTC-FR-2010-02, 2010; published as Oper. Res. 58(4):998–1011) study the case in which each site fails independently with its own probability. The most direct model of this situation is a scenario-based stochastic program: list every pattern of failures, give it its probability, and let each customer be served optimally in each pattern. That program has 2J2^J2J scenarios for JJJ candidate sites and cannot be written down for realistic JJJ. The paper proposes instead a compact formulation in which each customer receives an ordered list of backup facilities ("levels") and the probability that each level is the one that serves her is carried by a small set of recursive variables. This mission is about the claim that the compact model loses nothing.

The level-assignment technique comes from Snyder and Daskin (Transp. Sci. 39(3):400–416, 2005), who treated the case of one common failure probability for all sites. The uniform-probability model of Snyder and Shen's textbook is on the platform as SupplyChainTheory_disruptions; it is a different model (one qqq, no cap on the number of levels) and is not reused here.

Setting

There are III customers i=0,…,I−1i = 0,\dots,I-1i=0,…,I−1 with demand rates λi≥0\lambda_i \ge 0λi​≥0 and JJJ candidate sites j=0,…,J−1j = 0,\dots,J-1j=0,…,J−1 with fixed costs fjf_jfj​ and failure probabilities 0≤qj<10 \le q_j < 10≤qj​<1. Failures are independent. Shipping one unit from site jjj to customer iii costs dijd_{ij}dij​, and each unit of missed demand of customer iii costs a penalty ϕi\phi_iϕi​. An emergency facility with index JJJ never fails (qJ=0q_J = 0qJ​=0), costs nothing to open (fJ=0f_J = 0fJ​=0), and "serves" at the penalty cost diJ=ϕid_{iJ} = \phi_idiJ​=ϕi​.

The compact model (RUFL). Each customer is assigned to facilities at levels r=0,…,Rr = 0,\dots,Rr=0,…,R, with R≥1R \ge 1R≥1; a level-rrr facility serves her exactly when all her facilities at levels 0,…,r−10,\dots,r-10,…,r−1 have failed. The variables are Xj∈{0,1}X_j\in\{0,1\}Xj​∈{0,1} (site jjj open), Yijr∈{0,1}Y_{ijr}\in\{0,1\}Yijr​∈{0,1} (facility jjj is customer iii's level-rrr facility) and PijrP_{ijr}Pijr​, the probability that jjj serves iii at level rrr. Constraints (1b)–(1d) say that each level holds one facility until the emergency facility appears, which happens exactly once, and that only open sites are used, each at most once. Constraints (1e)–(1f) fix PPP: Pij0=1−qjP_{ij0} = 1-q_jPij0​=1−qj​ and Pijr=(1−qj)∑k<Jqk1−qkPi,k,r−1Yi,k,r−1P_{ijr} = (1-q_j)\sum_{k<J}\frac{q_k}{1-q_k}P_{i,k,r-1}Y_{i,k,r-1}Pijr​=(1−qj​)∑k<J​1−qk​qk​​Pi,k,r−1​Yi,k,r−1​. The objective is

Φ(X,Y,P)=∑j=0J−1fjXj+∑i=0I−1∑j=0J∑r=0RλidijPijrYijr.\Phi(X,Y,P) = \sum_{j=0}^{J-1} f_jX_j + \sum_{i=0}^{I-1}\sum_{j=0}^{J}\sum_{r=0}^{R}\lambda_i d_{ij}P_{ijr}Y_{ijr}.Φ(X,Y,P)=j=0∑J−1​fj​Xj​+i=0∑I−1​j=0∑J​r=0∑R​λi​dij​Pijr​Yijr​.

The scenario model (SSP). A scenario is ω∈Ω={0,1}J\omega\in\Omega=\{0,1\}^Jω∈Ω={0,1}J, with δjω=1\delta_{j\omega}=1δjω​=1 if site jjj operates in ω\omegaω (and δJω=1\delta_{J\omega}=1δJω​=1 always). Its probability is pω=∏j<J(1−qj)δjωqj1−δjωp_\omega = \prod_{j<J}(1-q_j)^{\delta_{j\omega}}q_j^{1-\delta_{j\omega}}pω​=∏j<J​(1−qj​)δjω​qj1−δjω​​. With Yijω∈{0,1}Y_{ij\omega}\in\{0,1\}Yijω​∈{0,1} (customer iii served by jjj in ω\omegaω), (SSP) minimizes

Ψ(X,Y)=∑j=0J−1fjXj+∑i=0I−1∑j=0J∑ω∈ΩλidijpωYijω\Psi(X,Y) = \sum_{j=0}^{J-1} f_jX_j + \sum_{i=0}^{I-1}\sum_{j=0}^{J}\sum_{\omega\in\Omega}\lambda_i d_{ij}p_\omega Y_{ij\omega}Ψ(X,Y)=j=0∑J−1​fj​Xj​+i=0∑I−1​j=0∑J​ω∈Ω∑​λi​dij​pω​Yijω​

subject to ∑j=0JYijω=1\sum_{j=0}^{J}Y_{ij\omega}=1∑j=0J​Yijω​=1 and Yijω≤δjωXjY_{ij\omega}\le\delta_{j\omega}X_jYijω​≤δjω​Xj​ for regular jjj.

Formalization targets

Goal: Proposition 1 (p. 10)

If R=JR = JR=J, both programs have optimal solutions, and for every optimal (X,Y,P)(X,Y,P)(X,Y,P) of (RUFL) and every optimal (X′,Y′)(X',Y')(X′,Y′) of (SSP),

Φ(X,Y,P)=Ψ(X′,Y′).\Phi(X,Y,P) = \Psi(X',Y').Φ(X,Y,P)=Ψ(X′,Y′).

The paper states this as "formulation (1a)–(1g) is equivalent to the stochastic programming formulation that covers all failure scenarios"; its proof shows equality of optimal values, and that is the reading formalized.

Milestones (Appendix A.1, pp. 32–34)

  1. Scenario-probability identity. For distinct regular sites j(0),…,j(r−1)j(0),\dots,j(r-1)j(0),…,j(r−1) and a facility j(r)j(r)j(r) not among them, the scenarios in which j(0),…,j(r−1)j(0),\dots,j(r-1)j(0),…,j(r−1) fail and j(r)j(r)j(r) operates have total probability
∑ω∈Ω(i,r)pω=(1−qj(r))∏ℓ=0r−1qj(ℓ).\sum_{\omega\in\Omega(i,r)}p_\omega = (1-q_{j(r)})\prod_{\ell=0}^{r-1}q_{j(\ell)}.ω∈Ω(i,r)∑​pω​=(1−qj(r)​)ℓ=0∏r−1​qj(ℓ)​.
  1. (RUFL) → (SSP). Every (RUFL)-feasible (X,Y,P)(X,Y,P)(X,Y,P) has an (SSP)-feasible (X,Y′)(X,Y')(X,Y′) with Ψ(X,Y′)=Φ(X,Y,P)\Psi(X,Y') = \Phi(X,Y,P)Ψ(X,Y′)=Φ(X,Y,P), for any RRR.
  2. Normalization. Some optimal solution of (SSP), with the same XXX, serves every customer in every scenario by her closest operating open facility, ties to the lowest index.
  3. (SSP) → (RUFL). If R=JR = JR=J, every normalized (SSP)-feasible (X,Y)(X,Y)(X,Y) has a (RUFL)-feasible (X,Y′,P′)(X,Y',P')(X,Y′,P′) with Φ(X,Y′,P′)=Ψ(X,Y)\Phi(X,Y',P') = \Psi(X,Y)Φ(X,Y′,P′)=Ψ(X,Y).

Significance

The proposition says that, with enough levels, the compact model is exact: its optimal value is the true minimum expected cost over all failure patterns. The compact model has O(IJR)O(IJR)O(IJR) variables and constraints against O(IJ2J)O(IJ2^J)O(IJ2J) for (SSP), and after the standard linearization of the products PijrYijrP_{ijr}Y_{ijr}Pijr​Yijr​ it is an ordinary mixed-integer program to which the paper's Lagrangian relaxation applies. For R<JR<JR<J the paper notes the compact model is in general not equivalent; Proposition 1 is the anchor that says what the parameter RRR trades away.

The result is proved in the paper; as far as we know it has not been formalized. The work here is to formalize that proof: the product-measure computation behind milestone 1, the two explicit solution maps, and the exchange argument behind the normalization. The probability identity for "first success in an ordered list of independent trials" and the scenario-to-level bookkeeping are reusable for other reliability models built on Snyder–Daskin levels.

Difficulty

The cost identities are routine once the right bookkeeping is in place; the obstacle is that bookkeeping. In direction (RUFL) → (SSP) one must show that the recursion (1e)–(1f), which multiplies by qk/(1−qk)q_k/(1-q_k)qk​/(1−qk​) and sums over all regular kkk, collapses to the closed product (1−qj(r))∏ℓ<rqj(ℓ)(1-q_{j(r)})\prod_{\ell<r}q_{j(\ell)}(1−qj(r)​)∏ℓ<r​qj(ℓ)​ along a customer's assigned list, using that (1b)–(1d) put exactly one facility on each level until the emergency facility and that (1c) forbids repeats. Then the sum over the 2J2^J2J scenarios must be regrouped by the first operating facility on that list, which needs milestone 1 on a product space.

The converse direction is where R=JR=JR=J enters, and the naive attempt fails: an arbitrary optimal (SSP) solution may serve a customer by different, equally good facilities in different scenarios in ways that no single ordered list reproduces. The normalization step removes this freedom; only after it can one read off a single list per customer, and R=JR=JR=J guarantees that this list (all open sites no farther than the penalty, then JJJ) fits on the available levels.

Formalization scope

Indices are 0-based; facilities are Fin (J+1) with Fin.last J the emergency facility, and levels are Fin (R+1). The extended data diJ=ϕid_{iJ}=\phi_idiJ​=ϕi​, qJ=0q_J=0qJ​=0, and the conventions δJω=1\delta_{J\omega}=1δJω​=1, XJ=1X_J=1XJ​=1 are definitions, not hypotheses. Scenarios are Fin J → Bool and pωp_\omegapω​ is the explicit finite product; no measure theory is involved, and (17a) is a finite sum. Binary variables are real numbers constrained to {0,1}\{0,1\}{0,1}. R=JR = JR=J is expressed by taking the instance type Instance I J J; with the standing R≥1R\ge 1R≥1 this means J≥1J\ge1J≥1. Demand rates are nonnegative; no sign is assumed on ddd, ϕ\phiϕ or fff.

Two printed constraints are corrected, and the formalization commits to the corrections. The first sum in (1b) is printed over the regular sites j≤J−1j\le J-1j≤J−1; it runs here over all J+1J+1J+1 facilities, as the paper's own reading of (1b) requires. Constraint (17c) is printed as ∑iYijω≤δjωXj\sum_i Y_{ij\omega}\le\delta_{j\omega}X_j∑i​Yijω​≤δjω​Xj​, which gives each site a capacity of one customer per scenario and makes Proposition 1 false; it is stated here per customer, Yijω≤δjωXjY_{ij\omega}\le\delta_{j\omega}X_jYijω​≤δjω​Xj​.

The goal asserts existence of optimal solutions of both programs before comparing their values, so it cannot hold vacuously. Contributions welcome: proofs of the milestones, a general lemma on the probability that the first success among independent Bernoulli trials occurs at a given position, and an existence-of-optimum lemma for finite binary programs.

Selected references

  • X. Cui, Y. Ouyang, Z.-J. M. Shen, Reliable Facility Location Design under the Risk of Disruptions, UCTC-FR-2010-02, University of California Transportation Center, 2010; Operations Research 58(4):998–1011, 2010. https://doi.org/10.1287/opre.1090.0801
  • L. V. Snyder, M. S. Daskin, Reliability models for facility location: the expected failure cost case, Transportation Science 39(3):400–416, 2005. https://doi.org/10.1287/trsc.1040.0107
  • H. D. Sherali, A. Alameddine, A new reformulation-linearization technique for bilinear programming problems, Journal of Global Optimization 2(4):379–410, 1992. https://doi.org/10.1007/BF00122429
8 thms2 active usersReviewed
Operations ResearchOptimization·Captain: mikedeng1

Reliable Facility Location Design Under the Risk of Disruptions 2: Optimal Solutions Order Each Customer's Assignment Levels by DistanceResearch Paper

Why backup assignments matter

A facility location plan decides which sites to open and which customers each site serves. Real facilities fail: plants are shut by strikes, warehouses by floods, distribution centres by power outages. When a customer's facility is down, she is served by a backup facility, or not served at all at a penalty. Reliable facility location chooses sites and backup assignments together, minimizing fixed costs plus the expected transportation and penalty cost over the random failures.

Snyder and Daskin (2005) introduced the level-assignment formulation in which every customer receives a ranked list of facilities, and they assumed all sites fail with the same probability. Cui, Ouyang and Shen (2010) allow each site its own failure probability qjq_jqj​, which is the realistic case: a site in a flood plain and a site inland do not fail equally often. Their compact mixed-integer program (RUFL) is the subject of this mission.

Timeline.

  • Snyder and Daskin (2005), Transportation Science 39(3): level-assignment formulation of the reliability P-median and UFL problems, equal failure probability qqq; consecutive assignments are ordered by distance in an optimal solution.
  • Snyder and Shen, Fundamentals of Supply Chain Theory, Theorem 9.10 (textbook treatment): the same ordering for the reliable fixed-charge location problem with 0<q<10<q<10<q<1 and positive demands.
  • Cui, Ouyang and Shen (2010), UCTC-FR-2010-02 / Operations Research 58(4): site-dependent failure probabilities qjq_jqj​, a cap RRR on the number of levels, and Proposition 2, the ordering result for this model.

The model (RUFL)

There are customers i=0,…,I−1i = 0,\dots,I-1i=0,…,I−1 with demand rates λi\lambda_iλi​, and candidate sites j=0,…,J−1j = 0,\dots,J-1j=0,…,J−1 with fixed costs fjf_jfj​ and failure probabilities 0≤qj<10 \le q_j < 10≤qj​<1; failures are independent. Shipping one unit from jjj to iii costs dijd_{ij}dij​, and each unserved unit of customer iii costs a penalty ϕi\phi_iϕi​. An emergency facility with index JJJ represents non-service: fJ=0f_J = 0fJ​=0, qJ=0q_J = 0qJ​=0 and diJ=ϕid_{iJ} = \phi_idiJ​=ϕi​.

Each customer is assigned at levels r=0,…,Rr = 0,\dots,Rr=0,…,R, R≥1R\ge 1R≥1. Her level-rrr facility serves her exactly when all her facilities at levels 0,…,r−10,\dots,r-10,…,r−1 have failed. The variables are Xj∈{0,1}X_j\in\{0,1\}Xj​∈{0,1} (site jjj open), Yijr∈{0,1}Y_{ijr}\in\{0,1\}Yijr​∈{0,1} (facility jjj is customer iii's level-rrr facility) and PijrP_{ijr}Pijr​, the probability that jjj serves iii at level rrr. (RUFL) minimizes

Φ(X,Y,P)=∑j=0J−1fjXj+∑i=0I−1∑j=0J∑r=0RλidijPijrYijr\Phi(X,Y,P) = \sum_{j=0}^{J-1} f_jX_j + \sum_{i=0}^{I-1}\sum_{j=0}^{J}\sum_{r=0}^{R}\lambda_i d_{ij}P_{ijr}Y_{ijr}Φ(X,Y,P)=j=0∑J−1​fj​Xj​+i=0∑I−1​j=0∑J​r=0∑R​λi​dij​Pijr​Yijr​

subject to: at every level a customer has exactly one facility unless she has already reached the emergency facility (1b); only open sites are used, each at most once (1c); the emergency facility is assigned exactly once (1d); and the probabilities follow the transition equations

Pij0=1−qj,Pijr=(1−qj)∑k=0J−1qk1−qkPi,k,r−1Yi,k,r−1(1≤r≤R).P_{ij0} = 1-q_j,\qquad P_{ijr} = (1-q_j)\sum_{k=0}^{J-1}\frac{q_k}{1-q_k}P_{i,k,r-1}Y_{i,k,r-1}\quad (1\le r\le R).Pij0​=1−qj​,Pijr​=(1−qj​)k=0∑J−1​1−qk​qk​​Pi,k,r−1​Yi,k,r−1​(1≤r≤R).

So if a customer's levels are j0,j1,…j_0, j_1, \dotsj0​,j1​,…, then Pijrr=(1−qjr) qj0⋯qjr−1P_{i j_r r} = (1-q_{j_r})\,q_{j_0}\cdots q_{j_{r-1}}Pijr​r​=(1−qjr​​)qj0​​⋯qjr−1​​.

Formalization targets

Goal: Proposition 2

Assume λi>0\lambda_i > 0λi​>0 for every customer and qk>0q_k > 0qk​>0 for every regular site. In every optimal solution (X,Y,P)(X,Y,P)(X,Y,P) of (RUFL),

Yijr=1, Yik,r+1=1 ⟹ dij≤dik(0≤r, r+1≤R, 0≤j,k≤J),Y_{ijr} = 1,\ Y_{ik,r+1} = 1 \ \Longrightarrow\ d_{ij}\le d_{ik}\qquad (0\le r,\ r+1\le R,\ 0\le j,k\le J),Yijr​=1, Yik,r+1​=1 ⟹ dij​≤dik​(0≤r, r+1≤R, 0≤j,k≤J),

where diJ=ϕid_{iJ} = \phi_idiJ​=ϕi​.

Milestones (the proof of Appendix A.2)

  1. Swap identity. If (X,Y,P)(X,Y,P)(X,Y,P) is feasible with Yijr=Yik,r+1=1Y_{ijr} = Y_{ik,r+1} = 1Yijr​=Yik,r+1​=1 for regular j,kj,kj,k, exchanging jjj and kkk and recomputing PPP gives a feasible solution whose cost changes by
λi(1−qk)(dik−dij)Pijr.\lambda_i(1-q_k)(d_{ik}-d_{ij})P_{ijr}.λi​(1−qk​)(dik​−dij​)Pijr​.
  1. Emergency case. If instead k=Jk = Jk=J, moving JJJ up to level rrr and dropping jjj gives a feasible solution whose cost changes by λiPijr(ϕi−dij)\lambda_i P_{ijr}(\phi_i - d_{ij})λi​Pijr​(ϕi​−dij​).
  2. Positivity. If every regular qk>0q_k>0qk​>0, an assigned facility has Pijr>0P_{ijr}>0Pijr​>0.

Significance

Proposition 2 says that for a given set of facilities assigned to a customer, the optimal order of the levels depends only on the distances, not on the failure probabilities. A solution method may therefore sort each customer's assigned facilities by distance instead of searching over orders. The paper's Lagrangian subproblem (RSPi_ii​) uses exactly this: "following a similar argument to Proposition 2" (§3.3.1, p. 13), its objective depends only on the set of facilities chosen, which is what makes the set function of Proposition 3 (a separate mission of this series) well defined. The proposition does not say that the RRR nearest open facilities are the right ones: the paper's Example 1 (p. 11) shows a farther but more reliable facility can be optimal.

The result is proved in the paper; no machine-checked proof exists. The equal-probability special case is published on Prove2Me as SupplyChainTheory.rflp_ordered_assignments (Snyder–Shen Theorem 9.10), in a different model (one qqq, no level cap). This mission adds the site-dependent case with a level cap, and it makes explicit two hypotheses the printed statement omits.

Difficulty

The exchange argument is short on paper, but its bookkeeping is exactly where a formal proof has to work. The paper's modified P′P'P′ keeps the old values at unlisted indices, and that array does not satisfy the transition equations, so feasibility of the swapped solution has to be shown with the recomputed probabilities, level by level, including the fact that levels after r+1r+1r+1 are unchanged. The emergency case is dismissed in one sentence; its cost change must be computed. Finally, "<0<0<0" needs λi>0\lambda_i>0λi​>0 and Pijr>0P_{ijr}>0Pijr​>0; the naive reading of the printed proposition, with qj=0q_j = 0qj​=0 allowed, is false, because a level-0 facility that never fails leaves all later levels with probability zero and in arbitrary order.

Formalization scope

Indices are 0-based. Facilities are Fin (J+1) with the emergency facility Fin.last J; levels are Fin (R+1); the extended data diJ=ϕid_{iJ}=\phi_idiJ​=ϕi​, qJ=0q_J=0qJ​=0 are definitions. XXX, YYY, PPP are real arrays, with (1g) requiring XXX, YYY to be 000 or 111. Constraint (1b) is printed with its first sum ending at J−1J-1J−1; it is formalized with the sum over all j≤Jj \le Jj≤J, the reading the paper's own explanation of (1b) gives. "Optimal" means feasible with objective at most that of every feasible solution; the feasible set is nonempty (send every customer to JJJ at level 0), so the goal is not vacuous. Proposition 2 carries the hypotheses λi>0\lambda_i>0λi​>0 and qk>0q_k>0qk​>0; without them it is false, and a statement that dropped them would be unprovable rather than trivial. The level rrr ranges over 0≤r≤R−10\le r\le R-10≤r≤R−1, the range in which level r+1r+1r+1 exists.

The development needs only finite sums and a recursion over levels; no measure theory is required. The recomputed probabilities transProb and the two moves swapY, emergencyUpY are reusable for any exchange argument on this formulation. Proofs of the milestones, of the goal, and of the equivalence of the transition equations with the closed product form are welcome.

Selected references

  • Cui, T., Ouyang, Y., Shen, Z.-J. M., Reliable Facility Location Design under the Risk of Disruptions, UCTC-FR-2010-02, University of California Transportation Center, 2010; published in Operations Research 58(4):998–1011, 2010. https://doi.org/10.1287/opre.1090.0801
  • Snyder, L. V., Daskin, M. S., Reliability Models for Facility Location: The Expected Failure Cost Case, Transportation Science 39(3):400–416, 2005. https://doi.org/10.1287/trsc.1040.0107
  • Snyder, L. V., Shen, Z.-J. M., Fundamentals of Supply Chain Theory, 2nd ed., Wiley, 2019, §9.6. https://doi.org/10.1002/9781119584445
6 thms2 active usersReviewed
Operations ResearchOptimizationProbability·Captain: mikedeng1

The Sample Average Approximation Method for Stochastic Discrete Optimization 1: Under Assumption A, 1 − P(Ŝ^ε_N ⊂ S^ε) Decays Exponentially Fast in the Sample Size NResearch Paper

Motivation

Many decision problems in operations research ask for the best element of a finite set of alternatives when each alternative's cost is random: which projects to fund when resource use is uncertain, which crew pairings to fly when delays are random, which items to pack into a knapsack whose overflow is penalized. The expected cost is rarely available in closed form, because it is a high-dimensional integral over the distribution of the random data. The sample average approximation (SAA) method replaces the expectation by an average over a random sample and solves the resulting deterministic problem with a standard discrete optimization routine. The method is widely used in stochastic programming (see Shapiro, Dentcheva and Ruszczyński, Lectures on Stochastic Programming, SIAM 2009, Ch. 5, https://doi.org/10.1137/1.9780898718751).

Kleywegt and Shapiro (preprint; published with Homem-de-Mello as SIAM J. Optim. 12(2):479–502, 2002, https://doi.org/10.1137/S1052623499363220) ask why the method works so well for discrete problems. Their answer is a large-deviations statement: when the feasible set is finite, the probability that the SAA problem returns a wrong answer decays exponentially in the sample size. This mission formalizes that result, Proposition 2.2 of the two-author preprint, together with its consistency companion, Proposition 2.1.

Setting

Let S\mathcal SS be a nonempty finite set, WWW a random element of a measurable space W\mathcal WW, and G:S×W→RG : \mathcal S \times \mathcal W \to \mathbb RG:S×W→R such that G(x,⋅)G(x,\cdot)G(x,⋅) is measurable and E∣G(x,W)∣<∞\mathbb E|G(x,W)| < \inftyE∣G(x,W)∣<∞ for every x∈Sx \in \mathcal Sx∈S. The true problem (1.1) is

v∗=min⁡x∈Sg(x),g(x)=E G(x,W).v^* = \min_{x \in \mathcal S} g(x), \qquad g(x) = \mathbb E\, G(x, W).v∗=x∈Smin​g(x),g(x)=EG(x,W).

Let W1,W2,…W^1, W^2, \dotsW1,W2,… be an independent, identically distributed sample with the law of WWW. The sample average function and the SAA problem (2.1) are

g^N(x)=1N∑n=1NG(x,Wn),v^N=min⁡x∈Sg^N(x).\hat g_N(x) = \frac1N \sum_{n=1}^N G(x, W^n), \qquad \hat v_N = \min_{x \in \mathcal S} \hat g_N(x).g^​N​(x)=N1​n=1∑N​G(x,Wn),v^N​=x∈Smin​g^​N​(x).

For ε≥0\varepsilon \ge 0ε≥0, the ε\varepsilonε-optimal sets are Sε={x∈S:g(x)≤v∗+ε}\mathcal S^\varepsilon = \{x \in \mathcal S : g(x) \le v^* + \varepsilon\}Sε={x∈S:g(x)≤v∗+ε} and S^Nε={x∈S:g^N(x)≤v^N+ε}\hat{\mathcal S}^\varepsilon_N = \{x \in \mathcal S : \hat g_N(x) \le \hat v_N + \varepsilon\}S^Nε​={x∈S:g^​N​(x)≤v^N​+ε}; at ε=0\varepsilon = 0ε=0 they are the optimal sets S∗\mathcal S^*S∗ and S^N\hat{\mathcal S}_NS^N​. Two numbers drive the analysis: the maximal deviation δN=max⁡x∈S∣g^N(x)−g(x)∣\delta_N = \max_{x \in \mathcal S}|\hat g_N(x) - g(x)|δN​=maxx∈S​∣g^​N​(x)−g(x)∣ of (2.2), and the well-conditioning number

α(ε)=min⁡x∈S∖Sεg(x)−v∗−ε\alpha(\varepsilon) = \min_{x \in \mathcal S \setminus \mathcal S^\varepsilon} g(x) - v^* - \varepsilonα(ε)=x∈S∖Sεmin​g(x)−v∗−ε

of (2.3), the gap between the ε\varepsilonε-optimal solutions and the rest.

For a real random variable XXX with moment generating function M(t)=E etXM(t) = \mathbb E\, e^{tX}M(t)=EetX and logarithmic moment generating function Λ(t)=log⁡M(t)∈(−∞,+∞]\Lambda(t) = \log M(t) \in (-\infty, +\infty]Λ(t)=logM(t)∈(−∞,+∞], the rate function is I(z)=sup⁡t≥0{tz−Λ(t)}I(z) = \sup_{t \ge 0}\{tz - \Lambda(t)\}I(z)=supt≥0​{tz−Λ(t)}. Assumption A requires that for every x∈Sx \in \mathcal Sx∈S the moment generating function of G(x,W)G(x, W)G(x,W) be finite in a neighbourhood of t=0t = 0t=0.

Formalization targets

Goal: Proposition 2.2

Under Assumption A, for every ε≥0\varepsilon \ge 0ε≥0 there is γ>0\gamma > 0γ>0 with

lim sup⁡N→∞1Nlog⁡[1−P(S^Nε⊂Sε)]≤−γ.(2.5)\limsup_{N \to \infty} \frac1N \log\Big[1 - P\big(\hat{\mathcal S}^\varepsilon_N \subset \mathcal S^\varepsilon\big)\Big] \le -\gamma. \tag{2.5}N→∞limsup​N1​log[1−P(S^Nε​⊂Sε)]≤−γ.(2.5)

The constant γ\gammaγ is not specified: it depends on α(ε)\alpha(\varepsilon)α(ε) through rate functions and cannot be computed before the problem is solved. The goal asserts only its existence, which is the paper's claim.

Milestones

  1. α(ε)>0\alpha(\varepsilon) > 0α(ε)>0 whenever S∖Sε≠∅\mathcal S \setminus \mathcal S^\varepsilon \ne \emptysetS∖Sε=∅ (2.3).
  2. δN<α(ε)/2\delta_N < \alpha(\varepsilon)/2δN​<α(ε)/2 implies S^Nε⊂Sε\hat{\mathcal S}^\varepsilon_N \subset \mathcal S^\varepsilonS^Nε​⊂Sε.
  3. The union bound 1−P(S^Nε⊂Sε)≤∑x∈SP{∣g^N(x)−g(x)∣≥α(ε)/2}1 - P(\hat{\mathcal S}^\varepsilon_N \subset \mathcal S^\varepsilon) \le \sum_{x \in \mathcal S} P\{|\hat g_N(x) - g(x)| \ge \alpha(\varepsilon)/2\}1−P(S^Nε​⊂Sε)≤∑x∈S​P{∣g^​N​(x)−g(x)∣≥α(ε)/2}.
  4. The large-deviations upper bound (2.4): 1Nlog⁡P(ZN≥a)≤−I(a)\frac1N \log P(Z_N \ge a) \le -I(a)N1​logP(ZN​≥a)≤−I(a) for i.i.d. averages ZNZ_NZN​.
  5. I(a)>0I(a) > 0I(a)>0 for aaa above the mean, when MMM is finite near 000.
  6. Under Assumption A, P{∣g^N(x)−g(x)∣≥r}≤e−Nγx+e−Nγx′P\{|\hat g_N(x) - g(x)| \ge r\} \le e^{-N\gamma_x} + e^{-N\gamma'_x}P{∣g^​N​(x)−g(x)∣≥r}≤e−Nγx​+e−Nγx′​ with γx,γx′>0\gamma_x, \gamma'_x > 0γx​,γx′​>0.

Companions

Proposition 2.1 (v^N→v∗\hat v_N \to v^*v^N​→v∗ w.p.1, and S^Nε⊂Sε\hat{\mathcal S}^\varepsilon_N \subset \mathcal S^\varepsilonS^Nε​⊂Sε w.p.1 for NNN large enough), the almost-sure convergence δN→0\delta_N \to 0δN​→0 of (2.2), the singleton consequence (Sε={x∗}\mathcal S^\varepsilon = \{x^*\}Sε={x∗} implies S^Nε={x∗}\hat{\mathcal S}^\varepsilon_N = \{x^*\}S^Nε​={x∗} eventually), the facts I(μ)=0=min⁡II(\mu) = 0 = \min II(μ)=0=minI, the Example of §3.2 showing that a sample size N>k/2N > k/2N>k/2 can be required, and the computation α(0)=min⁡ici\alpha(0) = \min_i c_iα(0)=mini​ci​ on the hypercube with best value 1/k1/p1/k^{1/p}1/k1/p (§4).

Significance

Proposition 2.2 explains the practical behaviour of the SAA method on discrete problems: an exact optimal solution of the true problem is obtained with probability approaching one exponentially fast, so a moderate sample often suffices even when the number of feasible solutions is astronomically large. It is the basis of the paper's replication argument (§3.2: the probability of success p(N)p(N)p(N) of one SAA replication tends to one exponentially fast) and identifies α(ε)\alpha(\varepsilon)α(ε) as the quantity that governs the difficulty of a stochastic discrete problem, which the numerical study of §4 then examines. Later sample-size estimates for SAA (Shapiro, Dentcheva and Ruszczyński 2009, §5.3) refine the same argument into explicit, non-asymptotic bounds.

The result is proved in the paper. The mission produces a machine-checked proof of it and of its ingredients, including a Lean statement of the Cramér–Chernoff upper bound with the rate function III in the extended reals and the positivity of III above the mean under a local moment condition. To our knowledge none of these is formalized on the platform or in Mathlib in this form.

Difficulty

The argument is short on paper; the formal difficulty is in the large-deviations step. Mathlib has the Chernoff inequality P(X≥a)≤e−ta EetXP(X \ge a) \le e^{-ta}\,\mathbb E e^{tX}P(X≥a)≤e−taEetX and the factorization of moment generating functions of independent sums, but the step from there to 1Nlog⁡P(ZN≥a)≤−I(a)\frac1N \log P(Z_N \ge a) \le -I(a)N1​logP(ZN​≥a)≤−I(a) requires passing to a supremum over ttt in the extended reals, handling ttt where M(t)=∞M(t) = \inftyM(t)=∞, and the case P(ZN≥a)=0P(Z_N \ge a) = 0P(ZN​≥a)=0. The positivity I(a)>0I(a) > 0I(a)>0 requires Λ′(0)=μ\Lambda'(0) = \muΛ′(0)=μ, i.e. differentiating the moment generating function at an interior point of its domain. A naive attempt that works with real logarithms fails at probability zero, where log⁡0\log 0log0 is not −∞-\infty−∞, and an attempt that bounds δN\delta_NδN​ by Chebyshev's inequality gives only a polynomial rate.

Formalization scope

The feasible set is a Finset of an arbitrary type X, assumed nonempty; minima and maxima over it are Finset.inf' and Finset.sup', so they are attained. The sample is a sequence W : ℕ → Ω → 𝒲 of measurable maps on a probability space, mutually independent (iIndepFun) and identically distributed with W 0; the paper's WnW^nWn is W (n - 1), and g(x)g(x)g(x) is the expectation of G(x,W1)G(x, W^1)G(x,W1). Measurability of G(x,⋅)G(x,\cdot)G(x,⋅) is Borel measurability. Logarithms of probabilities are ENNReal.log, with log⁡0=−∞\log 0 = -\inftylog0=−∞, and the limit superior in (2.5) is taken in the extended reals; this is the paper's convention and it makes the goal correct when Sε=S\mathcal S^\varepsilon = \mathcal SSε=S, where the event is sure. Assumption A is stated as integrability of etG(x,W)e^{tG(x,W)}etG(x,W) for ttt near 000, not through the value of Mathlib's mgf, which is 000 where the expectation is infinite. The logarithmic moment generating function is the published definition BellWilliams2001.ThresholdPolicy.logMGF (extended-real valued, +∞+\infty+∞ off the domain of MMM), and III is the supremum over t≥0t \ge 0t≥0 only, as on p. 3. Wherever α(ε)\alpha(\varepsilon)α(ε) appears, the nonemptiness of S∖Sε\mathcal S \setminus \mathcal S^\varepsilonS∖Sε is a hypothesis; the goal does not mention α\alphaα and needs none.

A trivializing formalization is ruled out: with Real.log the event "S^Nε⊂Sε\hat{\mathcal S}^\varepsilon_N \subset \mathcal S^\varepsilonS^Nε​⊂Sε is sure" would give log⁡0=0\log 0 = 0log0=0 and make the goal false, and a rate function built from mgf would count infinite moment generating functions as Λ=log⁡0=0\Lambda = \log 0 = 0Λ=log0=0; neither encoding is used.

A complete development needs the Cramér–Chernoff bound for i.i.d. sums with an extended-real rate function, differentiability of the moment generating function at interior points, and the strong law of large numbers applied to finitely many functions. The large-deviations items (milestones 4 and 5, and I(μ)=0I(\mu) = 0I(μ)=0) are stated for an arbitrary i.i.d. real sequence and are reusable beyond this mission. Proofs of any item, including the optional examples, are welcome.

Selected references

  • A. J. Kleywegt and A. Shapiro, The sample average approximation method for stochastic discrete optimization, preprint (two-author version), https://edoc.hu-berlin.de/server/api/core/bitstreams/2dcf2d5b-5fb9-44d1-b36a-5e378c803717/content. Published with T. Homem-de-Mello in SIAM J. Optim. 12(2):479–502, 2002. https://doi.org/10.1137/S1052623499363220
  • A. Dembo and O. Zeitouni, Large Deviations Techniques and Applications, 2nd ed., Springer, 1998. https://doi.org/10.1007/978-1-4612-5320-4
  • A. Shapiro, D. Dentcheva and A. Ruszczyński, Lectures on Stochastic Programming: Modeling and Theory, SIAM, 2009. https://doi.org/10.1137/1.9780898718751
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Dynamical SystemsOperations ResearchStochastic Systems+1·Captain: mikedeng1

The Power of Two Choices in Randomized Load Balancing I: In the Limiting Supermarket System the Expected Time Converges to T_d(λ) = Σ λ^((d^i−d)/(d−1))Research Paper

Motivation

Randomized load balancing asks how much a dispatcher gains from a little information. In the supermarket model, jobs arrive at nnn servers and each job inspects a few servers chosen at random before joining one. With one random choice every server is an independent M/M/1 queue, and the expected time a job spends in the system is 1/(1−λ)1/(1-\lambda)1/(1−λ) at load λ\lambdaλ. With two choices it is exponentially smaller as λ→1−\lambda \to 1^-λ→1−. This "power of two choices" underlies the design of distributed schedulers, hashing schemes and server farms, where querying every server is too expensive but querying two is cheap.

Timeline:

  • 1994/1999. Azar, Broder, Karlin and Upfal proved the static version, balanced allocations: throwing nnn balls into nnn bins with d≥2d \ge 2d≥2 choices per ball gives a maximum load of log⁡log⁡n/log⁡d+O(1)\log\log n/\log d + O(1)loglogn/logd+O(1) w.h.p., against Θ(log⁡n/log⁡log⁡n)\Theta(\log n/\log\log n)Θ(logn/loglogn) for one choice (SIAM J. Comput. 1999).
  • 1996. Vvedenskaya, Dobrushin and Karpelevich derived the dynamic limiting equations for d=2d = 2d=2 and showed convergence of their trajectories to the fixed point, without a rate (Problems of Information Transmission 32(1), 1996).
  • 1996/2001. Mitzenmacher, independently, introduced the limiting system for general ddd, proved doubly exponential tails along every trajectory and exponential convergence to the fixed point in a weighted L1L_1L1​ potential, and derived the limiting expected time Td(λ)T_d(\lambda)Td​(λ) (IEEE TPDS 2001). This mission formalizes Section 2 of that paper.

Setting

Customers arrive as a Poisson stream of rate λn\lambda nλn, 0<λ<10<\lambda<10<λ<1, at nnn FIFO servers. Each customer chooses ddd servers independently and uniformly at random with replacement and joins the one holding the fewest customers; service times are exponential with mean 111. Let si(t)s_i(t)si​(t) be the fraction of servers holding at least iii customers at time ttt.

A state is a sequence s=(s0,s1,s2,… )s = (s_0, s_1, s_2, \dots)s=(s0​,s1​,s2​,…) of reals with s0=1s_0 = 1s0​=1, si≥0s_i \ge 0si​≥0 and s0≥s1≥s2≥⋯s_0 \ge s_1 \ge s_2 \ge \cdotss0​≥s1​≥s2​≥⋯. The empty state has s0=1s_0 = 1s0​=1 and si=0s_i = 0si​=0 for i≥1i \ge 1i≥1. As n→∞n \to \inftyn→∞ the tails follow the limiting system

dsidt=λ (si−1d−sid)−(si−si+1)(i≥1),s0=1.(1)\frac{ds_i}{dt} = \lambda\,(s_{i-1}^d - s_i^d) - (s_i - s_{i+1}) \quad (i \ge 1), \qquad s_0 = 1. \tag{1}dtdsi​​=λ(si−1d​−sid​)−(si​−si+1​)(i≥1),s0​=1.(1)

A trajectory is a map t↦s(t)t \mapsto s(t)t↦s(t), t≥0t \ge 0t≥0, whose values are states and whose coordinates satisfy (1) (from the right at t=0t = 0t=0). Throughout, d≥2d \ge 2d≥2 is an integer.

The fixed point is πi=λ(di−1)/(d−1)\pi_i = \lambda^{(d^i - 1)/(d - 1)}πi​=λ(di−1)/(d−1), so π0=1\pi_0 = 1π0​=1, π1=λ\pi_1 = \lambdaπ1​=λ, π2=λ1+d\pi_2 = \lambda^{1+d}π2​=λ1+d. A customer arriving in state sss becomes the iii-th customer of its queue with probability si−1d−sids_{i-1}^d - s_i^dsi−1d​−sid​ and then waits for iii services, so the expected time it spends in the system is

E(s)=∑i=1∞i (si−1d−sid).E(s) = \sum_{i=1}^{\infty} i\,(s_{i-1}^d - s_i^d).E(s)=i=1∑∞​i(si−1d​−sid​).

The target constant is

Td(λ)=∑i=1∞λdi−dd−1.T_d(\lambda) = \sum_{i=1}^{\infty} \lambda^{\frac{d^i - d}{d-1}}.Td​(λ)=i=1∑∞​λd−1di−d​.

Formalization targets

Goal: Corollary 2

For d≥2d \ge 2d≥2 and 0<λ<10 < \lambda < 10<λ<1, Td(λ)<∞T_d(\lambda) < \inftyTd​(λ)<∞, and:

if sj(0)=0 for some j, then E(s(t))→t→∞Td(λ);if s(0) is empty, then E(s(t))≤Td(λ)  ∀t≥0.\text{if } s_j(0) = 0 \text{ for some } j, \text{ then } E(s(t)) \xrightarrow[t\to\infty]{} T_d(\lambda);\qquad \text{if } s(0) \text{ is empty, then } E(s(t)) \le T_d(\lambda) \ \ \forall t \ge 0.if sj​(0)=0 for some j, then E(s(t))t→∞​Td​(λ);if s(0) is empty, then E(s(t))≤Td​(λ)  ∀t≥0.

The hypothesis sj(0)=0s_j(0) = 0sj​(0)=0 holds for every initial state that comes from a finite system.

Milestones, in the order the proof uses them

  • Lemma 2. π\piπ is the unique fixed point of (1) with ∑i≥1si<∞\sum_{i\ge1} s_i < \infty∑i≥1​si​<∞.
  • Theorem 2. If sj(0)=0s_j(0) = 0sj​(0)=0 for some jjj, there are constants N≥1N \ge 1N≥1, 0<α<10<\alpha<10<α<1, β>1\beta>1β>1, γ>0\gamma>0γ>0, independent of ttt, with si(t)≤γ αβis_i(t) \le \gamma\,\alpha^{\beta^i}si​(t)≤γαβi for all i≥Ni \ge Ni≥N, t≥0t \ge 0t≥0. From the empty state, si(t)≤πis_i(t) \le \pi_isi​(t)≤πi​ for all iii and t≥0t \ge 0t≥0.
  • Theorem 3. There are weights wi≥1w_i \ge 1wi​≥1 such that Φ(t)=∑i≥1wi∣si(t)−πi∣\Phi(t) = \sum_{i\ge1} w_i |s_i(t) - \pi_i|Φ(t)=∑i≥1​wi​∣si​(t)−πi​∣ satisfies Φ(t)≤c0e−δt\Phi(t) \le c_0 e^{-\delta t}Φ(t)≤c0​e−δt (δ>0\delta > 0δ>0) whenever Φ(0)<∞\Phi(0) < \inftyΦ(0)<∞, and in particular whenever sj(0)=0s_j(0) = 0sj​(0)=0 for some jjj.
  • Corollary 1. Under the conditions of Theorem 3 (weights wi≥1w_i \ge 1wi​≥1 fixed before the trajectory, with Φ(0)<∞\Phi(0) < \inftyΦ(0)<∞, or sj(0)=0s_j(0) = 0sj​(0)=0 for some jjj), ∑i≥1∣si(t)−πi∣≤c0e−δt\sum_{i\ge1} |s_i(t) - \pi_i| \le c_0 e^{-\delta t}∑i≥1​∣si​(t)−πi​∣≤c0​e−δt.
  • Proof of Corollary 2, display. ∑i≥1i(si−1d−sid)=∑i≥0sid\sum_{i\ge1} i(s_{i-1}^d - s_i^d) = \sum_{i\ge0} s_i^d∑i≥1​i(si−1d​−sid​)=∑i≥0​sid​ for a state with si→0s_i \to 0si​→0.
  • Lemma 4. The drift of (1) is Lipschitz in ℓ1\ell^1ℓ1 on states, with constant 2+2dλ2 + 2d\lambda2+2dλ.

Significance

The comparison T1(λ)=1/(1−λ)T_1(\lambda) = 1/(1-\lambda)T1​(λ)=1/(1−λ) against Td(λ)T_d(\lambda)Td​(λ) is the quantitative content of the power of two choices: the companion mission shows Td(λ)/log⁡T1(λ)→1/log⁡dT_d(\lambda)/\log T_1(\lambda) \to 1/\log dTd​(λ)/logT1​(λ)→1/logd as λ→1−\lambda \to 1^-λ→1−, an exponential improvement. Corollary 2 is what connects that number to the dynamics: it says the fixed point's expected time is actually reached from realistic initial states, and is an upper bound from an empty start. Theorem 2's comparison argument and Theorem 3's weighted potential are reused across the mean-field analysis of load-balancing variants (threshold policies, heterogeneous servers, work stealing), so the formal statements here are templates for that literature.

All results are proved in the paper (Theorem 3's proof is written out for d=2d = 2d=2 with a remark that it extends). None has a machine-checked proof that we know of. The work is formalizing the known arguments for all d≥2d \ge 2d≥2, including the parts the paper delegates to a citation: quasimonotone comparison for countable ODE systems in Theorem 2, and the upper right Dini derivative handling of ∣ϵi∣|\epsilon_i|∣ϵi​∣ in Theorem 3.

Difficulty

The system is infinite-dimensional, so standard finite-dimensional ODE comparison and Lyapunov theorems do not apply as stated. Theorem 2 rests on a monotonicity property (raising the initial tails raises them for all time) that the paper justifies by a coupling intuition and a citation to a comparison theorem for quasimonotone systems; that theorem must be supplied for ℓ∞\ell^\inftyℓ∞-bounded countable systems. The plain L1L_1L1​ distance is nonincreasing along trajectories but does not decay exponentially by a direct estimate; the weights wiw_iwi​ must be built so that every coordinate's contribution to dΦ/dtd\Phi/dtdΦ/dt is dominated by −δwi∣ϵi∣-\delta w_i |\epsilon_i|−δwi​∣ϵi​∣, while staying geometrically bounded so that Φ(0)<∞\Phi(0) < \inftyΦ(0)<∞ under the doubly exponential tails of Theorem 2. Exchanging t→∞t \to \inftyt→∞ with the infinite sum defining EEE needs uniform tail control, which is again Theorem 2.

Formalization scope

  • Namespace PowerTwoChoices.Limit; λ is lam : ℝ, d:Nd : ℕd:N with 2≤d2 \le d2≤d, 0<λ<10 < \lambda < 10<λ<1 in every theorem.
  • A state is x : ℕ → ℝ with x 0 = 1, nonnegative and antitone. A trajectory is s : ℝ → ℕ → ℝ, a state for every t≥0t \ge 0t≥0, with HasDerivWithinAt on Set.Ici 0 for each coordinate i≥1i \ge 1i≥1: right derivative at t=0t = 0t=0, two-sided for t>0t > 0t>0.
  • Exponents are natural numbers: πi=λ∑k<idk\pi_i = \lambda^{\sum_{k<i} d^k}πi​=λ∑k<i​dk, and TdT_dTd​'s iii-th term is λ∑1≤k<idk\lambda^{\sum_{1\le k<i} d^k}λ∑1≤k<i​dk.
  • Φ\PhiΦ, the L1L_1L1​ distance, EEE and TdT_dTd​ are sums in [0,∞][0,\infty][0,∞], so a divergent series is ∞\infty∞, never a default 000. "Converges exponentially" (Definition 2) means Φ(t)≤c0e−δt\Phi(t) \le c_0 e^{-\delta t}Φ(t)≤c0​e−δt for all t≥0t \ge 0t≥0 with real c0c_0c0​ and δ>0\delta > 0δ>0; δ\deltaδ may depend on the trajectory. The paper's d(t)d(t)d(t) is renamed l1Dist.
  • Time is real and t→∞t \to \inftyt→∞ is Filter.atTop.
  • Every theorem quantifies over trajectories; existence of a trajectory from a given state (Picard iteration, cited by the paper) is not part of the mission. The class is nonempty: the constant trajectory at π\piπ is one.
  • Ruled out: summing EEE or TdT_dTd​ as a real tsum (a divergent series would make the upper bound free and the limit attainable by a junk 000), dropping the summability condition in Lemma 2 ((1,1,… )(1,1,\dots)(1,1,…) is also a fixed point), choosing Theorem 3's weights after the trajectory, and stating anything for d=2d = 2d=2 only.
  • Needed infrastructure: comparison principles for quasimonotone countable ODE systems, Dini-derivative Grönwall estimates, and interchange of limits and ℓ1\ell^1ℓ1 sums. All of these are reusable beyond this mission, and contributions of such lemmas as separate theorems are welcome.

Selected references

  • M. Mitzenmacher, The Power of Two Choices in Randomized Load Balancing, IEEE Transactions on Parallel and Distributed Systems 12(10), 2001, pp. 1094–1104. https://doi.org/10.1109/71.963420
  • Y. Azar, A. Z. Broder, A. R. Karlin, E. Upfal, Balanced Allocations, SIAM Journal on Computing 29(1), 1999, pp. 180–200. https://doi.org/10.1137/S0097539795288490
  • N. D. Vvedenskaya, R. L. Dobrushin, F. I. Karpelevich, Queueing System with Selection of the Shortest of Two Queues: An Asymptotic Approach, Problems of Information Transmission 32(1), 1996, pp. 15–27.
  • T. G. Kurtz, Approximation of Population Processes, SIAM, 1981. https://doi.org/10.1137/1.9781611970333
8 thms2 active usersReviewed
Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Designing a Call Center with Impatient Customers II: In the Halfin–Whitt Regime the Scaled Erlang-A Queue Converges to a Diffusion with Piecewise-Linear DriftResearch Paper

Motivation

Telephone call centers are large service systems: hundreds of agents answer callers who wait in a queue and hang up when their patience runs out. Staffing them is a trade-off between the cost of agents and the quality of service, and in large centers both the efficiency (agents busy almost all the time) and the service level (most callers answered almost immediately) can be high at once. Garnett, Mandelbaum and Reiman (M&SOM 4(3), 2002) study the simplest model that captures customer abandonment, the Erlang-A or M/M/N+MM/M/N+MM/M/N+M queue, and derive approximations for it in the regime where the number of agents is large.

Their Theorem 2 is the process-level justification of these approximations: the queue-length process, centred at the number of agents and scaled by its square root, converges to a one-dimensional diffusion. The steady-state performance formulas of the paper (delay probability, abandonment probability, waiting times) are computed from this diffusion and its stationary law.

Timeline.

  • Halfin and Whitt (1981) proved the corresponding limit for the M/M/NM/M/NM/M/N queue without abandonment, in the regime N(1−ρN)→β\sqrt N(1-\rho_N) \to \betaN​(1−ρN​)→β with β>0\beta > 0β>0 (Oper. Res. 29(3)). The limit is a diffusion with drift −μ(β+x)-\mu(\beta + x)−μ(β+x) below 000 and constant drift −μβ-\mu\beta−μβ above.
  • Fleming, Stolyar and Simon (1994) conjectured the limit with abandonment, with a slightly different centering, and proved the weak limit of the stationary distributions.
  • Garnett, Mandelbaum and Reiman (2002) state the process limit for 0<θ<∞0 < \theta < \infty0<θ<∞ as Theorem 2, with the extensions θ=0\theta = 0θ=0 and θ=∞\theta = \inftyθ=∞ as Theorem 2* in Appendix C.

Setting

Fix a service rate μ>0\mu > 0μ>0. For each N≥1N \ge 1N≥1 the NNN-th system has NNN statistically identical agents, Poisson arrivals of rate λN>0\lambda_N > 0λN​>0, exponential service times of rate μ\muμ, an unlimited waiting room served first come, first served, and exponential patience of rate θN>0\theta_N > 0θN​>0 for every caller. A caller whose wait in queue reaches their patience abandons and does not return. The number of callers in the system, QN(t)Q_N(t)QN​(t), is a birth–death process on {0,1,2,… }\{0, 1, 2, \dots\}{0,1,2,…} with birth rate λN\lambda_NλN​ and death rate min⁡(k,N)μ+(k−N)+θN\min(k, N)\mu + (k-N)^+\theta_Nmin(k,N)μ+(k−N)+θN​ in state kkk. Its initial value QN(0)Q_N(0)QN​(0) is an arbitrary random variable.

The traffic intensity is ρN=λN/(Nμ)\rho_N = \lambda_N/(N\mu)ρN​=λN​/(Nμ). The centred and scaled process is

qN(t)=QN(t)−NN,t≥0.q_N(t) = \frac{Q_N(t) - N}{\sqrt N}, \qquad t \ge 0 .qN​(t)=N​QN​(t)−N​,t≥0.

When qN≥0q_N \ge 0qN​≥0 it counts waiting callers and when qN≤0q_N \le 0qN​≤0 it counts idle agents, both in units of N\sqrt NN​.

For β∈R\beta \in \mathbb Rβ∈R and θ>0\theta > 0θ>0, the drift is the piecewise-linear function

f(x)={−μ(β+x),x≤0,−(μβ+θx),x>0,f(x) = \begin{cases} -\mu(\beta + x), & x \le 0,\\ -(\mu\beta + \theta x), & x > 0,\end{cases}f(x)={−μ(β+x),−(μβ+θx),​x≤0,x>0,​

and the limit diffusion qqq solves dq(t)=f(q(t)) dt+2μ db(t)dq(t) = f(q(t))\,dt + \sqrt{2\mu}\,db(t)dq(t)=f(q(t))dt+2μ​db(t), where bbb is a standard Brownian motion independent of q(0)q(0)q(0). The noise is additive, so this means: qqq has continuous paths and q(t)=q(0)+∫0tf(q(s)) ds+2μ b(t)q(t) = q(0) + \int_0^t f(q(s))\,ds + \sqrt{2\mu}\,b(t)q(t)=q(0)+∫0t​f(q(s))ds+2μ​b(t) for all t≥0t \ge 0t≥0. Below 000 it behaves like an Ornstein–Uhlenbeck process with restraining force μ\muμ, above 000 like one with restraining force θ\thetaθ.

Formalization targets

Goal: Theorem 2 (p. 216)

Assume

lim⁡N→∞N(1−ρN)=β∈(−∞,∞),lim⁡N→∞θN=θ∈(0,∞),\lim_{N\to\infty}\sqrt N(1-\rho_N) = \beta \in (-\infty,\infty), \qquad \lim_{N\to\infty}\theta_N = \theta \in (0,\infty),N→∞lim​N​(1−ρN​)=β∈(−∞,∞),N→∞lim​θN​=θ∈(0,∞),

and qN(0)⇒νq_N(0) \Rightarrow \nuqN​(0)⇒ν for a probability law ν\nuν on R\mathbb RR. Then

qN⇒qin D[0,∞),q_N \Rightarrow q \quad\text{in } D[0,\infty),qN​⇒qin D[0,∞),

where qqq is the solution of dq=f(q) dt+2μ dbdq = f(q)\,dt + \sqrt{2\mu}\,dbdq=f(q)dt+2μ​db with q(0)∼νq(0) \sim \nuq(0)∼ν, and this solution is unique in law.

Milestone: the limit equation is well posed (Theorem 2, p. 216)

On every probability space with a standard Brownian motion bbb and an independent initial value X0X_0X0​, the equation has a solution adapted to σ(X0,b(s):s≤t)\sigma(X_0, b(s): s \le t)σ(X0​,b(s):s≤t), and any two solutions with the same bbb and initial value are indistinguishable.

Milestone: infinitesimal moments (Appendix C, p. 224)

The infinitesimal expectation μN(x)\mu_N(x)μN​(x) and variance σN2(x)\sigma_N^2(x)σN2​(x) of qNq_NqN​ at the point xxx, as displayed on p. 224, satisfy

lim⁡N→∞μN(x)=f(x),lim⁡N→∞σN2(x)=2μ(x∈R).\lim_{N\to\infty}\mu_N(x) = f(x), \qquad \lim_{N\to\infty}\sigma_N^2(x) = 2\mu \qquad (x \in \mathbb R).N→∞lim​μN​(x)=f(x),N→∞lim​σN2​(x)=2μ(x∈R).

Significance

The result. Theorem 2 is the basis for the paper's QED (quality- and efficiency-driven) approximations QN≈N+qNQ_N \approx N + q\sqrt NQN​≈N+qN​, which give explicit formulas for the probability of delay, the probability of abandonment and the waiting-time distribution in terms of β\betaβ, μ\muμ and θ\thetaθ. Unlike the M/M/NM/M/NM/M/N case, β\betaβ may be of either sign: abandonment keeps the system stable even when the offered load exceeds the number of agents. The resulting square-root staffing rule N=R+βRN = R + \beta\sqrt RN=R+βR​, with R=λ/μR = \lambda/\muR=λ/μ, is used in call-center practice.

Formalizing it. The result is proved in the paper by Stone's criteria for birth–death processes, with uniqueness of the limit equation delegated to the literature. No many-server process limit exists on Prove2Me or in Mathlib. A formal proof would give the first machine-checked heavy-traffic process limit for a many-server queue, and the infrastructure (Poisson time-change representation of a birth–death process, path-space weak convergence to a continuous diffusion, well-posedness of a Lipschitz additive-noise SDE) would serve every other diffusion limit in queueing theory.

Difficulty

The infinitesimal-moment computation is elementary; it identifies the limit but does not prove convergence. The hard step is the passage from generator convergence to weak convergence of processes on D[0,∞)D[0,\infty)D[0,∞): tightness of {qN}\{q_N\}{qN​} in the Skorokhod space, which needs control of the jumps (of size 1/N1/\sqrt N1/N​) and of the unbounded state space, and identification of every limit point as a solution of the equation, which needs uniqueness of the limit. A pointwise limit of the drifts at each fixed xxx is not enough: the convergence has to be controlled locally uniformly along the paths. A finite-dimensional limit at fixed times is weaker than the theorem.

Formalization scope

  • Queue. QNQ_NQN​ is realized by the time-change representation of Mandelbaum, Massey and Reiman (1998), cited by the paper: QN(t)=QN(0)+A(λNt)−S(μ∫0tmin⁡(QN(s),N) ds)−R(θN∫0t(QN(s)−N)+ ds)Q_N(t) = Q_N(0) + A(\lambda_N t) - S(\mu\int_0^t \min(Q_N(s), N)\,ds) - R(\theta_N \int_0^t (Q_N(s)-N)^+\,ds)QN​(t)=QN​(0)+A(λN​t)−S(μ∫0t​min(QN​(s),N)ds)−R(θN​∫0t​(QN​(s)−N)+ds), with A,S,RA, S, RA,S,R independent unit-rate Poisson processes independent of QN(0)Q_N(0)QN​(0). This has the birth–death law above.
  • Time. Paths are functions on R\mathbb RR; every condition is imposed for t≥0t \ge 0t≥0 only. Brownian time is R≥0\mathbb R_{\ge 0}R≥0​.
  • Indexing. NNN is both the index and the number of agents; every hypothesis on the NNN-th system is imposed for N≥1N \ge 1N≥1. λN\lambda_NλN​, θN\theta_NθN​ are real sequences and μ\muμ is fixed.
  • Weak convergence. All QNQ_NQN​ live on one probability space, which is no loss since only their laws matter. qN(0)⇒νq_N(0) \Rightarrow \nuqN​(0)⇒ν is convergence of E g(qN(0))E\,g(q_N(0))Eg(qN​(0)) for every bounded continuous ggg. qN⇒qq_N \Rightarrow qqN​⇒q is stated in coupling form (Skorokhod representation with almost-sure uniform convergence on compact time intervals), which is equivalent to J1J_1J1​ weak convergence when the limit is continuous.
  • Limit. The SDE is pathwise (Lebesgue integral, no Itô integral). Brownian motion is Mathlib's IsBrownianReal with every path continuous and every coordinate measurable. q(0)q(0)q(0) is independent of bbb, which is implicit in the paper. The goal asserts existence of a solution with qN⇒qq_N \Rightarrow qqN​⇒q and uniqueness of its law; dropping the uniqueness clause, fixing ν\nuν to a point mass, restricting to β>0\beta > 0β>0, μ=1\mu = 1μ=1, θ=μ\theta = \muθ=μ, or the stationary case is a different theorem.
  • Infinitesimal moments. Defined exactly as displayed, with ⌊⋅⌋\lfloor\cdot\rfloor⌊⋅⌋ the integer part. The display is printed for θ=0\theta = 0θ=0; the milestone is its 0<θ<∞0 < \theta < \infty0<θ<∞ instance with the limit fff of Theorem 2, pointwise in xxx.
  • Not covered. The cases θ=0\theta = 0θ=0 and θ=∞\theta = \inftyθ=∞ of Theorem 2* and the interchange of limits (Part 2).

Contributions welcome: a Poisson time-change existence theorem, tightness criteria in D[0,∞)D[0,\infty)D[0,∞), well-posedness of Lipschitz SDEs with additive noise, and the martingale-problem approach to identifying limits.

Selected references

  • O. Garnett, A. Mandelbaum, M. Reiman, Designing a Call Center with Impatient Customers, Manufacturing & Service Operations Management 4(3):208–227, 2002. https://doi.org/10.1287/msom.4.3.208.7753
  • S. Halfin, W. Whitt, Heavy-Traffic Limits for Queues with Many Exponential Servers, Operations Research 29(3):567–588, 1981. https://doi.org/10.1287/opre.29.3.567
  • P. J. Fleming, A. Stolyar, B. Simon, Heavy Traffic Limit for a Mobile Phone System Loss Model, Proc. 2nd Int. Conf. on Telecommunication Systems Modeling and Analysis, 1994.
  • A. Mandelbaum, W. A. Massey, M. I. Reiman, Strong Approximations for Markovian Service Networks, Queueing Systems 30:149–201, 1998. https://doi.org/10.1023/A:1019112920622
  • S. N. Ethier, T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. https://doi.org/10.1002/9780470316658
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Algorithmic Game TheoryMachine LearningProbability·Captain: mikedeng1

A Simple Adaptive Procedure Leading to Correlated Equilibrium 1: Under Regret-Matching (2.2), the Empirical Distributions of Play Converge Almost Surely to the Set of Correlated EquilibriaResearch Paper

Motivation

A correlated equilibrium (Aumann 1974) is a probability distribution over strategy profiles of a game such that no player gains by deviating from a recommended strategy, given the recommendation. It is the solution concept of choice when players can condition on common signals, and its set is a convex polytope defined by linear inequalities, which makes it computationally tractable in a way that Nash equilibrium is not. A natural question in learning in games is whether simple adaptive behaviour by individual players, each using only their own payoffs and the observed history, leads to it.

Hart and Mas-Colell (2000) answer this with regret matching: each player switches away from their last action with probabilities proportional to the regret for not having played other actions in the past. They show that if every player uses this rule, the empirical distribution of play converges almost surely to the set of correlated equilibria. The procedure and its analysis became standard references for no-regret learning, internal (swap) regret, and the counterfactual-regret-minimization algorithms used in large imperfect-information games.

Timeline. Foster and Vohra (1997) obtained convergence to correlated equilibria by calibrated forecasting. Fudenberg and Levine (1999) gave conditionally consistent procedures with the same consequence. Hart and Mas-Colell (2000) gave the regret-matching procedure (2.2), in which a player's probabilities depend on regrets only, together with a Blackwell-approachability variant (their Theorem A, the subject of the companion mission 2 of this series).

Setting

A finite game Γ=(N,(Si)i∈N,(ui)i∈N)\Gamma=(N,(S^i)_{i\in N},(u^i)_{i\in N})Γ=(N,(Si)i∈N​,(ui)i∈N​) has a finite set of players NNN, a finite strategy set SiS^iSi for each player, and payoffs ui:S→Ru^i:S\to\mathbb Rui:S→R on S=∏iSiS=\prod_i S^iS=∏i​Si. A probability distribution ψ\psiψ on SSS is a correlated ε\varepsilonε-equilibrium if for every player iii and all j,k∈Sij,k\in S^ij,k∈Si

∑s: si=jψ(s) [ui(k,s−i)−ui(s)]≤ε;\sum_{s:\,s^i=j}\psi(s)\,[u^i(k,s^{-i})-u^i(s)]\le\varepsilon ;s:si=j∑​ψ(s)[ui(k,s−i)−ui(s)]≤ε;

a correlated equilibrium is the case ε=0\varepsilon=0ε=0.

The game is played at t=1,2,…t=1,2,\dotst=1,2,…, producing a history ht=(s1,…,st)h_t=(s_1,\dots,s_t)ht​=(s1​,…,st​). For j,k∈Sij,k\in S^ij,k∈Si the regret of player iii is

Dti(j,k)=1t∑τ≤t: sτi=j[ui(k,sτ−i)−ui(sτ)],Rti(j,k)=max⁡{Dti(j,k),0}:D^i_t(j,k)=\frac1t\sum_{\tau\le t:\,s^i_\tau=j}[u^i(k,s^{-i}_\tau)-u^i(s_\tau)],\qquad R^i_t(j,k)=\max\{D^i_t(j,k),0\}:Dti​(j,k)=t1​τ≤t:sτi​=j∑​[ui(k,sτ−i​)−ui(sτ​)],Rti​(j,k)=max{Dti​(j,k),0}:

the average gain player iii would have had by playing kkk every time they played jjj. Fix μ\muμ with μ>2Mi(mi−1)\mu>2M^i(m^i-1)μ>2Mi(mi−1) for every iii, where Mi≥∣ui∣M^i\ge|u^i|Mi≥∣ui∣ and mi=∣Si∣m^i=|S^i|mi=∣Si∣. Under regret matching (2.2), if player iii last played jjj, then at t+1t+1t+1 they play each k≠jk\ne jk=j with probability Rti(j,k)/μR^i_t(j,k)/\muRti​(j,k)/μ and repeat jjj with the remaining probability; the first-period mixed actions are arbitrary, and given the history the players randomize independently. The empirical distribution of play is zt(s)=1t∣{τ≤t:sτ=s}∣z_t(s)=\frac1t|\{\tau\le t:s_\tau=s\}|zt​(s)=t1​∣{τ≤t:sτ​=s}∣.

Formalization targets

Goal: the Main Theorem

Almost surely, ztz_tzt​ converges to the set of correlated equilibria:

P(∀ε>0 ∃T ∀t>T ∃ψ correlated equilibrium with dist⁡(zt,ψ)<ε)=1.P\Big(\forall\varepsilon>0\ \exists T\ \forall t>T\ \exists\psi\ \text{correlated equilibrium with } \operatorname{dist}(z_t,\psi)<\varepsilon\Big)=1 .P(∀ε>0 ∃T ∀t>T ∃ψ correlated equilibrium with dist(zt​,ψ)<ε)=1.

This is convergence to a set, not to a point; the paper notes that ztz_tzt​ need not converge.

Milestones

They follow the Appendix proof:

  • the PROPOSITION (§3), a deterministic equivalence: lim sup⁡tRti(j,k)≤ε\limsup_t R^i_t(j,k)\le\varepsilonlimsupt​Rti​(j,k)≤ε for all iii and j≠kj\ne kj=k iff ztz_tzt​ converges to the set of correlated ε\varepsilonε-equilibria;
  • positivity of the diagonal of the transition matrix Πt\Pi_tΠt​ of (2.2);
  • Steps M1–M11, with the two LEMMAs used in the proofs of M4 and M7.

The squared distance ρt=∑j≠k[Rt(j,k)]2\rho_t=\sum_{j\ne k}[R_t(j,k)]^2ρt​=∑j=k​[Rt​(j,k)]2 satisfies a block recursion (M1). The cross term is rewritten through the transition probabilities (M2) and compared with a stationary auxiliary process (M3–M5). It then factors into a difference of consecutive matrix powers (M6), which is small (M7). This gives

E[(t+v)2ρt+v∣ht]≤t2ρt+O(v3+tv1/2)(M8).E[(t+v)^2\rho_{t+v}\mid h_t]\le t^2\rho_t+O(v^3+tv^{1/2})\qquad\text{(M8)}.E[(t+v)2ρt+v​∣ht​]≤t2ρt​+O(v3+tv1/2)(M8).

Along tn=⌊n5/3⌋t_n=\lfloor n^{5/3}\rfloortn​=⌊n5/3⌋ this gives ρtn→0\rho_{t_n}\to0ρtn​​→0 a.s. (M9–M10), and then Rt(j,k)→0R_t(j,k)\to0Rt​(j,k)→0 a.s. (M11). A companion item states the strong law for dependent variables that M10 cites.

Significance

The result. The Main Theorem shows that correlated equilibrium is reached by uncoupled play: each player needs only their own payoff function and the history of play, and nothing about the others' payoffs. Steps M10–M11 give more than the goal, namely that every player's internal regrets vanish almost surely. The procedure underlies later work on swap regret, calibrated learning and regret-minimization algorithms for extensive-form games.

Formalizing it. The result is proved in the paper. As far as a search of the platform and the local index shows, it has no machine-checked proof. The mission asks for one, following the paper's eleven steps. Several pieces are general and reusable: a bound on consecutive powers of a stochastic matrix with positive diagonal (LEMMA, proof of M7); a perturbation bound for multi-step transition probabilities (LEMMA, proof of M4); and a strong law of large numbers for martingale differences with general normalizing sequences, which Mathlib does not have in this form.

Difficulty

The natural approach is Blackwell approachability: show that the expected regret vector moves toward the nonpositive orthant in one step. It fails here. The one-step condition holds when a player uses an invariant distribution of Πt\Pi_tΠt​, which is the procedure of Theorem A, but regret matching uses a row of Πt\Pi_tΠt​ instead. The cross term of the one-step recursion therefore does not vanish.

The proof has to work over blocks of vvv periods. Within a block the players' choices are not independent given hth_tht​, because the transition probabilities change with time. The paper therefore compares the play with a process whose transitions are frozen at time ttt. The matrix-power estimate cannot use convergence of Πtw\Pi_t^wΠtw​, since only the diagonal of Πt\Pi_tΠt​ is known to be positive and Πt\Pi_tΠt​ may be reducible or periodic in its off-diagonal structure. The block length must also balance the errors w2/tw^2/tw2/t and w−1/2w^{-1/2}w−1/2, which is why the subsequence tn=⌊n5/3⌋t_n=\lfloor n^{5/3}\rfloortn​=⌊n5/3⌋ appears.

Formalization scope

Players form a Fintype ι, strategies form Fintypes S i, each nonempty, and a profile is a function ∀ i, S i. Δ(Q)\Delta(Q)Δ(Q) is Mathlib's stdSimplex. Time is 0-based: play τ is sτ+1s_{\tau+1}sτ+1​, and a history is a tuple Fin t → ∀ i, S i. Regrets, ztz_tzt​, Πt\Pi_tΠt​ and ρt\rho_tρt​ are deterministic functions of a finite history. Every statement has t≥1t\ge1t≥1, because the Lean value at t=0t=0t=0 is a default. A play of a behaviour profile on a probability space (IsPlay) is a sequence of profile-valued random variables with measurable level sets whose conditional law given any history of positive probability is the product of the players' mixed actions. Statements quantify over every probability space carrying a play, and conditional quantities given hth_tht​ assume P[ht]>0P[h_t]>0P[ht​]>0. The auxiliary s^\hat ss^-process is encoded by its explicit law, a power of the product transition matrix. The paper's O(⋅)O(\cdot)O(⋅) (footnote 34) is a constant chosen after the game, MMM and μ\muμ and before the initial play, the probability space and the play. Distances on RS\mathbb R^SRS are sup distances.

The hypotheses are exactly footnote 5's: ∣ui∣≤Mi|u^i|\le M^i∣ui∣≤Mi and μ>2Mi(mi−1)\mu>2M^i(m^i-1)μ>2Mi(mi−1), with one μ\muμ for all players. The goal requires every player to follow (2.2). If other players may play arbitrarily the statement is false (§4(d)), so IsPlay constrains all of them. The goal is stated with an existential correlated equilibrium at distance less than ε\varepsilonε, not with a distance to a possibly empty set, so no encoding makes it vacuous.

Disclosed choices:

  • the LEMMA of M7 is stated with a constant that depends only on a lower bound on the diagonal, which is what the proof gives and what M7 uses;
  • the PROPOSITION states lim sup⁡≤ε\limsup\le\varepsilonlimsup≤ε as "for every δ>0\delta>0δ>0, eventually ≤ε+δ\le\varepsilon+\delta≤ε+δ";
  • the strong law assumes each XnX_nXn​ is measurable and in L2L^2L2.

Contributions are welcome at every milestone. The two LEMMAs and the strong law are self-contained and independent of the game.

Selected references

  • S. Hart and A. Mas-Colell, A Simple Adaptive Procedure Leading to Correlated Equilibrium, Econometrica 68(5) (2000), 1127–1150. https://doi.org/10.1111/1468-0262.00153
  • R. J. Aumann, Subjectivity and Correlation in Randomized Strategies, Journal of Mathematical Economics 1 (1974), 67–96. https://doi.org/10.1016/0304-4068(74)90037-8
  • D. P. Foster and R. V. Vohra, Calibrated Learning and Correlated Equilibrium, Games and Economic Behavior 21 (1997), 40–55. https://doi.org/10.1006/game.1997.0595
  • D. Fudenberg and D. K. Levine, Conditional Universal Consistency, Games and Economic Behavior 29 (1999), 104–130. https://doi.org/10.1006/game.1998.0705
  • D. Blackwell, An Analog of the Minimax Theorem for Vector Payoffs, Pacific Journal of Mathematics 6 (1956), 1–8. https://doi.org/10.2140/pjm.1956.6.1
  • M. Loève, Probability Theory II, 4th ed., Springer (1978), Theorem 32.1.E.
17 thms2 active usersReviewed
Operations ResearchOptimizationProbability·Captain: mikedeng1

Quantitative Stability in Stochastic Programming: The Method of Probability Metrics 4: Minimal-Risk Stable Portfolios Are Stable in the Stability Index and the Spectral MeasureResearch Paper

Motivation

Stable distributions were proposed as models of asset returns by Mandelbrot and Fama in the 1960s, because empirical returns show heavier tails than the normal law allows; Rachev and Mittnik's monograph Stable Paretian Models in Finance (2000) collects the later development. When the vector ϱ\varrhoϱ of per-share returns of sss assets follows a multivariate α\alphaα-stable law with α∈(1,2)\alpha\in(1,2)α∈(1,2), its distribution is determined by the stability index α\alphaα, a shift m0∈Rsm_0\in\mathbb R^sm0​∈Rs, and a finite Borel measure Γ\GammaΓ on the unit sphere, the spectral measure. The risk of a portfolio is then measured by the scale parameter of the return, and choosing an efficient portfolio becomes a deterministic optimization problem in (α,Γ)(\alpha,\Gamma)(α,Γ).

In practice neither α\alphaα nor Γ\GammaΓ is known: both are estimated from data. Whether the optimal portfolio is robust to estimation error is therefore a practical question. Section 5 of Rachev and Römisch, Quantitative stability in stochastic programming: The method of probability metrics (Math. Oper. Res. 27(4), 2002; this mission follows the authors' preprint), answers it with an explicit modulus, as an application of the paper's general stability theory for stochastic programs under perturbations of the underlying probability measure.

Setting

Fix s∈Ns\in\mathbb Ns∈N and equip Rs\mathbb R^sRs with the Euclidean scalar product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ and norm ∥⋅∥\|\cdot\|∥⋅∥.

  • Σs={ξ∈Rs:⟨ξ,ξ⟩=1}\Sigma^s=\{\xi\in\mathbb R^s:\langle\xi,\xi\rangle=1\}Σs={ξ∈Rs:⟨ξ,ξ⟩=1} is the unit sphere, and P(Σs)\mathcal P(\Sigma^s)P(Σs) is the set of Borel probability measures on it (normalized spectral measures).
  • X={x∈R+s:∑i=1sxi=1}X=\{x\in\mathbb R^s_+:\sum_{i=1}^s x_i=1\}X={x∈R+s​:∑i=1s​xi​=1} is the set of portfolios: xix_ixi​ is the proportion of shares held in asset iii.
  • For α∈(1,2)\alpha\in(1,2)α∈(1,2) and Γ∈P(Σs)\Gamma\in\mathcal P(\Sigma^s)Γ∈P(Σs), the risk of xxx is
rα,Γ(x)=∫Σs∣⟨x,ξ⟩∣α Γ(dξ).r_{\alpha,\Gamma}(x)=\int_{\Sigma^s}|\langle x,\xi\rangle|^\alpha\,\Gamma(d\xi).rα,Γ​(x)=∫Σs​∣⟨x,ξ⟩∣αΓ(dξ).
  • Problem (22) is min⁡{rα,Γ(x):x∈X}\min\{r_{\alpha,\Gamma}(x):x\in X\}min{rα,Γ​(x):x∈X}, with optimal value v(α,Γ)v(\alpha,\Gamma)v(α,Γ) and solution set S(α,Γ)S(\alpha,\Gamma)S(α,Γ).
  • The dual Lipschitz metric ζ1\zeta_1ζ1​ (the Fortet–Mourier metric of order 111) on P(Σs)\mathcal P(\Sigma^s)P(Σs) is
ζ1(Γ,Γ~)=sup⁡{∣∫Σsf dΓ−∫Σsf dΓ~∣:f:Σs→R, ∣f(ξ)−f(ξ~)∣≤∥ξ−ξ~∥}.\zeta_1(\Gamma,\tilde\Gamma)=\sup\Big\{\Big|\int_{\Sigma^s}f\,d\Gamma-\int_{\Sigma^s}f\,d\tilde\Gamma\Big|: f:\Sigma^s\to\mathbb R,\ |f(\xi)-f(\tilde\xi)|\le\|\xi-\tilde\xi\|\Big\}.ζ1​(Γ,Γ~)=sup{​∫Σs​fdΓ−∫Σs​fdΓ~​:f:Σs→R, ∣f(ξ)−f(ξ~​)∣≤∥ξ−ξ~​∥}.
  • The growth function of (22) is ψ(τ)=min⁡{rα,Γ(x)−v(α,Γ):d(x,S(α,Γ))≥τ, x∈X}\psi(\tau)=\min\{r_{\alpha,\Gamma}(x)-v(\alpha,\Gamma): d(x,S(\alpha,\Gamma))\ge\tau,\ x\in X\}ψ(τ)=min{rα,Γ​(x)−v(α,Γ):d(x,S(α,Γ))≥τ, x∈X} for τ≥0\tau\ge0τ≥0, its generalized inverse is ψ−1(t)=sup⁡{τ≥0:ψ(τ)≤t}\psi^{-1}(t)=\sup\{\tau\ge0:\psi(\tau)\le t\}ψ−1(t)=sup{τ≥0:ψ(τ)≤t}, and the stability modulus is Ψ(η)=η+ψ−1(2η)\Psi(\eta)=\eta+\psi^{-1}(2\eta)Ψ(η)=η+ψ−1(2η).
  • Γ\GammaΓ is nonsingular if ∫Σs∣⟨x,ξ⟩∣2Γ(dξ)=0\int_{\Sigma^s}|\langle x,\xi\rangle|^2\Gamma(d\xi)=0∫Σs​∣⟨x,ξ⟩∣2Γ(dξ)=0 implies x=0x=0x=0.

Formalization targets

Goal: Theorem 5.2, first assertion (p. 25)

For each (α,Γ)∈(1,2)×P(Σs)(\alpha,\Gamma)\in(1,2)\times\mathcal P(\Sigma^s)(α,Γ)∈(1,2)×P(Σs) there is δ>0\delta>0δ>0 such that

sup⁡x∈S(α~,Γ~)d(x,S(α,Γ))≤Ψ(α ζ1(Γ,Γ~)+e−1∣α−α~∣)\sup_{x\in S(\tilde\alpha,\tilde\Gamma)}d\big(x,S(\alpha,\Gamma)\big)\le\Psi\big(\alpha\,\zeta_1(\Gamma,\tilde\Gamma)+e^{-1}|\alpha-\tilde\alpha|\big)x∈S(α~,Γ~)sup​d(x,S(α,Γ))≤Ψ(αζ1​(Γ,Γ~)+e−1∣α−α~∣)

whenever (α~,Γ~)∈(1,2)×P(Σs)(\tilde\alpha,\tilde\Gamma)\in(1,2)\times\mathcal P(\Sigma^s)(α~,Γ~)∈(1,2)×P(Σs) and ζ1(Γ,Γ~)+∣α−α~∣<δ\zeta_1(\Gamma,\tilde\Gamma)+|\alpha-\tilde\alpha|<\deltaζ1​(Γ,Γ~)+∣α−α~∣<δ. The modulus Ψ\PsiΨ is not fixed: it is whatever the growth of the unperturbed problem gives.

Companion: Theorem 5.2, "Moreover" (p. 25)

If Γ\GammaΓ is nonsingular, then (22) has a unique solution and Ψ(η)≤Cη1/2\Psi(\eta)\le C\eta^{1/2}Ψ(η)≤Cη1/2 for some C>0C>0C>0 and all sufficiently small η≥0\eta\ge0η≥0.

Milestones

  1. Lemma 5.1, first assertion (p. 24): f0(ξ,x)=∣⟨x,ξ⟩∣αf_0(\xi,x)=|\langle x,\xi\rangle|^\alphaf0​(ξ,x)=∣⟨x,ξ⟩∣α is convex in xxx, and ∣f0(ξ,x)−f0(ξ~,x~)∣≤α(∥ξ−ξ~∥+∥x−x~∥)|f_0(\xi,x)-f_0(\tilde\xi,\tilde x)|\le\alpha(\|\xi-\tilde\xi\|+\|x-\tilde x\|)∣f0​(ξ,x)−f0​(ξ~​,x~)∣≤α(∥ξ−ξ~​∥+∥x−x~∥) on Σs×X\Sigma^s\times XΣs×X.
  2. Lemma 5.1, second assertion (p. 24): S(α,Γ)≠∅S(\alpha,\Gamma)\ne\emptysetS(α,Γ)=∅, and 14α(α−1)∫Σs∣⟨x−x∗,z⟩∣2Γ(dz)≤rα,Γ(x)−v(α,Γ)\frac14\alpha(\alpha-1)\int_{\Sigma^s}|\langle x-x_*,z\rangle|^2\Gamma(dz)\le r_{\alpha,\Gamma}(x)-v(\alpha,\Gamma)41​α(α−1)∫Σs​∣⟨x−x∗​,z⟩∣2Γ(dz)≤rα,Γ​(x)−v(α,Γ) for all x∈Xx\in Xx∈X and some x∗∈S(α,Γ)x_*\in S(\alpha,\Gamma)x∗​∈S(α,Γ).
  3. Proof of Theorem 5.2 (p. 25): sup⁡t∈[−1,1]∣∣t∣α−∣t∣α~∣≤e−1∣α−α~∣\sup_{t\in[-1,1]}\big||t|^\alpha-|t|^{\tilde\alpha}\big|\le e^{-1}|\alpha-\tilde\alpha|supt∈[−1,1]​​∣t∣α−∣t∣α~​≤e−1∣α−α~∣.
  4. Proof of Theorem 5.2 (p. 25): ∣rα,Γ(x)−rα~,Γ~(x)∣≤αζ1(Γ,Γ~)+e−1∣α−α~∣|r_{\alpha,\Gamma}(x)-r_{\tilde\alpha,\tilde\Gamma}(x)|\le\alpha\zeta_1(\Gamma,\tilde\Gamma)+e^{-1}|\alpha-\tilde\alpha|∣rα,Γ​(x)−rα~,Γ~​(x)∣≤αζ1​(Γ,Γ~)+e−1∣α−α~∣ for x∈Xx\in Xx∈X.
  5. Proof of Theorem 5.2 (p. 25): for nonsingular Γ\GammaΓ, c∥x∥2≤∫Σs∣⟨x,ξ⟩∣2Γ(dξ)c\|x\|^2\le\int_{\Sigma^s}|\langle x,\xi\rangle|^2\Gamma(d\xi)c∥x∥2≤∫Σs​∣⟨x,ξ⟩∣2Γ(dξ) for some c=c(s,Γ)>0c=c(s,\Gamma)>0c=c(s,Γ)>0.
  6. Proof of Theorem 5.2 (p. 25): for nonsingular Γ\GammaΓ, (22) has a unique solution x∗x_*x∗​ and 14cα(α−1)∥x−x∗∥2≤rα,Γ(x)−v(α,Γ)\frac14c\alpha(\alpha-1)\|x-x_*\|^2\le r_{\alpha,\Gamma}(x)-v(\alpha,\Gamma)41​cα(α−1)∥x−x∗​∥2≤rα,Γ​(x)−v(α,Γ) on XXX.

Significance

The theorem bounds how far the optimal portfolios can move when the stability index and the spectral measure are both perturbed, with a modulus computed from the unperturbed problem alone. Combined with the companion, the efficient portfolio of a nonsingular spectral measure is unique and moves by at most O((ζ1(Γ,Γ~)+∣α−α~∣)1/2)O\big((\zeta_1(\Gamma,\tilde\Gamma)+|\alpha-\tilde\alpha|)^{1/2}\big)O((ζ1​(Γ,Γ~)+∣α−α~∣)1/2). Since ζ1\zeta_1ζ1​ metrizes weak convergence on the compact sphere, any consistent estimator of Γ\GammaΓ in the weak topology, together with a consistent estimator of α\alphaα, yields consistent estimates of the optimal portfolio, and convergence rates for ζ1\zeta_1ζ1​ translate into rates for the portfolio. The paper notes (Example 5.3) that spectral measures of linear transformations of independent stable variables with a full-rank matrix are nonsingular, so the Hölder case covers the discrete spectral measures used in practice.

The result is proved in the paper; nothing here is open. To our knowledge none of it is machine-checked: Mathlib has strong convexity and the real power function but no stability theory of stochastic programs and no Fortet–Mourier metrics. The mission produces a checked proof of the result and a reusable formal treatment of the growth-function modulus Ψ\PsiΨ in a concrete, fully explicit instance.

Difficulty

The obvious argument compares the optimal values of the two problems and concludes that a perturbed minimizer is nearly optimal for the unperturbed problem. Turning near-optimality into a distance bound requires the growth function ψ\psiψ and its generalized inverse; ψ\psiψ is defined by an infimum over a set that may be empty, and ψ−1\psi^{-1}ψ−1 by a supremum that may be infinite, so this step has to be handled in extended arithmetic with care. A second difficulty is the ζ1\zeta_1ζ1​ term: the map ξ↦∣⟨x,ξ⟩∣α\xi\mapsto|\langle x,\xi\rangle|^\alphaξ↦∣⟨x,ξ⟩∣α must be shown to be α\alphaα-Lipschitz on the sphere uniformly over x∈Xx\in Xx∈X, which uses ∥x∥≤1\|x\|\le1∥x∥≤1 on the simplex. The change of exponent from α\alphaα to α~\tilde\alphaα~ is controlled by a sharp calculus inequality whose constant e−1e^{-1}e−1 needs α,α~≥1\alpha,\tilde\alpha\ge1α,α~≥1. In the nonsingular case, the quadratic form ∫∣⟨x,ξ⟩∣2Γ(dξ)\int|\langle x,\xi\rangle|^2\Gamma(d\xi)∫∣⟨x,ξ⟩∣2Γ(dξ) must be shown to dominate c∥x∥2c\|x\|^2c∥x∥2, a compactness argument on the unit sphere of Rs\mathbb R^sRs.

Formalization scope

  • Rs\mathbb R^sRs is EuclideanSpace ℝ (Fin s) with coordinates indexed 0,…,s−10,\dots,s-10,…,s−1. The paper says "the (Euclidean) scalar product", so Euclidean norms are the paper's own.
  • Σs\Sigma^sΣs is Metric.sphere 0 1. A spectral measure is a probability measure on Rs\mathbb R^sRs with Γ((Σs)c)=0\Gamma((\Sigma^s)^c)=0Γ((Σs)c)=0, and every integral is a set integral over Σs\Sigma^sΣs. For s=0s=0s=0 the sphere is empty, no spectral measure exists, and every statement is vacuous, as in the paper.
  • The standing assumption α∈(1,2)\alpha\in(1,2)α∈(1,2) of Section 5 is a hypothesis of every statement. The α\alphaα-stable law itself is not formalized: the characteristic function on p. 23 only motivates (22), and the mission captures problem (22) exactly.
  • ζ1\zeta_1ζ1​ is a supremum in [0,∞][0,\infty][0,∞] over functions on Rs\mathbb R^sRs that are 111-Lipschitz on Σs\Sigma^sΣs, integrated over Σs\Sigma^sΣs only. Such functions are continuous on the compact sphere, so no integral can collapse to a default value. For probability measures, ζ1≤2\zeta_1\le2ζ1​≤2.
  • vvv is the real infimum of rα,Γr_{\alpha,\Gamma}rα,Γ​ over XXX. SSS is the set of minimizers. The paper's "min" in ψ\psiψ is read as an infimum in the extended reals, equal to +∞+\infty+∞ when no feasible point is at distance at least τ\tauτ. Distances to sets are extended distances (Metric.infEDist, +∞+\infty+∞ to the empty set), and ψ−1\psi^{-1}ψ−1 and Ψ\PsiΨ take values in [0,∞][0,\infty][0,∞].
  • Ruled out: a real-valued supremum for ψ−1\psi^{-1}ψ−1 (which would be 000 on unbounded sets), a real distance (which is 000 to the empty set), and test functions integrated over all of Rs\mathbb R^sRs (whose off-sphere values could make an integral undefined). Any of these would make the goal trivially true.
  • "Sufficiently small η\etaη" is read as "all η∈[0,η0]\eta\in[0,\eta_0]η∈[0,η0​] for some η0>0\eta_0>0η0​>0". Milestone 6 holds for every constant c>0c>0c>0 of the norm bound of milestone 5, fixed before α\alphaα, as c=c(s,Γ)c=c(s,\Gamma)c=c(s,Γ) on the page.

Welcome contributions: the inequality ∣∣t∣α−∣t∣α~∣≤e−1∣α−α~∣\big||t|^\alpha-|t|^{\tilde\alpha}\big|\le e^{-1}|\alpha-\tilde\alpha|​∣t∣α−∣t∣α~​≤e−1∣α−α~∣ on [−1,1][-1,1][−1,1], strong convexity of ∣t∣α|t|^\alpha∣t∣α on [−1,1][-1,1][−1,1], and a general lemma converting a growth function and a uniform objective perturbation into a distance bound; the last is reusable for every stability result of the paper.

Selected references

  • S. T. Rachev, W. Römisch, Quantitative stability in stochastic programming: The method of probability metrics, Mathematics of Operations Research 27(4) (2002) 792–818. https://doi.org/10.1287/moor.27.4.792.304 (preprint at edoc.hu-berlin.de, followed here).
  • S. T. Rachev, S. Mittnik, Stable Paretian Models in Finance, Wiley, Chichester, 2000 (reference [33] of the paper).
  • G. Samorodnitsky, M. S. Taqqu, Stable Non-Gaussian Random Processes, Chapman & Hall, 1994. https://doi.org/10.1201/9780203738818
  • B. Mandelbrot, The variation of certain speculative prices, Journal of Business 36(4) (1963) 394–419. https://doi.org/10.1086/294632
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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A Coordinate Gradient Descent Method for Nonsmooth Separable Minimization 3: The Local Lipschitzian Error Bound Holds for Polyhedral P with Quadratic or Composite f, and for Strongly Convex fResearch Paper

Motivation

Many problems in statistics, signal processing and machine learning minimize the sum of a smooth function and a convex but nonsmooth one: ℓ1\ell_1ℓ1​-regularized least squares (the Lasso), bound-constrained problems, and group-sparse regression are standard examples. Tseng and Yun (Math. Program. Ser. B 117 (2009) 387–423) proposed the coordinate gradient descent (CGD) method for this class and proved that it converges linearly under a local Lipschitzian error bound, Assumption 2(a) of their paper. An assumption is only as useful as the list of problems known to satisfy it. Section 6 of the paper supplies that list, and this mission formalizes it.

Error bounds of this kind have a history in smooth constrained optimization. Luo and Tseng proved them for quadratic objectives over polyhedral sets (Luo–Tseng 1992, SIAM J. Optim.), for strongly convex functions composed with a linear map (Luo–Tseng 1992, SIAM J. Control Optim.), and for dual functionals of linearly constrained strictly convex programs (Luo–Tseng 1993, Math. Oper. Res.), and used them to derive linear rates for feasible descent methods (Luo–Tseng 1993, Ann. Oper. Res.). Tseng and Yun carry these results over to the nonsmooth problem (1) by reformulating it as a smooth problem over the epigraph of the nonsmooth part.

Setting

Throughout, Rn\mathbb R^nRn carries the Euclidean norm ∥⋅∥\|\cdot\|∥⋅∥. The problem is

min⁡x  Fc(x)=f(x)+cP(x),(1)\min_x\; F_c(x) = f(x) + cP(x), \qquad (1)xmin​Fc​(x)=f(x)+cP(x),(1)

where c>0c > 0c>0, P:Rn→(−∞,∞]P:\mathbb R^n \to (-\infty,\infty]P:Rn→(−∞,∞] is proper, convex and lower semicontinuous with effective domain dom⁡P={x∣P(x)<∞}\operatorname{dom}P = \{x \mid P(x) < \infty\}domP={x∣P(x)<∞}, and fff is continuously differentiable on an open set containing dom⁡P\operatorname{dom}PdomP.

The residual at x∈dom⁡Px \in \operatorname{dom}Px∈domP is

dI(x)=arg⁡min⁡d{∇f(x)⊤d+12∥d∥2+cP(x+d)},d_I(x) = \arg\min_d \Big\{\nabla f(x)^\top d + \tfrac12\|d\|^2 + cP(x+d)\Big\},dI​(x)=argdmin​{∇f(x)⊤d+21​∥d∥2+cP(x+d)},

the unique minimizer of a strongly convex function. A point x∈dom⁡Px \in \operatorname{dom}Px∈domP is stationary if the one-sided directional derivative satisfies Fc′(x;d)≥0F_c'(x;d) \ge 0Fc′​(x;d)≥0 for every direction ddd; Xˉ\bar XXˉ denotes the set of stationary points and dist⁡(x,Xˉ)\operatorname{dist}(x,\bar X)dist(x,Xˉ) the distance to it. A point is stationary exactly when its residual vanishes.

Assumption 2(a) asks that Xˉ≠∅\bar X \neq \emptysetXˉ=∅ and that for every level ζ\zetaζ there be constants τ,ϵ>0\tau, \epsilon > 0τ,ϵ>0 with

dist⁡(x,Xˉ)≤τ∥dI(x)∥whenever Fc(x)≤ζ, ∥dI(x)∥≤ϵ.\operatorname{dist}(x,\bar X) \le \tau\|d_I(x)\| \quad\text{whenever } F_c(x) \le \zeta,\ \|d_I(x)\| \le \epsilon.dist(x,Xˉ)≤τ∥dI​(x)∥whenever Fc​(x)≤ζ, ∥dI​(x)∥≤ϵ.

Writing epi⁡P={(x,ξ)∣P(x)≤ξ}\operatorname{epi}P = \{(x,\xi) \mid P(x) \le \xi\}epiP={(x,ξ)∣P(x)≤ξ}, problem (1) is equivalent to the smooth problem min⁡{f(x)+cξ∣(x,ξ)∈epi⁡P}\min\{f(x) + c\xi \mid (x,\xi) \in \operatorname{epi}P\}min{f(x)+cξ∣(x,ξ)∈epiP} (41). Its projection residual at (x,ξ)(x,\xi)(x,ξ) is the optimal solution (d~,δ~)(\tilde d,\tilde\delta)(d~,δ~) of

min⁡(d,δ){∇f(x)⊤d+12∥d∥2+12δ2+cδ  ∣  (x+d,ξ+δ)∈epi⁡P}.(42)\min_{(d,\delta)}\Big\{\nabla f(x)^\top d + \tfrac12\|d\|^2 + \tfrac12\delta^2 + c\delta \;\Big|\; (x+d,\xi+\delta) \in \operatorname{epi}P\Big\}. \qquad (42)(d,δ)min​{∇f(x)⊤d+21​∥d∥2+21​δ2+cδ​(x+d,ξ+δ)∈epiP}.(42)

PPP is polyhedral if epi⁡P\operatorname{epi}PepiP is the solution set of finitely many linear inequalities in (x,ξ)(x,\xi)(x,ξ); fff is quadratic if f(x)=12x⊤Ax+b⊤x+c0f(x) = \tfrac12 x^\top Ax + b^\top x + c_0f(x)=21​x⊤Ax+b⊤x+c0​ with AAA symmetric, not necessarily positive semidefinite. The four problem classes are:

  • C1: fff quadratic, PPP polyhedral;
  • C2: f(x)=g(Ex)+q⊤xf(x) = g(Ex) + q^\top xf(x)=g(Ex)+q⊤x with ggg strongly convex and differentiable on Rm\mathbb R^mRm, ∇g\nabla g∇g Lipschitz, PPP polyhedral;
  • C3: f(x)=max⁡y∈Y{(Ex)⊤y−g(y)}+q⊤xf(x) = \max_{y\in Y}\{(Ex)^\top y - g(y)\} + q^\top xf(x)=maxy∈Y​{(Ex)⊤y−g(y)}+q⊤x with YYY polyhedral and ggg as in C2, PPP polyhedral;
  • C4: fff strongly convex with ∇f\nabla f∇f Lipschitz on dom⁡P\operatorname{dom}PdomP (condition (22)).

Formalization targets

Goal: Theorem 4 (p. 412)

(Xˉ≠∅ ∧ (C1∨C2∨C3)) ∨ C4  ⟹  Assumption 2(a).\Big(\bar X \neq \emptyset \ \wedge\ (\mathrm{C1} \vee \mathrm{C2} \vee \mathrm{C3})\Big) \ \vee\ \mathrm{C4} \;\Longrightarrow\; \text{Assumption 2(a)}.(Xˉ=∅ ∧ (C1∨C2∨C3)) ∨ C4⟹Assumption 2(a).

Under C4, nonemptiness of Xˉ\bar XXˉ is part of the conclusion. The constants τ,ϵ\tau, \epsilonτ,ϵ are existential, so the goal does not depend on any particular estimate.

Milestone: Lemma 6 (p. 410)

If PPP is Lipschitz on dom⁡P\operatorname{dom}PdomP with constant KKK, there is κ>0\kappa > 0κ>0 depending only on KKK with

∥(d~,δ~)∥≤κ ∥dI(x)∥(x∈dom⁡P, ξ=P(x)).\|(\tilde d,\tilde\delta)\| \le \kappa\,\|d_I(x)\| \qquad (x \in \operatorname{dom}P,\ \xi = P(x)).∥(d~,δ~)∥≤κ∥dI​(x)∥(x∈domP, ξ=P(x)).

Milestone: Lemma 7 (p. 411)

If Xˉ≠∅\bar X \neq \emptysetXˉ=∅ and C1, C2 or C3 holds, then for every ζ\zetaζ there are τ′,ϵ′>0\tau', \epsilon' > 0τ′,ϵ′>0 with

dist⁡(x,Xˉ)≤τ′∥(d~,δ~)∥whenever Fc(x)≤ζ, ∥(d~,δ~)∥≤ϵ′,(44)\operatorname{dist}(x,\bar X) \le \tau'\|(\tilde d,\tilde\delta)\| \quad\text{whenever } F_c(x) \le \zeta,\ \|(\tilde d,\tilde\delta)\| \le \epsilon', \qquad (44)dist(x,Xˉ)≤τ′∥(d~,δ~)∥whenever Fc​(x)≤ζ, ∥(d~,δ~)∥≤ϵ′,(44)

where (d~,δ~)(\tilde d,\tilde\delta)(d~,δ~) solves (42) with ξ=P(x)\xi = P(x)ξ=P(x).

A further item, not a milestone, states the remark after Assumption 2 (p. 404) that Assumption 2(b) (stationary points with different objective values are uniformly separated) holds whenever fff is convex.

Significance

Theorem 4 is what makes the linear convergence theorem of the paper (Theorem 2, the subject of the second mission of this series) applicable. Through C1 it covers every problem with a quadratic fff and a polyhedral PPP, including the Lasso and ℓ1\ell_1ℓ1​-regularized or bound-constrained quadratic programs, without convexity of fff. Through C2 it covers losses of the form g(Ex)g(Ex)g(Ex) with ggg strongly convex, such as least squares 12∥Ex−b∥2\tfrac12\|Ex - b\|^221​∥Ex−b∥2, where fff itself is not strongly convex because EEE may have a nontrivial kernel. These error bounds became a standard tool for linear rates of proximal and coordinate methods without strong convexity.

The paper's result is proved, but Lemma 7 is proved by citation: it applies three error bounds of Luo and Tseng to the reformulation (41). A complete formalization therefore requires those error bounds for smooth problems over polyhedral sets, which are not in Mathlib. To our knowledge none of the results of this mission has a machine-checked proof.

Difficulty

Lemma 6 and the C4 case of Theorem 4 are short inequality arguments. The difficulty is Lemma 7. The natural first idea, proving an error bound from strong convexity, fails for C1–C3: fff may be nonconvex (C1) or have a degenerate Hessian (C2, C3), and the objective f(x)+cξf(x) + c\xif(x)+cξ of (41) is never strongly convex in (x,ξ)(x,\xi)(x,ξ). What replaces strong convexity is the polyhedral structure of epi⁡P\operatorname{epi}PepiP, and the cited Luo–Tseng error bounds that exploit it are substantial results in their own right, each of which has to be established for a projection residual over a general polyhedron in Rn+1\mathbb R^{n+1}Rn+1.

Formalization scope

Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n), with indices 0,…,n−10,\dots,n-10,…,n−1. PPP is the pair (D,P)(D, P)(D,P), its effective domain and its finite values there, with "proper, convex, lsc" given by the published ProxNewton.Inexact.IsProperClosedConvex. The value +∞+\infty+∞ is never computed: every statement quantifies over x∈Dx \in Dx∈D, and membership in epi⁡P\operatorname{epi}PepiP is x + d ∈ D ∧ P (x + d) ≤ ξ + δ. dI(x)d_I(x)dI​(x) is a chosen minimizer of its subproblem, which at x∈Dx \in Dx∈D is the paper's unique one. The solutions of (42) enter through a predicate, and every bound is asserted for every optimal solution. Stationarity is the liminf form of Fc′(x;d)≥0F_c'(x;d) \ge 0Fc′​(x;d)≥0. dist⁡\operatorname{dist}dist is the infimum distance. Assumption 2(a) quantifies over every real ζ\zetaζ, which agrees with the paper's "ζ≥min⁡Fc\zeta \ge \min F_cζ≥minFc​" because the condition is vacuous below inf⁡Fc\inf F_cinfFc​. In Lemma 6 the constant κ\kappaκ is quantified before the dimension and the data, so it depends on the Lipschitz constant only.

Explicit choices relative to the printed text:

  • In C4, strong convexity and (22) are required on dom⁡P\operatorname{dom}PdomP only, since fff is only assumed smooth near dom⁡P\operatorname{dom}PdomP. This hypothesis is weaker than the paper's, so the formal theorem is at least as strong.
  • In C2 and C3, EEE is a continuous linear map Rn→Rm\mathbb R^n \to \mathbb R^mRn→Rm (equivalently an m×nm \times nm×n matrix). Strong convexity has a positive modulus and ∇g\nabla g∇g is globally Lipschitz.
  • In C3, the maximum must be attained at every xxx, which forces Y≠∅Y \neq \emptysetY=∅, as the paper's formula presumes.
  • Assumption 2(b) for convex fff is stated with convexity on dom⁡P\operatorname{dom}PdomP.

A polyhedrality notion that admits only affine or constant PPP, an Assumption 2(a) whose constants are chosen after xxx, and a Lemma 7 whose residual is dI(x)d_I(x)dI​(x) instead of the solution of (42) would all trivialize or change the statements. The encoding rules out each of them: polyhedral means a finite system of linear inequalities in (x,ξ)(x,\xi)(x,ξ), the constants precede xxx, and Lemma 7 is stated for (42).

Welcome contributions: proofs of Lemma 6 and of the C4 case; Lipschitz continuity of polyhedral functions on their domain (Rockafellar–Wets, Example 9.35); the Luo–Tseng error bounds for affine variational inequalities and for composite strongly convex objectives over polyhedra, which can be reused well beyond this mission.

Selected references

  • P. Tseng, S. Yun, A coordinate gradient descent method for nonsmooth separable minimization, Math. Program. Ser. B 117 (2009) 387–423. https://doi.org/10.1007/s10107-007-0170-0
  • Z.-Q. Luo, P. Tseng, Error bounds and the convergence analysis of matrix splitting algorithms for the affine variational inequality problem, SIAM J. Optim. 2 (1992) 43–54. https://doi.org/10.1137/0802004
  • Z.-Q. Luo, P. Tseng, On the linear convergence of descent methods for convex essentially smooth minimization, SIAM J. Control Optim. 30 (1992) 408–425. https://doi.org/10.1137/0330025
  • Z.-Q. Luo, P. Tseng, On the convergence rate of dual ascent methods for linearly constrained convex minimization, Math. Oper. Res. 18 (1993) 846–867. https://doi.org/10.1287/moor.18.4.846
  • Z.-Q. Luo, P. Tseng, Error bounds and convergence analysis of feasible descent methods: a general approach, Ann. Oper. Res. 46 (1993) 157–178. https://doi.org/10.1007/BF02096261
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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AnalysisOperations ResearchProbability+2·Captain: mikedeng1

Some Useful Functions for Functional Limit Theorems 3: The First-Passage-Time Map Is M₁-Continuous and J₁-Continuous at Strictly Increasing PathsResearch Paper

Why first passage times need a continuity theorem

Functional limit theorems in queueing and applied probability are rarely proved from scratch. A limit theorem is established once for a primitive process, such as a random walk, a cumulative input or a renewal-reward process, and then transferred to the quantities of interest through the continuous mapping theorem: if Xn⇒XX_n \Rightarrow XXn​⇒X in a function space and fff is continuous at almost every path of XXX, then f(Xn)⇒f(X)f(X_n) \Rightarrow f(X)f(Xn​)⇒f(X). The method works only if the functions in use are known to be continuous, and in which topology.

Ward Whitt's 1980 paper supplies these facts for composition, addition, the supremum, the reflecting barrier, the inverse or first passage time, and time reversal. This mission covers §7, the first passage time. Its role in applications is direct: the counting process of a renewal process is the first passage time of the partial-sum process. A limit theorem for cumulative work can therefore yield one for the number of completed jobs, and a limit theorem for a cumulative input can yield one for the time it takes to reach a level, when the mapping theorem's hypotheses hold.

Timeline. Skorohod (1956) introduced the topologies J1J_1J1​ and M1M_1M1​ on the space DDD of right-continuous paths with left limits. Vervaat (1972) studied functional central limit theorems for processes with positive drift and their inverses, and Whitt (1971) studied weak convergence of first passage time processes. Whitt's 1980 paper restates M1M_1M1​ continuity (Theorem 7.1) and adds the J1J_1J1​ result: the map is continuous at every strictly increasing path (Theorem 7.2), although it is not J1J_1J1​-continuous on its whole domain.

Setting

A path is a function x:[0,∞)→Rx : [0,\infty) \to \mathbb Rx:[0,∞)→R. It belongs to D=D([0,∞),R)D = D([0,\infty),\mathbb R)D=D([0,∞),R) when it is right-continuous and has a left limit at every t>0t > 0t>0.

  • J1J_1J1​ convergence. On a compact interval [0,b][0,b][0,b], xn→xx_n \to xxn​→x in J1J_1J1​ when there are increasing homeomorphisms λn\lambda_nλn​ of [0,b][0,b][0,b] with sup⁡t∣λn(t)−t∣→0\sup_t |\lambda_n(t) - t| \to 0supt​∣λn​(t)−t∣→0 and sup⁡t∣xn(t)−x(λn(t))∣→0\sup_t |x_n(t) - x(\lambda_n(t))| \to 0supt​∣xn​(t)−x(λn​(t))∣→0. On [0,∞)[0,\infty)[0,∞) this is required on [0,b][0,b][0,b] for every bbb at which xxx is continuous.
  • UUU convergence. Uniform convergence on compact subintervals.
  • M1M_1M1​ convergence. The completed graph of xxx on [0,b][0,b][0,b] adds to the graph the vertical segment joining x(t−)x(t-)x(t−) and x(t)x(t)x(t) at each jump. xn→xx_n \to xxn​→x in M1M_1M1​ when the completed graphs admit parametric representations (continuous, order-preserving maps from [0,1][0,1][0,1] onto the completed graph) that are uniformly close in both time and space.
  • The supremum. x↑(t)=sup⁡0≤s≤tx(s)x^{\uparrow}(t) = \sup_{0 \le s \le t} x(s)x↑(t)=sup0≤s≤t​x(s).
  • The domain EEE. The set of x∈Dx \in Dx∈D that are unbounded above and have x(0)≥0x(0) \ge 0x(0)≥0.
  • First passage time. For x∈Ex \in Ex∈E,
x−1(t)=inf⁡{s≥0:x(s)>t},t≥0.x^{-1}(t) = \inf\{s \ge 0 : x(s) > t\}, \qquad t \ge 0.x−1(t)=inf{s≥0:x(s)>t},t≥0.
  • D0D_0D0​. The nondecreasing paths in DDD, and CCC the continuous ones.

Formalization targets

Goal: Theorem 7.2, continuity clause

If xn,x∈Ex_n, x \in Exn​,x∈E, xxx is strictly increasing, and xn→xx_n \to xxn​→x in J1J_1J1​, then

xn−1→x−1(J1).x_n^{-1} \to x^{-1} \quad (J_1).xn−1​→x−1(J1​).

The theorem says that every strictly increasing path is a continuity point of the first passage time map for J1J_1J1​. It fixes no constants, so a sharper variant of a milestone does not invalidate it.

Milestones

  1. J1J_1J1​ convergence implies M1M_1M1​ convergence (§6, p. 80).
  2. The supremum map is M1M_1M1​-continuous on paths with x(0)≥0x(0) \ge 0x(0)≥0 (§6, p. 80, as used in the proof of Theorem 7.1).
  3. x∈Ex \in Ex∈E implies x−1∈E∩D0([0,∞),[0,∞))x^{-1} \in E \cap D_0([0,\infty),[0,\infty))x−1∈E∩D0​([0,∞),[0,∞)) (§7, p. 82).
  4. x↑∈Ex^{\uparrow} \in Ex↑∈E and (x↑)−1=x−1(x^{\uparrow})^{-1} = x^{-1}(x↑)−1=x−1 (proof of Theorem 7.1).
  5. Theorem 7.1. If xn,x∈Ex_n, x \in Exn​,x∈E and xn→xx_n \to xxn​→x in M1M_1M1​, then xn−1→x−1x_n^{-1} \to x^{-1}xn−1​→x−1 in M1M_1M1​.
  6. For strictly increasing x∈Ex \in Ex∈E, x−1x^{-1}x−1 is continuous with x−1(0)=0x^{-1}(0) = 0x−1(0)=0.
  7. M1M_1M1​ convergence to a continuous limit starting at 000 is UUU convergence.
  8. UUU convergence implies J1J_1J1​ convergence.
  9. Theorem 7.4. If cn→∞c_n \to \inftycn​→∞, xn∈Ex_n \in Exn​∈E, cn(xn↑−e)→xc_n(x_n^{\uparrow} - e) \to xcn​(xn↑​−e)→x and cn(xn−1−e)→−xc_n(x_n^{-1} - e) \to -xcn​(xn−1​−e)→−x in J1J_1J1​, then x∈Cx \in Cx∈C.

Significance

The result. Theorem 7.2 lets J1J_1J1​ functional limit theorems pass to first passage times when the limit has strictly increasing paths. The typical case is the fluid limit x(t)=μtx(t) = \mu tx(t)=μt of a cumulative process, with μ>0\mu>0μ>0. Together with the composition results of §3, it supports Theorem 7.3's centered inverse limit: if cn→∞c_n \to \inftycn​→∞, xn∈Ex_n \in Exn​∈E, x(0)=0x(0)=0x(0)=0, xxx has no positive jumps, and cn(xn−e)→xc_n(x_n-e) \to xcn​(xn​−e)→x in J1J_1J1​, then cn(xn−1−e)→−xc_n(x_n^{-1}-e) \to -xcn​(xn−1​−e)→−x in J1J_1J1​. This is one step from a central limit theorem for partial sums to one for counting processes. Theorem 7.4 shows a limitation: convergence of both the centered supremum and the centered inverse in J1J_1J1​ forces a continuous limit.

Formalizing it. The results are proved and classical, but none of them has a machine-checked proof. The mission produces the M1M_1M1​ topology on D([0,∞),R)D([0,\infty),\mathbb R)D([0,∞),R) in Lean, the first passage time map with its basic properties, and the comparison between J1J_1J1​, M1M_1M1​ and UUU. That infrastructure is reused by every later formalization that goes through counting processes or the M1M_1M1​ topology, including the planned wave of §§3–7 corollaries in this series.

Difficulty

The first passage time map is not J1J_1J1​-continuous. On p. 82 the paper gives paths xn→xx_n \to xxn​→x in J1J_1J1​ whose inverses converge only in M1M_1M1​: a flat stretch of the limit becomes a jump of x−1x^{-1}x−1, which the inverses of the approximating paths approach through two separate jumps. Inverting the time changes λn\lambda_nλn​ of the J1J_1J1​ convergence cannot handle that split, because J1J_1J1​ matches jumps one to one. The hypothesis that xxx is strictly increasing excludes flat stretches of the limit. The technical weight lies in completed graphs and their parametric representations, which Mathlib does not have, and in the restriction to compact intervals at continuity points of the limit.

Formalization scope

  • Paths are total functions R→R\mathbb R \to \mathbb RR→R. Only [0,∞)[0,\infty)[0,∞) matters, and every statement is on Ici 0. All convergences are sequential, which is equivalent because the spaces are metrizable (Theorem 2.6). Membership of every path in DDD is part of each convergence.
  • J1J_1J1​ is the shared layer of the series: the metric (2.1) with [0,∞][0,\infty][0,∞]-valued distances, extended to [0,∞)[0,\infty)[0,∞) through restrictions to [a,b][a,b][a,b] whose endpoints are continuity points or endpoints.
  • M1M_1M1​ is not defined in the paper. The mission defines it with the convention x(0−):=0x(0-) := 0x(0−):=0 at the origin, so the completed graph on [0,b][0,b][0,b] starts with the segment from (0,0)(0,0)(0,0) to (0,x(0))(0,x(0))(0,x(0)). With the convention x(0−)=x(0)x(0-) = x(0)x(0−)=x(0), Theorem 7.1 is false. For x(s)=(s−1)+x(s) = (s-1)^+x(s)=(s−1)+ and xn=x+1/nx_n = x + 1/nxn​=x+1/n, xn−1x_n^{-1}xn−1​ jumps from 000 to 111 at t=1/nt = 1/nt=1/n while x−1(0)=1x^{-1}(0) = 1x−1(0)=1. The convention is Whitt's later M1′M_1'M1′​. Two milestones carry a hypothesis that this convention forces, and each says so: the supremum milestone requires xn(0),x(0)≥0x_n(0), x(0) \ge 0xn​(0),x(0)≥0 (as on EEE), and the M1⇒UM_1 \Rightarrow UM1​⇒U milestone requires x(0)=0x(0) = 0x(0)=0. The goal, which is stated in J1J_1J1​, does not depend on the convention.
  • x−1x^{-1}x−1 is a real infimum. Its set is nonempty because paths in EEE are unbounded above, so every statement that uses x−1x^{-1}x−1 assumes membership in EEE. The inequality x(s)>tx(s) > tx(s)>t is strict, as on the page.
  • Omitted. The measurability clause of Theorem 7.2 refers to the Borel σ-field of J1J_1J1​, which the series does not build, and it is not stated. Replacing it by measurability for the product σ-algebra would be a different statement. The second clause of the §6 sentence on D0D_0D0​ is also not stated.
  • Ruled out. A formalization in which x−1x^{-1}x−1 is applied outside EEE (giving the junk value 000), or in which J1J_1J1​ convergence omits membership in DDD (making the restriction clause vacuous), would trivialize the goal. Both are excluded.

Contributions welcome: the general theory of parametric representations (existence, and the M1M_1M1​ comparison with J1J_1J1​ and UUU), which is reusable for any M1M_1M1​ result. Alternative proofs of Theorem 7.2 that avoid M1M_1M1​ are also welcome.

Selected references

  • W. Whitt, Some Useful Functions for Functional Limit Theorems, Mathematics of Operations Research 5(1), 1980, 67–85. https://doi.org/10.1287/moor.5.1.67
  • A. V. Skorohod, Limit theorems for stochastic processes, Theory of Probability and Its Applications 1(3), 1956, 261–290. https://doi.org/10.1137/1101022
  • W. Whitt, Weak convergence of first passage time processes, Journal of Applied Probability 8(2), 1971, 417–422. https://doi.org/10.2307/3211913
  • W. Vervaat, Functional central limit theorems for processes with positive drift and their inverses, Zeitschrift für Wahrscheinlichkeitstheorie 23, 1972, 245–253. https://doi.org/10.1007/BF00532510
  • W. Whitt, Stochastic-Process Limits, Springer, 2002, §13.6. https://doi.org/10.1007/b97479
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Convex OptimizationNumerical AnalysisOperations Research+1·Captain: mikedeng1

A Coordinate Gradient Descent Method for Nonsmooth Separable Minimization 2: Under a Local Lipschitzian Error Bound, CGD with the Restricted Gauss–Seidel Rule Converges LinearlyResearch Paper

Motivation

Many problems in statistics, signal processing and machine learning minimize the sum of a smooth loss and a convex, nonsmooth, separable regularizer: smooth optimization with ℓ1\ell_1ℓ1​-regularization, bound-constrained optimization, the group Lasso and, through duality, support vector regression are special cases listed in §1 of the paper discussed below. For such problems, methods that update one coordinate, or one small block of coordinates, at a time are often the method of choice, because each update is cheap and exploits separability.

Paul Tseng and Sangwoon Yun (Math. Program. Ser. B 117 (2009) 387–423) introduced the coordinate gradient descent (CGD) method for this class: at each iteration it minimizes a quadratic model of the smooth part plus the exact nonsmooth part over a chosen block of coordinates, then takes an Armijo step. Their paper proves global convergence (Theorem 1) and, under a local error bound, linear convergence (Theorems 2 and 3). This mission is the second of a three-mission series on the paper; it targets the linear convergence theorem for the cyclic (Gauss–Seidel-type) choice of blocks.

The analysis follows Luo and Tseng's error-bound framework for smooth constrained problems (Ann. Oper. Res. 46 (1993) 157–178), which established linear rates for feasible descent methods without strong convexity. Tseng and Yun extend that framework to a nonsmooth convex term.

Setting

Let ℜn\Re^nℜn carry the Euclidean norm ∥⋅∥\|\cdot\|∥⋅∥, let N={1,…,n}\mathcal N=\{1,\dots,n\}N={1,…,n}, and for J⊆N\mathcal J\subseteq\mathcal NJ⊆N let xJx_{\mathcal J}xJ​ be the subvector of coordinates in J\mathcal JJ. The problem (1) is

min⁡x Fc(x)=f(x)+cP(x),\min_x\ F_c(x)=f(x)+cP(x),xmin​ Fc​(x)=f(x)+cP(x),

where c>0c>0c>0, P:ℜn→(−∞,∞]P:\Re^n\to(-\infty,\infty]P:ℜn→(−∞,∞] is proper, convex and lower semicontinuous, and fff is continuously differentiable on an open set containing dom⁡P\operatorname{dom}PdomP.

Given x∈dom⁡Px\in\operatorname{dom}Px∈domP, a nonempty block J\mathcal JJ and a symmetric positive definite matrix HHH, the direction (6) is

dH(x;J)=arg⁡min⁡d{∇f(x)Td+12dTHd+cP(x+d) ∣ dj=0 ∀j∉J}.d_H(x;\mathcal J)=\arg\min_d\Big\{\nabla f(x)^Td+\tfrac12d^THd+cP(x+d)\ \Big|\ d_j=0\ \forall j\notin\mathcal J\Big\}.dH​(x;J)=argdmin​{∇f(x)Td+21​dTHd+cP(x+d) ​ dj​=0 ∀j∈/J}.

The CGD method starts at x0∈dom⁡Px^0\in\operatorname{dom}Px0∈domP, chooses at each iteration kkk a block Jk\mathcal J^kJk and a matrix HkH^kHk, computes dk=dHk(xk;Jk)d^k=d_{H^k}(x^k;\mathcal J^k)dk=dHk​(xk;Jk), and sets xk+1=xk+αkdkx^{k+1}=x^k+\alpha^kd^kxk+1=xk+αkdk. The Armijo rule takes αk\alpha^kαk as the largest element of {αinitkβj}j≥0\{\alpha^k_{\rm init}\beta^j\}_{j\ge0}{αinitk​βj}j≥0​ with

Fc(xk+αkdk)≤Fc(xk)+αkσΔk,Δk=∇f(xk)Tdk+γ dkTHkdk+cP(xk+dk)−cP(xk),F_c(x^k+\alpha^kd^k)\le F_c(x^k)+\alpha^k\sigma\Delta^k,\qquad \Delta^k=\nabla f(x^k)^Td^k+\gamma\,d^{kT}H^kd^k+cP(x^k+d^k)-cP(x^k),Fc​(xk+αkdk)≤Fc​(xk)+αkσΔk,Δk=∇f(xk)Tdk+γdkTHkdk+cP(xk+dk)−cP(xk),

with 0<β,σ<10<\beta,\sigma<10<β,σ<1 and 0≤γ<10\le\gamma<10≤γ<1. The restricted Gauss–Seidel rule (12) asks for indices 0=t0<t1<⋯0=t_0<t_1<\cdots0=t0​<t1​<⋯ (the set T\mathcal TT) such that the blocks used during each cycle ti≤k<ti+1t_i\le k<t_{i+1}ti​≤k<ti+1​ are pairwise disjoint and cover N\mathcal NN. PPP is block-separable with respect to J\mathcal JJ if P(x)=PJ(xJ)+PJC(xJC)P(x)=P_{\mathcal J}(x_{\mathcal J})+P_{\mathcal J^C}(x_{\mathcal J^C})P(x)=PJ​(xJ​)+PJC​(xJC​).

The analysis uses three assumptions: ∇f\nabla f∇f is LLL-Lipschitz on dom⁡P\operatorname{dom}PdomP (22); Assumption 1, λˉI⪰Hk⪰λ‾I\bar\lambda I\succeq H^k\succeq\underline\lambda IλˉI⪰Hk⪰λ​I with 0<λ‾≤λˉ0<\underline\lambda\le\bar\lambda0<λ​≤λˉ; and Assumption 2. Writing Xˉ\bar XXˉ for the set of stationary points of FcF_cFc​ and dI(x)d_I(x)dI​(x) for the full direction with H=IH=IH=I, Assumption 2 says (a) Xˉ≠∅\bar X\ne\emptysetXˉ=∅ and the local Lipschitzian error bound dist⁡(x,Xˉ)≤τ∥dI(x)∥\operatorname{dist}(x,\bar X)\le\tau\|d_I(x)\|dist(x,Xˉ)≤τ∥dI​(x)∥ holds on every level set {Fc≤ζ}\{F_c\le\zeta\}{Fc​≤ζ} wherever ∥dI(x)∥≤ϵ\|d_I(x)\|\le\epsilon∥dI​(x)∥≤ϵ; (b) stationary points with different objective values are at least a fixed distance δ>0\delta>0δ>0 apart.

Formalization targets

Goal: Theorem 2(b)

Under (22), Assumptions 1 and 2, the restricted Gauss–Seidel rule, block-separability of PPP with respect to every Jk\mathcal J^kJk, and Armijo steps with sup⁡kαinitk≤1\sup_k\alpha^k_{\rm init}\le1supk​αinitk​≤1 and inf⁡kαinitk>0\inf_k\alpha^k_{\rm init}>0infk​αinitk​>0:

{Fc(xk)}↓−∞or({Fc(xk)}T Q-linear and {xk}T R-linear).\{F_c(x^k)\}\downarrow-\infty\quad\text{or}\quad\big(\{F_c(x^k)\}_{\mathcal T}\ \text{Q-linear}\ \text{and}\ \{x^k\}_{\mathcal T}\ \text{R-linear}\big).{Fc​(xk)}↓−∞or({Fc​(xk)}T​ Q-linear and {xk}T​ R-linear).

No rate constant is fixed: the goal asserts the shape of the convergence, so it is not invalidated by sharper constants.

Milestones

Lemma 4 (Hölder dependence of the subproblem's solution on its linear term), Lemma 5(a) (a per-block variational inequality), Lemma 5(b) (an explicit stepsize at which the Armijo test passes), Theorem 1(f) (Armijo stepsizes bounded away from zero, Δk→0\Delta^k\to0Δk→0, dk→0d^k\to0dk→0), and Theorem 2(a) (the residual ∥dI(xk)∥\|d_I(x^k)\|∥dI​(xk)∥ at the start of a cycle is bounded by the step lengths of the cycle).

Significance

Theorem 2(b) gives a linear rate for a block coordinate method on a nonsmooth, possibly nonconvex composite problem without strong convexity: the rate follows from the error bound, which holds for a large class of problems studied in §6 of the paper (the third mission of this series).

The theorem is proved in the paper; none of it has been machine-checked, as far as a search of the Prove2Me library shows. Formalizing it requires a reusable treatment of extended-valued convex functions through their effective domains, of the coordinate-restricted proximal subproblem, and of the Armijo rule for composite objectives. The milestones Lemma 4 and Lemma 5 are self-contained facts about this subproblem and are reusable for other proximal coordinate methods.

Difficulty

The classical route to a linear rate, as in Luo and Tseng's smooth analysis, derives Fc(xk+1)−υˉ≤τ′∥xk+1−xk∥2F_c(x^{k+1})-\bar\upsilon\le\tau'\|x^{k+1}-x^k\|^2Fc​(xk+1)−υˉ≤τ′∥xk+1−xk∥2 from the error bound, where υˉ\bar\upsilonυˉ is the limit value. With a nonsmooth PPP this inequality is not available: the authors say so on p. 405, and work with −Δk-\Delta^k−Δk in place of the quadratic term. A second obstacle is that the error bound controls the full residual dI(xk)d_I(x^k)dI​(xk), while each iteration only computes a block direction at a different point; relating the two over a cycle needs the disjointness of the blocks in the restricted rule and block-separability of PPP. Neither the global analysis nor the error bound alone gives the rate.

Formalization scope

ℜn\Re^nℜn is EuclideanSpace ℝ (Fin n), with 0-based coordinates. The extended-valued PPP is encoded as a pair: its effective domain D=dom⁡PD=\operatorname{dom}PD=domP and its finite values on DDD, with "proper convex lsc" given by the published definition ProxNewton.Inexact.IsProperClosedConvex; FcF_cFc​ is never evaluated off DDD, and every statement carries membership in DDD explicitly. The direction dH(x;J)d_H(x;\mathcal J)dH​(x;J) is the unique minimizer of (6) when x∈Dx\in Dx∈D and H≻0H\succ0H≻0 (chosen by Classical.epsilon), and runs of the method carry the minimizer property itself. The Armijo rule takes the first admissible exponent jjj. T\mathcal TT is a strictly increasing map ttt with t0=0t_0=0t0​=0. Stationarity is Fc′(x;d)≥0F_c'(x;d)\ge0Fc′​(x;d)≥0 for all ddd, in liminf form. In Assumption 2, dist⁡\operatorname{dist}dist is the infimum distance and "for any ζ≥min⁡Fc\zeta\ge\min F_cζ≥minFc​" is "for every real ζ\zetaζ" (equivalent, since the condition is empty below inf⁡Fc\inf F_cinfFc​). Q-linear convergence includes convergence of the sequence; R-linear convergence is ∥xti−xˉ∥≤Cqi\|x^{t_i}-\bar x\|\le Cq^i∥xti​−xˉ∥≤Cqi with q<1q<1q<1. The rates in the goal are along T\mathcal TT, as the paper states.

Explicit choices relative to the printed text:

  • Theorem 2(a) is corrected. As printed, ∥dI(xk)∥≤sup⁡jαj C rk\|d_I(x^k)\|\le\sup_j\alpha^j\,C\,r^k∥dI​(xk)∥≤supj​αjCrk fails for small constant stepsizes and fails without block-separability (counterexamples in the item's statement). The milestone states ∥dI(xk)∥≤max⁡{1,sup⁡jαj} C rk\|d_I(x^k)\|\le\max\{1,\sup_j\alpha^j\}\,C\,r^k∥dI​(xk)∥≤max{1,supj​αj}Crk under block-separability of PPP with respect to every Jk\mathcal J^kJk (both are what the paper's proof gives and what Theorem 2(b) supplies), with the iterates in dom⁡P\operatorname{dom}PdomP, and with CCC quantified before the problem data, so it depends only on n,L,λ‾,λˉn,L,\underline\lambda,\bar\lambdan,L,λ​,λˉ.
  • Lemma 5(b)'s range 0≤α≤min⁡{1,2λ‾(1−σ+σγ)/L}0\le\alpha\le\min\{1,2\underline\lambda(1-\sigma+\sigma\gamma)/L\}0≤α≤min{1,2λ​(1−σ+σγ)/L} is stated as 0≤α≤10\le\alpha\le10≤α≤1 and αL≤2λ‾(1−σ+σγ)\alpha L\le2\underline\lambda(1-\sigma+\sigma\gamma)αL≤2λ​(1−σ+σγ), so that L=0L=0L=0 gives [0,1][0,1][0,1] as on paper rather than {0}\{0\}{0}.
  • Lemma 5(a) holds for every decomposition of PPP in (20), and xˉ\bar xxˉ ranges over dom⁡PJ\operatorname{dom}P_{\mathcal J}domPJ​ (outside it the left side is −∞-\infty−∞).
  • "lim⁡Fc(xk)>−∞\lim F_c(x^k)>-\inftylimFc​(xk)>−∞" is "the values Fc(xk)F_c(x^k)Fc​(xk) are bounded below"; "{Fc(xk)}↓−∞\{F_c(x^k)\}\downarrow-\infty{Fc​(xk)}↓−∞" is "nonincreasing and tending to −∞-\infty−∞"; suprema and infima of stepsizes are explicit bounds.

A statement that replaces Assumption 2 by strong convexity, claims a rate along the whole sequence rather than along T\mathcal TT, or asserts the Q-linear contraction without convergence to a limit is not this theorem and is out of scope.

Lemma 1, the claim after (10), Lemma 3 and Theorem 1(a), which the proof also uses, are milestones of the first mission of this series and are not restated here. Theorem 3 (the same conclusion along the whole sequence for the Gauss–Southwell-q rule) is not included: its proof is omitted in the paper. Contributions welcome: proofs of the milestones, and general facts about the coordinate-restricted proximal subproblem (existence and uniqueness of dH(x;J)d_H(x;\mathcal J)dH​(x;J), optimality conditions) that the milestones rely on.

Selected references

  • P. Tseng and S. Yun, A coordinate gradient descent method for nonsmooth separable minimization, Mathematical Programming Ser. B 117 (2009) 387–423. https://doi.org/10.1007/s10107-007-0170-0
  • Z.-Q. Luo and P. Tseng, Error bounds and convergence analysis of feasible descent methods: a general approach, Annals of Operations Research 46 (1993) 157–178. https://doi.org/10.1007/BF02096261
  • J. M. Ortega and W. C. Rheinboldt, Iterative Solution of Nonlinear Equations in Several Variables, Academic Press, 1970, Chap. 9 (Q- and R-linear convergence). https://doi.org/10.1137/1.9780898719468
  • R. T. Rockafellar and R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Consistent Nonparametric Regression II: Nearest-Neighbor Weights with Vanishing Coefficients Are Consistent for Every Distribution of X (Theorem 2)Research Paper

Motivation

Nonparametric regression estimates the regression function x↦E(Y∣X=x)x \mapsto E(Y \mid X = x)x↦E(Y∣X=x) from i.i.d. observations (X1,Y1),…,(Xn,Yn)(X_1, Y_1), \dots, (X_n, Y_n)(X1​,Y1​),…,(Xn​,Yn​) without assuming a parametric form. The simplest such estimates are local averages: to predict at a point XXX, average the responses YiY_iYi​ of the sample points closest to XXX. Nearest neighbor rules of this kind go back to Fix and Hodges (1951) for classification and are still a standard baseline in statistics and machine learning.

Before 1977, consistency results for such estimates assumed regularity of the distribution of XXX: a density, continuity of the regression function, or bounded support. C. J. Stone's paper Consistent nonparametric regression (Ann. Statist. 5 (1977) 595–645) proved that suitable nearest neighbor estimates are consistent in LrL^rLr for every joint distribution of (X,Y)(X, Y)(X,Y) with E∣Y∣r<∞E|Y|^r < \inftyE∣Y∣r<∞. This property, now called universal consistency, is the subject of the first chapters of Györfi, Kohler, Krzyżak and Walk, A Distribution-Free Theory of Nonparametric Regression (Springer, 2002), where Stone's theorem is the organising result.

This mission formalizes Theorem 2 of Stone's paper, the universal consistency of nearest neighbor weights. Mission I of the series formalizes the general criterion (Theorem 1) that the proof applies; mission III treats conditional quantiles.

Setting

Let X,X1,X2,…X, X_1, X_2, \dotsX,X1​,X2​,… be i.i.d. random vectors in Rd\mathbb R^dRd with an arbitrary law μ\muμ. A weight function WnW_nWn​ assigns to the query point XXX and the sample numbers Wni(X)=Wni(X,X1,…,Xn)W_{ni}(X) = W_{ni}(X, X_1, \dots, X_n)Wni​(X)=Wni​(X,X1​,…,Xn​), 1≤i≤n1 \le i \le n1≤i≤n. It is a probability weight function if Wni≥0W_{ni} \ge 0Wni​≥0 and ∑iWni(X)=1\sum_i W_{ni}(X) = 1∑i​Wni​(X)=1. Given i.i.d. pairs (X,Y),(X1,Y1),…(X, Y), (X_1, Y_1), \dots(X,Y),(X1​,Y1​),… with YYY real, the estimate of E(Y∣X)E(Y \mid X)E(Y∣X) is

E^n(Y∣X)=∑i=1nWni(X) Yi.\hat E_n(Y \mid X) = \sum_{i=1}^n W_{ni}(X)\, Y_i .E^n​(Y∣X)=i=1∑n​Wni​(X)Yi​.

The sequence {Wn}\{W_n\}{Wn​} is consistent if, whenever the pairs are i.i.d. with the given law of XXX, r≥1r \ge 1r≥1 and E∣Y∣r<∞E|Y|^r < \inftyE∣Y∣r<∞, one has E∣E^n(Y∣X)−E(Y∣X)∣r→0E|\hat E_n(Y\mid X) - E(Y\mid X)|^r \to 0E∣E^n​(Y∣X)−E(Y∣X)∣r→0.

Scales and metrics. A scale is a nonnegative function snj=snj(X,X1,…,Xn)s_{nj} = s_{nj}(X, X_1, \dots, X_n)snj​=snj​(X,X1​,…,Xn​), 1≤j≤d1 \le j \le d1≤j≤d, and its pseudometric is

ρn(u,v)=(∑j: snj>0(uj−vjsnj)2)1/2.\rho_n(u, v) = \Big(\sum_{j:\, s_{nj} > 0} \Big(\frac{u_j - v_j}{s_{nj}}\Big)^2\Big)^{1/2}.ρn​(u,v)=(j:snj​>0∑​(snj​uj​−vj​​)2)1/2.

The choice snj≡1s_{nj} \equiv 1snj​≡1 gives the Euclidean metric; the sample standard deviations of the coordinates give a unit-free one. The sequence {sn}\{s_n\}{sn​} is regular (p. 599) with constants 0<a≤b0 < a \le b0<a≤b if P(snj>0)→1P(s_{nj} > 0) \to 1P(snj​>0)→1 for every coordinate of XXX with a nondegenerate law, snj/snls_{nj}/s_{nl}snj​/snl​ is bounded in probability for any two such coordinates, and condition (7) holds: interchanging XXX and XiX_iXi​ changes snjs_{nj}snj​ by a factor in [a,b][a, b][a,b] whenever the jjjth coordinates of X1,…,XnX_1, \dots, X_nX1​,…,Xn​ do not all coincide.

Nearest neighbor weights. Let cn1≥⋯≥cnn≥0c_{n1} \ge \dots \ge c_{nn} \ge 0cn1​≥⋯≥cnn​≥0 with ∑icni=1\sum_i c_{ni} = 1∑i​cni​=1 and cni=0c_{ni} = 0cni​=0 for i>ni > ni>n. The weight of XiX_iXi​ is

Wni(X)=cnν+⋯+cn,ν+λ−1λ,W_{ni}(X) = \frac{c_{n\nu} + \dots + c_{n,\nu+\lambda-1}}{\lambda},Wni​(X)=λcnν​+⋯+cn,ν+λ−1​​,

where ν−1\nu - 1ν−1 is the number of other sample points strictly ρn\rho_nρn​-closer to XXX than XiX_iXi​ and λ−1\lambda - 1λ−1 the number at the same distance: the kkkth closest point receives cnkc_{nk}cnk​, and tied points share the average of the coefficients of their ranks. The uniform kkk-NN rule is cni=1/kc_{ni} = 1/kcni​=1/k for i≤ki \le ki≤k.

Formalization targets

Goal: Theorem 2 (p. 600)

For every law μ\muμ of XXX and every regular sequence of scales,

lim⁡n∑i>αncni=0  (∀α>0)andlim⁡ncn1=0⟹{Wn} is consistent.\lim_{n} \sum_{i > \alpha n} c_{ni} = 0 \ \ (\forall \alpha > 0) \quad\text{and}\quad \lim_n c_{n1} = 0 \quad\Longrightarrow\quad \{W_n\} \text{ is consistent.}nlim​i>αn∑​cni​=0  (∀α>0)andnlim​cn1​=0⟹{Wn​} is consistent.

Uniform, triangular and quadratic knk_nkn​-NN weights with kn→∞k_n \to \inftykn​→∞, kn/n→0k_n / n \to 0kn​/n→0 satisfy both conditions (Corollary 3).

Milestones

  1. Corollary 1 (sufficiency), p. 598. Probability weights with E∑iWni(X)f(Xi)≤C Ef(X)E\sum_i W_{ni}(X) f(X_i) \le C\,Ef(X)E∑i​Wni​(X)f(Xi​)≤CEf(X) for some C≥1C \ge 1C≥1 and all nonnegative Borel fff, with ∑iWni(X)I{∥Xi−X∥>a}→0\sum_i W_{ni}(X) I_{\{\|X_i - X\| > a\}} \to 0∑i​Wni​(X)I{∥Xi​−X∥>a}​→0 and max⁡iWni(X)→0\max_i W_{ni}(X) \to 0maxi​Wni​(X)→0 in probability, are consistent.
  2. Proposition 9, p. 611. For every δ>0\delta > 0δ>0, lim⁡α↓0lim sup⁡nP(max⁡i∈In,αn(X)∥Xi−X∥>δ)=0\lim_{\alpha\downarrow 0}\limsup_n P(\max_{i \in I_{n,\alpha n}(X)} \|X_i - X\| > \delta) = 0limα↓0​limsupn​P(maxi∈In,αn​(X)​∥Xi​−X∥>δ)=0, where In,t(X)I_{n,t}(X)In,t​(X) are the indices of the ⌊t⌋\lfloor t \rfloor⌊t⌋ nearest neighbors (with ties).
  3. Proposition 10, p. 613. For 0<a≤bj≤b0 < a \le b_j \le b0<a≤bj​≤b, two vectors 0<∥u∥≤∥v∥0 < \|u\| \le \|v\|0<∥u∥≤∥v∥ in a set V∈V(d,a/b)V \in \mathcal V(d, a/b)V∈V(d,a/b) satisfy ∥v~∥>∥v~−u~∥\|\tilde v\| > \|\tilde v - \tilde u\|∥v~∥>∥v~−u~∥ after rescaling u~j=bjuj\tilde u_j = b_j u_ju~j​=bj​uj​, v~j=bjvj\tilde v_j = b_j v_jv~j​=bj​vj​. Here V(d,c)\mathcal V(d, c)V(d,c) is the family of sets in which any two nonzero vectors satisfy u⋅v>(1−c2/2)∥u∥∥v∥u\cdot v > (1 - c^2/2)\|u\|\|v\|u⋅v>(1−c2/2)∥u∥∥v∥, and β(d,c)\beta(d, c)β(d,c) is the least number of members of V(d,c)\mathcal V(d,c)V(d,c) covering Rd\mathbb R^dRd.
  4. Proposition 12, p. 613. For fixed points, the swapped weights Uni(X)=Wni(Xi,X1,…,X,…,Xn)U_{ni}(X) = W_{ni}(X_i, X_1, \dots, X, \dots, X_n)Uni​(X)=Wni​(Xi​,X1​,…,X,…,Xn​) satisfy ∑iUni(X)≤β(d,a/b)\sum_i U_{ni}(X) \le \beta(d, a/b)∑i​Uni​(X)≤β(d,a/b).
  5. Proposition 11, p. 613. E∑iWni(X)f(Xi)≤β(d,a/b) Ef(X)E \sum_i W_{ni}(X) f(X_i) \le \beta(d, a/b)\, Ef(X)E∑i​Wni​(X)f(Xi​)≤β(d,a/b)Ef(X) for nonnegative Borel fff with Ef(X)<∞Ef(X) < \inftyEf(X)<∞.

Significance

Theorem 2 established that a local averaging estimate can be consistent with no assumption on the distribution of XXX beyond the moment condition on YYY. The same argument, through Theorem 1, became the standard template for proving universal consistency of kernel, partitioning and nearest neighbor estimates, and of the classification rules derived from them (Devroye, Györfi and Lugosi, A Probabilistic Theory of Pattern Recognition, 1996). The constant β(d,a/b)\beta(d, a/b)β(d,a/b) of Proposition 11 is an early instance of the cone-covering bound on how many points can have a given point among their nearest neighbors, a lemma that reappears throughout nearest neighbor theory.

The result is proved (1977), and textbook proofs exist. Mathlib contains no formalization of Theorem 2, of Stone's criterion, or of the cone-covering lemma. A formal development would supply reusable infrastructure: nearest neighbor weights with averaged ties, the exchangeability argument behind Proposition 11, and LrL^rLr consistency of weighted averages for i.i.d. data encoded through kernels.

Difficulty

The obvious argument estimates E^n(Y∣X)\hat E_n(Y\mid X)E^n​(Y∣X) by a continuity argument around XXX, which needs a density or continuity of E(Y∣X)E(Y\mid X)E(Y∣X) and is unavailable here. The difficulty is condition (1) of Stone's criterion: a single sample point may be a nearest neighbor of many query points, so E∑iWni(X)f(Xi)E\sum_i W_{ni}(X) f(X_i)E∑i​Wni​(X)f(Xi​) is not obviously comparable to Ef(X)Ef(X)Ef(X) for arbitrary fff and arbitrary μ\muμ (atoms, singular parts, unbounded support). The bound must hold uniformly in nnn and in the distribution, with a data-dependent metric whose scale changes when XXX and XiX_iXi​ are interchanged. Ties in ρn\rho_nρn​, which have positive probability when μ\muμ has atoms, must be handled by the averaged weights (8), not by an index tie-break.

Formalization scope

Points live in EuclideanSpace ℝ (Fin d). The i.i.d. sequence is the coordinate process of Measure.infinitePi, coordinate 0 being XXX; sample indices are 0-based, coefficients cn,mc_{n,m}cn,m​ keep the paper's 1-based index. "Whenever the pairs are i.i.d." is encoded by quantifying over every Markov kernel κ\kappaκ (the conditional law of YYY given XXX), with pairs distributed as (μ⊗κ)⊗N(\mu \otimes \kappa)^{\otimes\mathbb N}(μ⊗κ)⊗N and E(Y∣X=x)=∫y κ(x,dy)E(Y\mid X=x) = \int y\,\kappa(x, dy)E(Y∣X=x)=∫yκ(x,dy). Expectations of nonnegative quantities are lower Lebesgue integrals in [0,∞][0,\infty][0,∞]; convergence in probability is TendstoInMeasure; limits of probabilities are taken in [0,∞][0,\infty][0,∞].

Standing assumptions and additions, each disclosed in the item statements:

  • the scales are regular (the standing assumption of §3, p. 599) and Borel measurable (added; the paper treats them as random variables);
  • condition (7) is read for all points, as Proposition 12's proof uses it, and "do not coincide" means "are not all equal";
  • "nondegenerate" means the coordinate's law is not a point mass; snj/snls_{nj}/s_{nl}snj​/snl​ is real division (000 where snl=0s_{nl} = 0snl​=0, an event of vanishing probability);
  • Corollary 1's weights are assumed jointly Borel;
  • Proposition 9's distance aaa is renamed δ\deltaδ, and the maximum over an empty index set is read as "no index";
  • β(d,c)\beta(d, c)β(d,c) is an infimum over N\mathbb NN; that a finite cover exists is part of the work, not an assumption.

No statement corrects the print.

The goal is stated as LrL^rLr consistency over all kernels and all r≥1r \ge 1r≥1, for an unrestricted law μ\muμ: it is not stated through Corollary 1's three conditions nor through β\betaβ, and no density, moment or support hypothesis on XXX is present, so a proof cannot reduce to a special case.

A complete development needs: exchangeability of finite i.i.d. samples under the product measure, the finite cone cover of Rd\mathbb R^dRd, the strong law of large numbers (Proposition 9's proof), and Stone's criterion (mission I). Contributions proving any milestone, the cone-cover existence lemma, or the transfer of exchangeability through infinitePi are welcome.

Selected references

  • C. J. Stone, Consistent nonparametric regression, Ann. Statist. 5(4) (1977) 595–645. https://doi.org/10.1214/aos/1176343886
  • L. Györfi, M. Kohler, A. Krzyżak, H. Walk, A Distribution-Free Theory of Nonparametric Regression, Springer, 2002. https://doi.org/10.1007/b97848
  • L. Devroye, L. Györfi, G. Lugosi, A Probabilistic Theory of Pattern Recognition, Springer, 1996. https://doi.org/10.1007/978-1-4612-0711-5
  • E. Fix, J. L. Hodges, Discriminatory analysis. Nonparametric discrimination: consistency properties, USAF School of Aviation Medicine, Report 4, 1951; reprinted in Int. Stat. Rev. 57(3) (1989) 238–247. https://doi.org/10.2307/1403797
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Consistent Nonparametric Regression III: Consistent Probability Weights Give Consistent Estimators of Conditional Quantiles (Theorem 3)Research Paper

Motivation

Many prediction tasks ask not for the mean of a response YYY given covariates XXX but for a quantile of its conditional distribution: a median that is robust to outliers, a high quantile that sets a safety stock or a value at risk, or a pair of quantiles that forms a prediction interval. Conditional quantiles are also the Bayes rules for piecewise linear loss, which makes them the decision-theoretic answer to asymmetric prediction costs.

C. J. Stone's 1977 paper Consistent nonparametric regression (DOI 10.1214/aos/1176343886) introduced a single framework for local averaging estimators (nearest-neighbor, kernel and related rules) built from weight functions, and proved that their consistency can be decided from simple conditions on the weights, for every distribution of (X,Y)(X,Y)(X,Y). Section 7 of the paper extends the framework from conditional means to conditional quantiles: the same weights that estimate E(Y∣X)E(Y\mid X)E(Y∣X) define a weighted empirical distribution of YYY near XXX, whose quantiles estimate the conditional quantiles. Theorem 3 says that consistency for the mean already gives one-sided consistency for the quantiles. This mission formalizes Theorem 3 and the results its proof rests on.

Setting

Let X,X1,X2,…X, X_1, X_2, \dotsX,X1​,X2​,… be independent Rd\mathbb R^dRd-valued random variables with common law μ\muμ, and let Y,Y1,Y2,…Y, Y_1, Y_2,\dotsY,Y1​,Y2​,… be real responses such that the pairs (X,Y),(X1,Y1),(X2,Y2),…(X,Y), (X_1,Y_1), (X_2,Y_2),\dots(X,Y),(X1​,Y1​),(X2​,Y2​),… are i.i.d. The conditional law of YYY given X=xX=xX=x is a probability measure κ(x,⋅)\kappa(x,\cdot)κ(x,⋅) on R\mathbb RR.

A weight function WnW_nWn​ assigns to a point xxx and a sample x1,…,xnx_1,\dots,x_nx1​,…,xn​ real weights Wni(x)=Wni(x;x1,…,xn)W_{ni}(x)=W_{ni}(x;x_1,\dots,x_n)Wni​(x)=Wni​(x;x1​,…,xn​), 1≤i≤n1\le i\le n1≤i≤n. A sequence {Wn}\{W_n\}{Wn​} is a sequence of probability weights if for every n≥1n\ge1n≥1 the weights are nonnegative and sum to 111. The weights define the regression estimate E^n(Y∣X)=∑iWni(X)Yi\hat E_n(Y\mid X)=\sum_i W_{ni}(X)Y_iE^n​(Y∣X)=∑i​Wni​(X)Yi​. The sequence is consistent if, whenever r≥1r\ge1r≥1 and E∣Y∣r<∞E|Y|^r<\inftyE∣Y∣r<∞,

E ∣E^n(Y∣X)−E(Y∣X)∣r→0,E\,\big|\hat E_n(Y\mid X)-E(Y\mid X)\big|^r\to0,E​E^n​(Y∣X)−E(Y∣X)​r→0,

for every response YYY with i.i.d. pairs as above. Consistency is a property of the weights and the law of XXX alone.

The conditional distribution function is FY(y∣X)=P(Y≤y∣X)F^Y(y\mid X)=P(Y\le y\mid X)FY(y∣X)=P(Y≤y∣X). For 0<p<10<p<10<p<1 the lower and upper pppth conditional quantiles are

LY(p∣X)=inf⁡{y:FY(y∣X)≥p},UY(p∣X)=sup⁡{y:FY(y∣X)≤p}.L^Y(p\mid X)=\inf\{y:F^Y(y\mid X)\ge p\},\qquad U^Y(p\mid X)=\sup\{y:F^Y(y\mid X)\le p\}.LY(p∣X)=inf{y:FY(y∣X)≥p},UY(p∣X)=sup{y:FY(y∣X)≤p}.

They coincide unless the conditional distribution function is flat at level ppp. The weights estimate the conditional distribution function by F^nY(y∣X)=∑iWni(X)I{Yi≤y}\hat F_n^Y(y\mid X)=\sum_i W_{ni}(X)I_{\{Y_i\le y\}}F^nY​(y∣X)=∑i​Wni​(X)I{Yi​≤y}​, and the quantiles by

L^nY(p∣X)=inf⁡{y:F^nY(y∣X)≥p},U^nY(p∣X)=sup⁡{y:F^nY(y∣X)≤p}.\hat L_n^Y(p\mid X)=\inf\{y:\hat F_n^Y(y\mid X)\ge p\},\qquad \hat U_n^Y(p\mid X)=\sup\{y:\hat F_n^Y(y\mid X)\le p\}.L^nY​(p∣X)=inf{y:F^nY​(y∣X)≥p},U^nY​(p∣X)=sup{y:F^nY​(y∣X)≤p}.

Write x−=−(x∧0)x^-=-(x\wedge0)x−=−(x∧0) and x+=x∨0x^+=x\vee0x+=x∨0.

Formalization targets

Goal: Theorem 3 (p. 604)

For a consistent sequence of probability weights and 0<p<10<p<10<p<1,

(L^nY(p∣X)−LY(p∣X))−→0and(U^nY(p∣X)−UY(p∣X))+→0in probability,(\hat L_n^Y(p\mid X)-L^Y(p\mid X))^-\to0\quad\text{and}\quad(\hat U_n^Y(p\mid X)-U^Y(p\mid X))^+\to0\quad\text{in probability},(L^nY​(p∣X)−LY(p∣X))−→0and(U^nY​(p∣X)−UY(p∣X))+→0in probability,

and if r≥1r\ge1r≥1 and E∣Y∣r<∞E|Y|^r<\inftyE∣Y∣r<∞, both convergences hold in LrL^rLr. The theorem is one-sided on purpose: when the conditional quantile is not unique, L^n\hat L_nL^n​ and U^n\hat U_nU^n​ may oscillate inside [L,U][L,U][L,U].

Milestones

  1. Corollary 1, necessity (p. 598). Consistent probability weights satisfy condition (1), E∑iWni(X)f(Xi)≤C Ef(X)E\sum_i W_{ni}(X)f(X_i)\le C\,Ef(X)E∑i​Wni​(X)f(Xi​)≤CEf(X) for some C≥1C\ge1C≥1; condition (3), ∑iWni(X)I{∥Xi−X∥>a}→0\sum_i W_{ni}(X)I_{\{\|X_i-X\|>a\}}\to0∑i​Wni​(X)I{∥Xi​−X∥>a}​→0 in probability; and condition (5), max⁡iWni(X)→0\max_i W_{ni}(X)\to0maxi​Wni​(X)→0 in probability.
  2. Proposition 4 (p. 609). Under (1)–(3), for every Borel fff and ε>0\varepsilon>0ε>0, ∑i∣Wni(X)∣I{∣f(Xi)−f(X)∣>ε}→0\sum_i|W_{ni}(X)|I_{\{|f(X_i)-f(X)|>\varepsilon\}}\to0∑i​∣Wni​(X)∣I{∣f(Xi​)−f(X)∣>ε}​→0 in probability.
  3. Proposition 13 (p. 616). P(L^nY(p∣X)≥LY(p∣X)−ε)→1P(\hat L_n^Y(p\mid X)\ge L^Y(p\mid X)-\varepsilon)\to1P(L^nY​(p∣X)≥LY(p∣X)−ε)→1 and P(U^nY(p∣X)≤UY(p∣X)+ε)→1P(\hat U_n^Y(p\mid X)\le U^Y(p\mid X)+\varepsilon)\to1P(U^nY​(p∣X)≤UY(p∣X)+ε)→1 for every ε>0\varepsilon>0ε>0.
  4. Proposition 14 (p. 616). E∣LY(p∣X)∣r≤E∣Y∣r/(p∧(1−p))E|L^Y(p\mid X)|^r\le E|Y|^r/(p\wedge(1-p))E∣LY(p∣X)∣r≤E∣Y∣r/(p∧(1−p)), and the same for UYU^YUY.
  5. Proposition 15 (p. 617). For a probability weight function satisfying (1), E∣L^nY∣rI{∣L^nY∣≥M}≤Cp∧(1−p)E∣Y∣rI{∣Y∣≥M}E|\hat L_n^Y|^rI_{\{|\hat L_n^Y|\ge M\}}\le \frac{C}{p\wedge(1-p)}E|Y|^rI_{\{|Y|\ge M\}}E∣L^nY​∣rI{∣L^nY​∣≥M}​≤p∧(1−p)C​E∣Y∣rI{∣Y∣≥M}​, and the same for U^nY\hat U_n^YU^nY​.

Significance

Theorem 3 transfers every consistency result for conditional means to conditional quantiles at no extra cost. In particular, the nearest-neighbor weights of Stone's Theorem 2, which are consistent for every distribution of XXX, give universally consistent one-sided estimates of conditional quantiles, and when the conditional pppth quantile is unique, the midpoint estimate (L^n+U^n)/2(\hat L_n+\hat U_n)/2(L^n​+U^n​)/2 is consistent (Corollary 5 of the paper). The theorem is also the input for the consistency in Bayes risk of approximate Bayes rules under piecewise linear loss (Theorem 4, Model 2), which connects nonparametric regression to data-driven decision making such as the newsvendor problem with covariates.

The result has been proved since 1977; it has no machine-checked proof that this mission is aware of. A formalization produces a reusable layer for distribution-free statistics in Lean: weighted empirical distributions, conditional quantiles defined from a Markov kernel, convergence in probability and in LrL^rLr of statistics of an i.i.d. sequence, and the moment bounds of Propositions 14 and 15, which hold for every weight function and do not depend on the asymptotics.

Difficulty

The obvious argument fails because the conditional distribution function at XXX is never estimated uniformly. Consistency controls the weighted average ∑iWni(X)g(Yi)\sum_iW_{ni}(X)g(Y_i)∑i​Wni​(X)g(Yi​) only for responses that are a fixed function of the pair; the event {L^n<L(X)−ε}\{\hat L_n<L(X)-\varepsilon\}{L^n​<L(X)−ε} involves the random threshold L(X)L(X)L(X), which varies with the target point while the sample responses YiY_iYi​ are drawn at the sample points XiX_iXi​. Connecting the two requires a statement about the weights alone, Proposition 4, that holds for an arbitrary Borel function with no continuity or integrability; the conditional quantile function is in general neither continuous nor integrable.

A second difficulty is that convergence in probability does not give convergence in LrL^rLr without uniform integrability, and the estimated quantiles are not averages of the YiY_iYi​. The bound in Proposition 15 must hold for each nnn separately, with a constant independent of nnn, for an estimator defined as an infimum.

Finally, the two-sided statement L^n→L\hat L_n\to LL^n​→L need not hold when the conditional distribution function has a flat stretch at level ppp, which is why the paper asks for a unique conditional quantile in Corollary 5; a solver should not aim for it.

Formalization scope

The i.i.d. sequences are the coordinate processes of infinite product measures, Measure.infinitePi, with coordinate 000 the point XXX (or the pair (X,Y)(X,Y)(X,Y)) and coordinate i+1i+1i+1 the (i+1)(i+1)(i+1)st sample; sample indices are 0-based. The response is given by its conditional law, a Markov kernel κ\kappaκ from Rd\mathbb R^dRd to R\mathbb RR, and the joint law of a pair is μ⊗κ\mu\otimes\kappaμ⊗κ. "Whenever the pairs are i.i.d." in the definition of consistency is a quantifier over all Markov kernels; every joint law with XXX-marginal μ\muμ arises this way. This also provides the independent standard normal variables that the paper assumes on its probability space.

Committed conventions:

  • Measurability (added). Every weight function WnW_nWn​ is assumed jointly Borel in (x,x1,…,xn)(x,x_1,\dots,x_n)(x,x1​,…,xn​). The paper treats Wni(X)W_{ni}(X)Wni​(X) as random variables without saying so.
  • Expectations of nonnegative quantities (E∣Y∣rE|Y|^rE∣Y∣r, the LrL^rLr errors, the moment bounds) are [0,∞][0,\infty][0,∞]-valued lower integrals, so an infinite expectation is never read as 000.
  • Convergence in probability is Mathlib's TendstoInMeasure.
  • Quantiles are real sInf/sSup. For a Markov kernel, 0<p<10<p<10<p<1, probability weights and n≥1n\ge1n≥1, the defining sets are nonempty and bounded on the relevant side, so the values are the paper's; at n=0n=0n=0 the estimates are a junk value that no limit statement sees.
  • Conditions (1)–(5) are stated with ∣Wni∣|W_{ni}|∣Wni​∣, as in Theorem 1; for probability weights they coincide with Corollary 1's.

Corrections and choices of range. Proposition 14 is printed for r>1r>1r>1. The proof of Theorem 3 applies it for every r≥1r\ge1r≥1, and the statement is posed for r≥1r\ge1r≥1. Proposition 15 leaves rrr unquantified and is posed for r≥1r\ge1r≥1, the range Theorem 3 uses.

A goal stated through the probabilities of Proposition 13, or through truncated moments, would be a different and weaker theorem; the goal states convergence of the quantile errors (L^n−L)−(\hat L_n-L)^-(L^n​−L)− and (U^n−U)+(\hat U_n-U)^+(U^n​−U)+ themselves, in probability and in LrL^rLr. Swapping the negative and positive parts gives a false statement.

Corollary 1 (necessity) is a special case of Theorem 1, the goal of the first mission of this series; it is posed here as a milestone so that this mission is self-contained, and can be replaced by a reference once that mission is published. Contributions are welcome on any milestone, and on general infrastructure for Markov kernels, conditional distribution functions and quantiles, which is reusable beyond this mission.

Selected references

  • C. J. Stone, Consistent nonparametric regression, Annals of Statistics 5(4), 595–645, 1977. https://doi.org/10.1214/aos/1176343886
  • L. Györfi, M. Kohler, A. Krzyżak, H. Walk, A Distribution-Free Theory of Nonparametric Regression, Springer, 2002. https://doi.org/10.1007/b97848
  • R. Koenker, G. Bassett, Regression quantiles, Econometrica 46(1), 33–50, 1978. https://doi.org/10.2307/1913643
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Convex OptimizationOperations ResearchOptimization·Captain: mikedeng1

Primal-Dual Interior-Point Methods for Self-Scaled Cones II: The Functional-Proximity Predictor-Corrector Step Has α²/(1 − α) ≥ ω₁(Δ, κ)/ν and Boundedly Many Newton CorrectionsResearch Paper

Motivation

Primal-dual interior-point methods are the standard algorithms for linear, second-order-cone and semidefinite programming. Their best-known variants keep the iterates in a narrow neighbourhood of the central path and take short or moderately long steps whose length is fixed in advance. Practical codes instead take long steps and recentre only when needed. Nesterov and Todd (SIAM J. Optim. 8 (1998) 324–364) developed a common theory of primal-dual methods for all self-scaled cones, the class that contains the nonnegative orthant, the second-order cone, the cone of positive semidefinite matrices, and their products. Section 7 of that paper analyses a predictor-corrector method whose neighbourhood is defined by the functional proximity measure γF\gamma_FγF​, the conic version of the Tanabe–Todd–Ye potential. The predictor may move arbitrarily far from the central path, as measured by γF\gamma_FγF​, and a Newton corrector brings the iterate back.

Timeline:

  • 1994: Nesterov and Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, develop self-concordant barriers and logarithmically homogeneous barriers.
  • 1997: Nesterov and Todd, Self-scaled barriers and interior-point methods for convex programming (Math. Oper. Res. 22 (1997) 1–42), introduce self-scaled barriers and the scaling point.
  • 1998: the paper of this mission proves the symmetric primal-dual estimates and the complexity of the functional-proximity predictor-corrector method (Theorem 7.1).

Setting

Let E=RnE=\mathbb R^nE=Rn with the Euclidean inner product, and let K⊆EK\subseteq EK⊆E be a closed convex cone that is pointed and has nonempty interior. Its dual cone is K∗={s:⟨s,x⟩≥0 ∀x∈K}K^*=\{s:\langle s,x\rangle\ge0\ \forall x\in K\}K∗={s:⟨s,x⟩≥0 ∀x∈K}. A ν\nuν-self-concordant logarithmically homogeneous barrier FFF for KKK is a self-concordant function on int⁡K\operatorname{int}KintK that tends to +∞+\infty+∞ at the boundary and satisfies (F′(x)h)2≤ν⟨F′′(x)h,h⟩(F'(x)h)^2\le\nu\langle F''(x)h,h\rangle(F′(x)h)2≤ν⟨F′′(x)h,h⟩ and F(τx)=F(x)−νln⁡τF(\tau x)=F(x)-\nu\ln\tauF(τx)=F(x)−νlnτ. Its conjugate is F∗(s)=sup⁡{−⟨s,x⟩−F(x):x∈int⁡K}F_*(s)=\sup\{-\langle s,x\rangle-F(x):x\in\operatorname{int}K\}F∗​(s)=sup{−⟨s,x⟩−F(x):x∈intK}. FFF is self-scaled if, for all w,x∈int⁡Kw,x\in\operatorname{int}Kw,x∈intK, F′′(w)x∈int⁡K∗F''(w)x\in\operatorname{int}K^*F′′(w)x∈intK∗ and F∗(F′′(w)x)=F(x)−2F(w)−νF_*(F''(w)x)=F(x)-2F(w)-\nuF∗​(F′′(w)x)=F(x)−2F(w)−ν. For x∈int⁡Kx\in\operatorname{int}Kx∈intK and s∈int⁡K∗s\in\operatorname{int}K^*s∈intK∗, the scaling point w∈int⁡Kw\in\operatorname{int}Kw∈intK satisfies F′′(w)x=sF''(w)x=sF′′(w)x=s.

The problem is min⁡{⟨c,x⟩:Ax=b, x∈K}\min\{\langle c,x\rangle:Ax=b,\ x\in K\}min{⟨c,x⟩:Ax=b, x∈K} with dual max⁡{⟨b,y⟩:A∗y+s=c, s∈K∗}\max\{\langle b,y\rangle:A^*y+s=c,\ s\in K^*\}max{⟨b,y⟩:A∗y+s=c, s∈K∗}, where A:E→RmA:E\to\mathbb R^mA:E→Rm is surjective. A triple (x,y,s)(x,y,s)(x,y,s) is strictly feasible if x∈int⁡Kx\in\operatorname{int}Kx∈intK, s∈int⁡K∗s\in\operatorname{int}K^*s∈intK∗ and both equality constraints hold. With μ(x,s)=⟨s,x⟩/ν\mu(x,s)=\langle s,x\rangle/\nuμ(x,s)=⟨s,x⟩/ν the functional proximity measure is

γF(x,s)=F(x)+F∗(s)+νln⁡μ(x,s)+ν ≥0,\gamma_F(x,s)=F(x)+F_*(s)+\nu\ln\mu(x,s)+\nu\ \ge0,γF​(x,s)=F(x)+F∗​(s)+νlnμ(x,s)+ν ≥0,

and it vanishes exactly on the central path. The neighbourhood is F(β)={(x,y,s) strictly feasible:γF(x,s)≤β}\mathcal F(\beta)=\{(x,y,s)\ \text{strictly feasible}:\gamma_F(x,s)\le\beta\}F(β)={(x,y,s) strictly feasible:γF​(x,s)≤β}. The affine-scaling direction (px,py,ps)(p_x,p_y,p_s)(px​,py​,ps​) solves F′′(w)px+ps=sF''(w)p_x+p_s=sF′′(w)px​+ps​=s, Apx=0Ap_x=0Apx​=0, A∗py+ps=0A^*p_y+p_s=0A∗py​+ps​=0. The centering direction (dx,dy,ds)(d_x,d_y,d_s)(dx​,dy​,ds​) solves the same system with right-hand side s+μ(x,s)F′(x)s+\mu(x,s)F'(x)s+μ(x,s)F′(x). One Newton step moves by −α(dx,dy,ds)-\alpha(d_x,d_y,d_s)−α(dx​,dy​,ds​), with α=1/(1+γ∞+σˉ)\alpha=1/(1+\gamma_\infty+\bar\sigma)α=1/(1+γ∞​+σˉ), where γ∞\gamma_\inftyγ∞​ is the uniform proximity measure and σˉ=max⁡{σx(dx),σs(ds)}\bar\sigma=\max\{\sigma_x(d_x),\sigma_s(d_s)\}σˉ=max{σx​(dx​),σs​(ds​)}.

One iteration of Algorithm 7.1 starts from (x,y,s)∈F(β)(x,y,s)\in\mathcal F(\beta)(x,y,s)∈F(β). It takes the largest predictor step α\alphaα along the affine-scaling direction with γF=β+Δ\gamma_F=\beta+\DeltaγF​=β+Δ, then applies Newton steps until the iterate is back in F(β)\mathcal F(\beta)F(β).

Formalization targets

Goal: Theorem 7.1

Let β=κ−ln⁡(1+κ)\beta=\kappa-\ln(1+\kappa)β=κ−ln(1+κ) with κ∈(0,1)\kappa\in(0,1)κ∈(0,1) and Δ>0\Delta>0Δ>0. There are constants ω1,ω2>0\omega_1,\omega_2>0ω1​,ω2​>0, depending only on Δ\DeltaΔ and κ\kappaκ, such that one iteration of Algorithm 7.1 on any self-scaled cone satisfies

⟨s+,x+⟩≤(1−α)⟨s,x⟩,α21−α≥ω1ν,α21−α≥ω2∣px∣x ∥ps∥s≥ω2ν ∣px∣x ∣ps∣s,\langle s_+,x_+\rangle\le(1-\alpha)\langle s,x\rangle,\qquad \frac{\alpha^2}{1-\alpha}\ge\frac{\omega_1}{\nu},\qquad \frac{\alpha^2}{1-\alpha}\ge\frac{\omega_2}{|p_x|_x\,\|p_s\|_s}\ge\frac{\omega_2}{\sqrt\nu\,|p_x|_x\,|p_s|_s},⟨s+​,x+​⟩≤(1−α)⟨s,x⟩,1−αα2​≥νω1​​,1−αα2​≥∣px​∣x​∥ps​∥s​ω2​​≥ν​∣px​∣x​∣ps​∣s​ω2​​,

and the corrector reaches F(β)\mathcal F(\beta)F(β) after N≤⌈Δ/(τˉ−ln⁡(1+τˉ))⌉N\le\lceil\Delta/(\bar\tau-\ln(1+\bar\tau))\rceilN≤⌈Δ/(τˉ−ln(1+τˉ))⌉ Newton steps, where τˉ=123β/(1+β)\bar\tau=\tfrac12\sqrt{3\beta/(1+\beta)}τˉ=21​3β/(1+β)​. The constants are left existential, as on the page.

Milestones

In the paper's order, the milestones are:

  • the σ-identities at the scaling point (Lemma 3.4);
  • the norm comparison ∣a∣b≤∥a∥b≤ν∣a∣b|a|_b\le\|a\|_b\le\sqrt\nu|a|_b∣a∣b​≤∥a∥b​≤ν​∣a∣b​ (Proposition 3.5);
  • the third-derivative bounds (Theorem 3.8) and the parallelogram rule (Theorem 3.11);
  • the barrier form of γF\gamma_FγF​ (Lemma 3.12);
  • the relations between the proximity measures (Theorem 4.2, (4.28)) and the comparison of metrics at xxx, sss, www (Lemma 4.3);
  • the properties of the affine-scaling direction (Lemma 5.2) and the exact change of γF\gamma_FγF​ along it (Theorem 5.3, Lemma 5.4);
  • the properties of the centering direction (Lemma 5.6) and the decrease of γF\gamma_FγF​ per Newton step (Theorem 5.7).

Significance

Theorem 7.1 gives an O(νln⁡(⟨s0,x0⟩/ϵ))O(\sqrt\nu\ln(\langle s_0,x_0\rangle/\epsilon))O(ν​ln(⟨s0​,x0​⟩/ϵ)) iteration bound for a method whose predictor neighbourhood F(β+Δ)\mathcal F(\beta+\Delta)F(β+Δ) can be as wide as desired, with a bounded number of corrector steps per iteration. Inequality (7.3) also lets the step adapt to the problem: in the paper's normalisation the predictor step is at least of the order of the square root of the maximal feasible step. The same bounds apply to the narrow-neighbourhood predictor-corrector method of Section 6. One theorem covers linear, second-order-cone and semidefinite programming, with no reformulation through matrices.

The result is proved in the paper. No machine-checked proof of it, or of any of the self-scaled-barrier estimates it rests on, is known. Formalizing the proof produces a reusable library of local norms, σ-measures and third-derivative bounds for self-scaled barriers, and of the proximity measures of primal-dual methods.

Difficulty

A naive argument would bound the predictor step with the usual self-concordance estimate ∣F′′′(x)[p,p,p]∣≤2∥p∥x3|F'''(x)[p,p,p]|\le2\|p\|_x^3∣F′′′(x)[p,p,p]∣≤2∥p∥x3​. That bound loses a factor ν\sqrt\nuν​ and cannot give (7.2) or (7.3). What is needed is the sharper self-scaled bound (3.14), in which one factor is the smaller norm ∣p∣x|p|_x∣p∣x​. It in turn depends on the cone being self-scaled: F′′′(x)[v]F'''(x)[v]F′′′(x)[v] must be negative semidefinite for v∈Kv\in Kv∈K, and the scaling point must exist. The other obstacle is that the change of γF\gamma_FγF​ along the affine-scaling direction must be computed exactly, not just estimated. That is the parallelogram rule (Theorem 3.11), an identity special to self-scaled barriers. The corrector bound needs a lower bound on the Newton decrement that holds uniformly outside F(β)\mathcal F(\beta)F(β), which (4.28) supplies.

Formalization scope

  • Spaces. The dual space E∗E^*E∗ is identified with EEE through the inner product. Which local norm is meant is carried by the function used:

    • lnorm G v u and dnorm G v u, with G=FG=FG=F or G=F∗G=F_*G=F∗​;
    • sigma C c u =min⁡{β≥0:βc−u∈C}=\min\{\beta\ge0:\beta c-u\in C\}=min{β≥0:βc−u∈C}, with the cone CCC and the centre ccc fixed by the paper's four cases.

    Each two-form measure uses its first printed form.

  • Standing assumptions. Every statement assumes that KKK is a proper cone and that FFF is a ν\nuν-self-scaled barrier, and it also states ν≥1\nu\ge1ν≥1, which the paper derives. The barrier includes explicit nondegeneracy of F′′F''F′′, which also follows from the other axioms. The conjugate is a supremum over int⁡K\operatorname{int}KintK and is only evaluated on int⁡K∗\operatorname{int}K^*intK∗. Assumptions (2.4)–(2.5) are implied by the strictly feasible points that the statements start from.

  • Scaling points, directions and steps are predicates given by their defining equations; nothing is computed by inverting a matrix.

  • Corrections to the page. Two printed slips are corrected, and both are disclosed:

    • the predictor point of Algorithm 7.1 is (x−αpx,y−αpy,s−αps)(x-\alpha p_x,y-\alpha p_y,s-\alpha p_s)(x−αpx​,y−αpy​,s−αps​);
    • (7.4) is stated with a ceiling, since N≥1N\ge1N≥1 while the printed right-hand side can be below 111.
  • Ruling out trivial versions. The goal does not assume any of the following; they are milestones, not hypotheses:

    • the identity (7.5);
    • the bounds of Lemma 5.4;
    • the decrease of Theorem 5.7;
    • the gap identity (5.9).

    The constants ω1,ω2\omega_1,\omega_2ω1​,ω2​ are quantified before the cone, the barrier and the data, so they cannot depend on them. The predictor step is the largest step whose whole segment stays strictly feasible.

  • Out of scope. No self-scaled barrier, existence of scaling points (T*3.2 of [NT97]), or result of Nesterov–Nemirovskii is formalized here. These and the central-path duality theorem (Theorem 4.1) are external results. Proofs that build them are welcome, as is a non-vacuity witness for the goal on the orthant of R2\mathbb R^2R2.

Selected references

  • Yu. E. Nesterov and M. J. Todd, Primal-dual interior-point methods for self-scaled cones, SIAM J. Optim. 8 (1998) 324–364. https://doi.org/10.1137/S1052623495290209
  • Yu. E. Nesterov and M. J. Todd, Self-scaled barriers and interior-point methods for convex programming, Math. Oper. Res. 22 (1997) 1–42. https://doi.org/10.1287/moor.22.1.1
  • Yu. Nesterov and A. Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
  • O. Güler, Barrier functions in interior point methods, Math. Oper. Res. 21 (1996) 860–885. https://doi.org/10.1287/moor.21.4.860
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ProbabilityStochastic Systems·Captain: mikedeng1

The Two-Parameter Poisson–Dirichlet Distribution Derived from a Stable Subordinator 4: The Density of V_1 under PD(α, θ) Is Determined by the PD(α, α + θ) Law of V_1Research Paper

Motivation

A random discrete distribution is a random sequence of frequencies V1≥V2≥⋯≥0V_1 \ge V_2 \ge \cdots \ge 0V1​≥V2​≥⋯≥0 with ∑nVn=1\sum_n V_n = 1∑n​Vn​=1. Such sequences model the relative sizes of species in a large population, of allele classes in population genetics, of cycles of a random permutation, of prime factors of a random integer, and of the excursion intervals of a Brownian motion or Bessel process. The two-parameter Poisson–Dirichlet family PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ), 0≤α<10 \le \alpha < 10≤α<1, θ>−α\theta > -\alphaθ>−α, contains Kingman's one-parameter law PD(0,θ)\mathrm{PD}(0,\theta)PD(0,θ) (Ewens sampling formula, random permutations) and the law PD(α,0)\mathrm{PD}(\alpha, 0)PD(α,0) of the ranked jumps of a stable subordinator. It is the reference prior in Bayesian nonparametrics (the Pitman–Yor process) and the reference model in the combinatorics of random partitions.

J. Pitman and M. Yor, The two-parameter Poisson–Dirichlet distribution derived from a stable subordinator (Ann. Probab. 25 (1997)), extend what was known for PD(0,θ)\mathrm{PD}(0,\theta)PD(0,θ) and PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0) to the whole family. This mission formalizes one of their results: an identity (Proposition 19, p. 867) that describes the law of the largest frequency V1V_1V1​ under PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) through the law of the largest frequency under PD(α,α+θ)\mathrm{PD}(\alpha,\alpha+\theta)PD(α,α+θ).

Timeline. McCloskey (1965) showed that sampling from PD(0,θ)\mathrm{PD}(0,\theta)PD(0,θ) discovers the frequencies in the stick-breaking order of independent beta(1,θ)\mathrm{beta}(1,\theta)beta(1,θ) variables. Dickman (1930) found the distribution of the largest prime factor; Vershik (1986) recorded it as the case α=0\alpha = 0α=0, θ=1\theta = 1θ=1 of an equation of this form. Engen (1978) introduced the two-parameter stick-breaking scheme for θ>0\theta > 0θ>0. Perman, Pitman and Yor (1992) and Pitman (1996) proved that this scheme is the size-biased permutation of the ranked frequencies for the whole parameter range (Proposition 2 here). Pitman and Yor (1997) derived (52) for all 0≤α<10 \le \alpha < 10≤α<1, θ>−α\theta > -\alphaθ>−α.

Setting

Fix 0≤α<10 \le \alpha < 10≤α<1 and θ>−α\theta > -\alphaθ>−α. Let Y~1,Y~2,…\tilde Y_1, \tilde Y_2, \dotsY~1​,Y~2​,… be independent random variables, Y~n\tilde Y_nY~n​ having the beta distribution beta(1−α,θ+nα)\mathrm{beta}(1-\alpha, \theta + n\alpha)beta(1−α,θ+nα), with density Γ(a+b)Γ(a)Γ(b)xa−1(1−x)b−1\frac{\Gamma(a+b)}{\Gamma(a)\Gamma(b)}x^{a-1}(1-x)^{b-1}Γ(a)Γ(b)Γ(a+b)​xa−1(1−x)b−1 on (0,1)(0,1)(0,1) for a=1−αa = 1-\alphaa=1−α, b=θ+nαb = \theta+n\alphab=θ+nα. Break a stick of length one:

V~1=Y~1,V~n=(1−Y~1)⋯(1−Y~n−1) Y~n(n≥2).(4)\tilde V_1 = \tilde Y_1, \qquad \tilde V_n = (1-\tilde Y_1)\cdots(1-\tilde Y_{n-1})\,\tilde Y_n \quad (n \ge 2). \tag{4}V~1​=Y~1​,V~n​=(1−Y~1​)⋯(1−Y~n−1​)Y~n​(n≥2).(4)

Let V1≥V2≥⋯V_1 \ge V_2 \ge \cdotsV1​≥V2​≥⋯ be the ranked values of the pieces V~n\tilde V_nV~n​. The law of (Vn)(V_n)(Vn​) is PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) (Definition 1, p. 857); Pα,θP_{\alpha,\theta}Pα,θ​ denotes probability for this construction.

A random variable V~1\tilde V_1V~1​ is a size-biased pick from (Vn)(V_n)(Vn​) if P(V~1=Vn∣V1,V2,… )=VnP(\tilde V_1 = V_n \mid V_1, V_2, \dots) = V_nP(V~1​=Vn​∣V1​,V2​,…)=Vn​ for every nnn: it is the frequency of the species of an individual drawn at random. A size-biased permutation continues the sampling without replacement, (2) and p. 857. A sample from (Vn)(V_n)(Vn​) is a random index NNN with P(N=n∣V)=VnP(N = n \mid V) = V_nP(N=n∣V)=Vn​ (113).

In Lean all sequences are ℕ → ℝ, 0-based (V ω 0 is V1V_1V1​); the objects are stick, ranked, IsStickLaw, HasPD, IsSizeBiasedPick, IsSizeBiasedPerm, IsSample, deleteAt, insertAt in the namespace PoissonDirichlet.MaxDensity.

Formalization targets

Goal: Proposition 19, identity (52)

For 0≤α<10 \le \alpha < 10≤α<1, θ>−α\theta > -\alphaθ>−α, the variable V1V_1V1​ lies in (0,1)(0,1)(0,1) almost surely and

Pα,θ(V1∈dx)dx=Γ(θ+1)Γ(θ+α)Γ(1−α) x−α−1(1−x)α+θ−1  Pα,α+θ ⁣(V1<x1−x),0<x<1.\frac{P_{\alpha,\theta}(V_1 \in dx)}{dx} = \frac{\Gamma(\theta+1)}{\Gamma(\theta+\alpha)\Gamma(1-\alpha)}\, x^{-\alpha-1}(1-x)^{\alpha+\theta-1}\; P_{\alpha,\alpha+\theta}\!\left(V_1 < \frac{x}{1-x}\right), \qquad 0 < x < 1.dxPα,θ​(V1​∈dx)​=Γ(θ+α)Γ(1−α)Γ(θ+1)​x−α−1(1−x)α+θ−1Pα,α+θ​(V1​<1−xx​),0<x<1.

Milestones

  1. Proposition 2 (p. 857): V1>V2>⋯>0V_1 > V_2 > \cdots > 0V1​>V2​>⋯>0, ∑nVn=1\sum_n V_n = 1∑n​Vn​=1 a.s., and (V~n)(\tilde V_n)(V~n​) is a size-biased permutation of (Vn)(V_n)(Vn​).
  2. Corollary 3 (p. 858): every size-biased pick from a PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) sequence has the beta(1−α,θ+α)\mathrm{beta}(1-\alpha,\theta+\alpha)beta(1−α,θ+α) law.
  3. Display (6) (p. 858): E∑nf(Vn)=E[f(V~1)/V~1]=Γ(θ+1)Γ(θ+α)Γ(1−α)∫01f(u)(1−u)α+θ−1u−α−1 duE\sum_n f(V_n) = E[f(\tilde V_1)/\tilde V_1] = \frac{\Gamma(\theta+1)}{\Gamma(\theta+\alpha)\Gamma(1-\alpha)}\int_0^1 f(u)(1-u)^{\alpha+\theta-1}u^{-\alpha-1}\,duE∑n​f(Vn​)=E[f(V~1​)/V~1​]=Γ(θ+α)Γ(1−α)Γ(θ+1)​∫01​f(u)(1−u)α+θ−1u−α−1du.
  4. The stick-tail identity (p. 876): (V~2,V~3,… )/(1−V~1)(\tilde V_2, \tilde V_3, \dots)/(1-\tilde V_1)(V~2​,V~3​,…)/(1−V~1​) has the Pα,α+θP_{\alpha,\alpha+\theta}Pα,α+θ​ law of (V~1,V~2,… )(\tilde V_1, \tilde V_2, \dots)(V~1​,V~2​,…), independently of V~1\tilde V_1V~1​.
  5. Display (91) (p. 876): Pα,θ(V1∈dx,V1=V~1)=x Pα,θ(V1∈dx)P_{\alpha,\theta}(V_1 \in dx, V_1 = \tilde V_1) = x\,P_{\alpha,\theta}(V_1 \in dx)Pα,θ​(V1​∈dx,V1​=V~1​)=xPα,θ​(V1​∈dx).
  6. Display (92) (p. 876): the same quantity equals Γ(θ+1)Γ(θ+α)Γ(1−α)x−α(1−x)α+θ−1 dx Pα,α+θ(V1<x/(1−x))\frac{\Gamma(\theta+1)}{\Gamma(\theta+\alpha)\Gamma(1-\alpha)}x^{-\alpha}(1-x)^{\alpha+\theta-1}\,dx\,P_{\alpha,\alpha+\theta}(V_1 < x/(1-x))Γ(θ+α)Γ(1−α)Γ(θ+1)​x−α(1−x)α+θ−1dxPα,α+θ​(V1​<x/(1−x)).
  7. Uniqueness (p. 877): (52), imposed for all θ>−α\theta > -\alphaθ>−α, determines the family of laws of V1V_1V1​.
  8. Propositions 34 and 35 (p. 881): deleting a sampled frequency and renormalising maps PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) to PD(α,θ+α)\mathrm{PD}(\alpha,\theta+\alpha)PD(α,θ+α), independently of VN∼beta(1−α,θ+α)V_N \sim \mathrm{beta}(1-\alpha,\theta+\alpha)VN​∼beta(1−α,θ+α); inserting an independent beta variable reverses it.

Significance

The result. The law of V1V_1V1​ under PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) has no closed form. Identity (52) is a functional equation in the parameter: on (1/2,1)(1/2,1)(1/2,1) the last factor equals one and the density is explicit; on (1/(n+1),1/n)(1/(n+1), 1/n)(1/(n+1),1/n) it is expressed through the law of V1V_1V1​ under PD(α,α+θ)\mathrm{PD}(\alpha,\alpha+\theta)PD(α,α+θ) on (1/n,1)(1/n, 1)(1/n,1). Specialised to α=0\alpha = 0α=0, θ=1\theta = 1θ=1 it is Dickman's equation for the largest prime factor of a random integer and for the longest cycle of a random permutation. The size-biased tools of the milestones (Corollary 3, (6), Propositions 34 and 35) are the standard way to compute with PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) and its partition structure.

Formalizing it. All results here are proved in the literature; none is formalized. Mathlib has the beta distribution, infinite product measures, independence and conditional expectation, but no random discrete distributions, no ranking of a countable sequence, and no size-biased sampling. The mission produces these objects and the first theorems about them: the identification of the stick-breaking scheme with the size-biased permutation of the ranked frequencies (cited by the paper, not proved there), the structural distribution, and the density identity.

Difficulty

The obvious obstacle is Proposition 2: the identification of the stick-breaking order with the size-biased order of the ranked values is a statement about conditional probabilities given an infinite sequence, it is only cited in the paper, and its proof (Perman–Pitman–Yor, Pitman) goes through exchangeable partitions or Poisson point processes. Everything else in the mission rests on it. A second obstacle is the events themselves: {V1=V~1}\{V_1 = \tilde V_1\}{V1​=V~1​} coincides with {max⁡n≥2V~n<V~1}\{\max_{n \ge 2}\tilde V_n < \tilde V_1\}{maxn≥2​V~n​<V~1​} only because the pieces are almost surely distinct, and conditioning on V~1=x\tilde V_1 = xV~1​=x needs the independence of the renormalised tail from V~1\tilde V_1V~1​, which is not a pointwise identity but a statement about infinite product measures. Reading (52) off the page as a pointwise identity of densities is not enough: densities are defined only almost everywhere.

Formalization scope

The parameter range 0≤α<10 \le \alpha < 10≤α<1, θ>−α\theta > -\alphaθ>−α of Definition 1 is a hypothesis of every statement; α=0\alpha = 0α=0 is included. A sequence "has the PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) distribution" (HasPD) if it is a.e.-measurable and, for some law μ\muμ of independent beta variables as in Definition 1 (IsStickLaw), P(V∈S)=μ(ranked stick∈S)P(V \in S) = \mu(\text{ranked stick} \in S)P(V∈S)=μ(ranked stick∈S) for every measurable SSS. Ranked values are defined with Set.encard, so infinitely many large terms are never counted as zero. Conditional probabilities are conditional expectations of indicators; size-biased picks, permutations and samples are measurable random variables, an assumption the page makes implicitly. Expectations of nonnegative functions are lower Lebesgue integrals. The density identity is an equality of measures on Borel subsets of (0,1)(0,1)(0,1), with two probability spaces for the two parameter values. Indices are 0-based. Insertion (p. 881) is defined with the index n−1n-1n−1 for the shifted tail, where the page prints n+1n+1n+1.

The formalization rules out the trivial readings: no Measure.map of a possibly non-measurable map (which would be the zero measure), no Set.ncard in the ranking, no Bochner integral of a possibly non-integrable function (whose value would be 000), no limUnder, and no dropped parameter range. Corollary 3 quantifies over every pick from every PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) sequence, not over the stick-breaking construction where it is the hypothesis. A sorry-free check shows that IsStickLaw is inhabited for every admissible (α,θ)(\alpha,\theta)(α,θ), so HasPD is not vacuous.

Contributions are welcome at every level: measurability of ranked, the law of the renormalised stick tail (infinite product measures), Proposition 2 through exchangeable partitions, and the recursion of the uniqueness statement, which is pure measure theory. The definitions are reusable by the other missions of this series.

Selected references

  • J. Pitman and M. Yor, The two-parameter Poisson–Dirichlet distribution derived from a stable subordinator, Ann. Probab. 25(2):855–900, 1997. https://doi.org/10.1214/aop/1024404422
  • M. Perman, J. Pitman and M. Yor, Size-biased sampling of Poisson point processes and excursions, Probab. Theory Related Fields 92:21–39, 1992. https://doi.org/10.1007/BF01205234
  • J. Pitman, Random discrete distributions invariant under size-biased permutation, Adv. Appl. Probab. 28:525–539, 1996. https://doi.org/10.2307/1428070
  • K. Dickman, On the frequency of numbers containing prime factors of a certain relative magnitude, Arkiv för Matematik, Astronomi och Fysik 22:1–14, 1930.
  • S. Engen, Stochastic Abundance Models, Chapman and Hall, 1978.
  • J. W. McCloskey, A model for the distribution of individuals by species in an environment, PhD thesis, Michigan State University, 1965.
  • A. M. Vershik, The asymptotic distribution of factorizations of natural numbers into prime divisors, Soviet Math. Dokl. 34:57–61, 1986.
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ProbabilityStochastic Systems·Captain: mikedeng1

The Two-Parameter Poisson–Dirichlet Distribution Derived from a Stable Subordinator 3: Moments E_{α,θ}(V_n^p) of the n-th Largest PD(α, θ) Frequency as One Integral of φ_α and ψ_αResearch Paper

Motivation

Random discrete distributions — a random sequence of nonnegative frequencies V1≥V2≥…V_1\ge V_2\ge\dotsV1​≥V2​≥… summing to one — model the relative sizes of species in a population, of cycles in a random permutation, of excursion intervals of a Markov process, and of clusters in Bayesian nonparametric models. The two-parameter Poisson–Dirichlet law PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) is the family that contains Kingman's one-parameter law PD(0,θ)\mathrm{PD}(0,\theta)PD(0,θ) (Ewens sampling, random permutations) and the law PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0) of ranked excursion lengths of a stable subordinator. J. Pitman and M. Yor, The two-parameter Poisson–Dirichlet distribution derived from a stable subordinator (Ann. Probab. 25 (1997)), developed its distribution theory systematically. In Bayesian nonparametrics the same family appears as the Pitman–Yor process prior.

A basic quantitative question about any random discrete distribution is the size of its nnn-th largest atom. This mission formalizes the paper's answer for PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ): every moment E(Vnp)E(V_n^p)E(Vnp​) as one explicit integral.

Timeline. The moment formula for PD(0,θ)\mathrm{PD}(0,\theta)PD(0,θ) (Corollary 18 below) was known before 1997 (references [63, 73, 25, 50] of the paper). The Laplace transform of 1/Vn1/V_n1/Vn​ under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0) was obtained, in different settings, by Darling (1952) and Lamperti (1961) for n=1n=1n=1 and by Wendel (1964) for n=2,3,…n=2,3,\dotsn=2,3,…. Perman, Pitman and Yor (1992) proved that PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) has density a constant times Lθ/αL^{\theta/\alpha}Lθ/α relative to PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0). Pitman and Yor (1997) combined these into Proposition 17.

Setting

Fix 0≤α<10\le\alpha<10≤α<1 and θ>−α\theta>-\alphaθ>−α. Let Y~1,Y~2,…\tilde Y_1,\tilde Y_2,\dotsY~1​,Y~2​,… be independent with Y~n∼beta(1−α,θ+nα)\tilde Y_n\sim\mathrm{beta}(1-\alpha,\theta+n\alpha)Y~n​∼beta(1−α,θ+nα), the law with density Γ(a+b)Γ(a)Γ(b)xa−1(1−x)b−1\frac{\Gamma(a+b)}{\Gamma(a)\Gamma(b)}x^{a-1}(1-x)^{b-1}Γ(a)Γ(b)Γ(a+b)​xa−1(1−x)b−1 on (0,1)(0,1)(0,1). Break a unit stick:

V~1=Y~1,V~n=(1−Y~1)⋯(1−Y~n−1)Y~n(n≥2),\tilde V_1=\tilde Y_1,\qquad \tilde V_n=(1-\tilde Y_1)\cdots(1-\tilde Y_{n-1})\tilde Y_n\quad(n\ge2),V~1​=Y~1​,V~n​=(1−Y~1​)⋯(1−Y~n−1​)Y~n​(n≥2),

and let V1≥V2≥…V_1\ge V_2\ge\dotsV1​≥V2​≥… be the ranked values of the V~n\tilde V_nV~n​. The law of (Vn)(V_n)(Vn​) is PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) (Definition 1); Eα,θE_{\alpha,\theta}Eα,θ​ denotes expectation under it.

For 0<α<10<\alpha<10<α<1 and λ≥0\lambda\ge0λ≥0 the paper introduces

ϕα(λ)=α∫1∞e−λxx−α−1 dx,ψα(λ)=1+α∫01(1−e−λx)x−α−1 dx.\phi_\alpha(\lambda)=\alpha\int_1^\infty e^{-\lambda x}x^{-\alpha-1}\,dx,\qquad \psi_\alpha(\lambda)=1+\alpha\int_0^1(1-e^{-\lambda x})x^{-\alpha-1}\,dx .ϕα​(λ)=α∫1∞​e−λxx−α−1dx,ψα​(λ)=1+α∫01​(1−e−λx)x−α−1dx.

Under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0) the local time L=lim⁡n→∞nVnαL=\lim_{n\to\infty}nV_n^\alphaL=limn→∞​nVnα​ exists almost surely. From (Vn)(V_n)(Vn​) one derives Rn=Vn+1/VnR_n=V_{n+1}/V_nRn​=Vn+1​/Vn​, An=(V1+⋯+Vn)/Vn+1A_n=(V_1+\dots+V_n)/V_{n+1}An​=(V1​+⋯+Vn​)/Vn+1​ (with A0=0A_0=0A0​=0) and Xn=LVn−αX_n=LV_n^{-\alpha}Xn​=LVn−α​. Finally

Cα,θ=Γ(θ+1)Γ(θ/α+1)Γ(1−α)θ/α.C_{\alpha,\theta}=\frac{\Gamma(\theta+1)}{\Gamma(\theta/\alpha+1)}\Gamma(1-\alpha)^{\theta/\alpha}.Cα,θ​=Γ(θ/α+1)Γ(θ+1)​Γ(1−α)θ/α.

The Lean declarations Xseq, pdConst, and expIntE are in PoissonDirichlet.Moments; the other objects come from the frozen shared PoissonDirichlet.Ratio and PoissonDirichlet.Wendel modules.

Formalization targets

Goal: Proposition 17

For 0<α<10<\alpha<10<α<1, θ>−α\theta>-\alphaθ>−α, p>0p>0p>0 with θ+p>0\theta+p>0θ+p>0, and n=1,2,…n=1,2,\dotsn=1,2,…,

Eα,θ(Vnp)=Γ(1−α)θ/αΓ(n)Γ(θ+1)Γ(θ+p)Γ(θ/α+n)Γ(θ/α+1)∫0∞tp+θ−1e−tϕα(t)n−1ψα(t)−θ/α−n dt.E_{\alpha,\theta}(V_n^p)=\frac{\Gamma(1-\alpha)^{\theta/\alpha}}{\Gamma(n)}\frac{\Gamma(\theta+1)}{\Gamma(\theta+p)}\frac{\Gamma(\theta/\alpha+n)}{\Gamma(\theta/\alpha+1)}\int_0^\infty t^{p+\theta-1}e^{-t}\phi_\alpha(t)^{n-1}\psi_\alpha(t)^{-\theta/\alpha-n}\,dt .Eα,θ​(Vnp​)=Γ(n)Γ(1−α)θ/α​Γ(θ+p)Γ(θ+1)​Γ(θ/α+1)Γ(θ/α+n)​∫0∞​tp+θ−1e−tϕα​(t)n−1ψα​(t)−θ/α−ndt.

Milestones, in attack order

  1. (86): for X>0X>0X>0 a.s. and p>0p>0p>0, E[X−p]=1Γ(p)∫0∞tp−1E[e−tX] dtE[X^{-p}]=\frac1{\Gamma(p)}\int_0^\infty t^{p-1}E[e^{-tX}]\,dtE[X−p]=Γ(p)1​∫0∞​tp−1E[e−tX]dt.
  2. Proposition 26: under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0), E[exp⁡(−λ/Vn)∣R1,…,Rn−1,Xn]=exp⁡(−λ(1+An−1))exp⁡[−Xn(ψα(λ)−1)]E[\exp(-\lambda/V_n)\mid R_1,\dots,R_{n-1},X_n]=\exp(-\lambda(1+A_{n-1}))\exp[-X_n(\psi_\alpha(\lambda)-1)]E[exp(−λ/Vn​)∣R1​,…,Rn−1​,Xn​]=exp(−λ(1+An−1​))exp[−Xn​(ψα​(λ)−1)].
  3. (36): under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0), E[exp⁡(−λAn−1)]=ϕα(λ)n−1E[\exp(-\lambda A_{n-1})]=\phi_\alpha(\lambda)^{n-1}E[exp(−λAn−1​)]=ϕα​(λ)n−1.
  4. Under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0), XnX_nXn​ is gamma(n)\mathrm{gamma}(n)gamma(n) and independent of An−1A_{n-1}An−1​.
  5. Lemma 27: under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0), for ℓ>−1\ell>-1ℓ>−1, p>0p>0p>0, p+ℓα>0p+\ell\alpha>0p+ℓα>0,
E[LℓVnp]=Γ(ℓ+n)Γ(n)Γ(p+ℓα)∫0∞tp+ℓα−1e−tϕα(t)n−1ψα(t)−ℓ−n dt.E[L^\ell V_n^p]=\frac{\Gamma(\ell+n)}{\Gamma(n)\Gamma(p+\ell\alpha)}\int_0^\infty t^{p+\ell\alpha-1}e^{-t}\phi_\alpha(t)^{n-1}\psi_\alpha(t)^{-\ell-n}\,dt .E[LℓVnp​]=Γ(n)Γ(p+ℓα)Γ(ℓ+n)​∫0∞​tp+ℓα−1e−tϕα​(t)n−1ψα​(t)−ℓ−ndt.
  1. Proposition 14: Eα,θ[f(V)]=Cα,θEα,0[Lθ/αf(V)]E_{\alpha,\theta}[f(V)]=C_{\alpha,\theta}E_{\alpha,0}[L^{\theta/\alpha}f(V)]Eα,θ​[f(V)]=Cα,θ​Eα,0​[Lθ/αf(V)] for nonnegative measurable fff, and Cα,θ=1/Eα,0(Lθ/α)C_{\alpha,\theta}=1/E_{\alpha,0}(L^{\theta/\alpha})Cα,θ​=1/Eα,0​(Lθ/α).

Two consequences close the list: (50), np/αEα,θ(Vnp)→Cα,θ/Cα,θ+pn^{p/\alpha}E_{\alpha,\theta}(V_n^p)\to C_{\alpha,\theta}/C_{\alpha,\theta+p}np/αEα,θ​(Vnp​)→Cα,θ​/Cα,θ+p​, and Corollary 18, the PD(0,θ)\mathrm{PD}(0,\theta)PD(0,θ) formula

E0,θ(Vnp)=Γ(θ)Γ(θ+p)θnΓ(n)∫0∞tp−1e−tE(t)n−1e−θE(t) dt,E(t)=∫t∞x−1e−xdx.E_{0,\theta}(V_n^p)=\frac{\Gamma(\theta)}{\Gamma(\theta+p)}\frac{\theta^n}{\Gamma(n)}\int_0^\infty t^{p-1}e^{-t}E(t)^{n-1}e^{-\theta E(t)}\,dt,\qquad E(t)=\int_t^\infty x^{-1}e^{-x}dx .E0,θ​(Vnp​)=Γ(θ+p)Γ(θ)​Γ(n)θn​∫0∞​tp−1e−tE(t)n−1e−θE(t)dt,E(t)=∫t∞​x−1e−xdx.

Significance

The ranked frequencies of PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) have no tractable joint density; their one-dimensional laws are known only through transforms. Proposition 17 makes every moment of VnV_nVn​ computable by a single quadrature, for all parameters at once. It yields the large-nnn decay (50), Vn≈(L/n)1/αV_n\approx(L/n)^{1/\alpha}Vn​≈(L/n)1/α in mean, and recovers the classical PD(0,θ)\mathrm{PD}(0,\theta)PD(0,θ) formula in the limit α↓0\alpha\downarrow0α↓0. The intermediate statements, the conditional Wendel formula and the joint moments E[LℓVnp]E[L^\ell V_n^p]E[LℓVnp​], are used elsewhere in the paper (Proposition 16, Lemma 29).

All statements are proved in the 1997 paper, except Proposition 14, which the paper quotes from Perman, Pitman and Yor (1992). To our knowledge none of them has been machine-checked. A formal development would produce the first verified construction of the Poisson–Dirichlet family in Lean, together with reusable facts about stick-breaking with beta variables, ranked rearrangements of sequences, and the Laplace-transform representation of negative moments.

Difficulty

The identity (86) and the final integration are elementary. The difficulty lies upstream. The naive route, computing E(Vnp)E(V_n^p)E(Vnp​) from the stick-breaking definition, fails: VnV_nVn​ is the nnn-th ranked value of the V~k\tilde V_kV~k​, and ranking destroys the product structure of the beta variables. The paper instead works under PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0), where the ranked sequence is the normalized sequence of points of a Poisson random measure (equivalently, transformed arrival times of a unit Poisson process). Proposition 14 is itself a deep change-of-measure result about stable subordinators, and the existence of the local time LLL is an almost sure limit theorem. Neither has any counterpart in Mathlib.

Formalization scope

Sequences are indexed from 000 in Lean: the paper's VnV_nVn​ is V ω (n-1), and statements "for n=1,2,…n=1,2,\dotsn=1,2,…" quantify over k : ℕ with n=k+1n=k+1n=k+1. PD(α,θ)\mathrm{PD}(\alpha,\theta)PD(α,θ) is defined exactly as Definition 1, with independent beta coordinates (Mathlib's betaMeasure) and the ranked values defined with Set.encard. The law is stated through preimages, so no measurability of the ranking map is presupposed. The local time LLL is carried as a random variable together with its defining almost sure limit (24). Expectations of quantities that may be infinite are lower integrals. The conditional expectation of Proposition 26 is stated through its defining property, for every nonnegative measurable test function of (R1,…,Rn−1,Xn)(R_1,\dots,R_{n-1},X_n)(R1​,…,Rn−1​,Xn​). The parameter ranges 0<α<10<\alpha<10<α<1, θ>−α\theta>-\alphaθ>−α (and θ>0\theta>0θ>0 at α=0\alpha=0α=0) are hypotheses wherever the page has them. Two hypotheses are added and disclosed: θ+p>0\theta+p>0θ+p>0 in Proposition 17 and p+ℓα>0p+\ell\alpha>0p+ℓα>0 in Lemma 27. Without them the printed ttt-integrals diverge and Γ\GammaΓ is evaluated at a pole or a negative argument, while the left sides are finite. Both follow from the printed hypotheses when θ≥0\theta\ge0θ≥0 (resp. ℓ≥0\ell\ge0ℓ≥0).

Trivializing encodings are ruled out: no law is written as an image measure of a possibly non-measurable map, no count uses Set.ncard, no limit uses limUnder, Cα,θC_{\alpha,\theta}Cα,θ​ is not defined as 1/E(Lθ/α)1/E(L^{\theta/\alpha})1/E(Lθ/α), and every Bochner integral in a statement is of an integrable function under the stated hypotheses, so no statement holds because of a junk value 000.

A complete development needs: infinite products of beta laws, the ranked rearrangement and its measurability, the Poisson-process representation of PD(α,0)\mathrm{PD}(\alpha,0)PD(α,0) (Proposition 10), and the change of measure of Proposition 14. These are reusable beyond this mission. Proofs of the general identity (86), of the gamma–independence milestone, and of Lemma 27 from its milestones are welcome independently.

Selected references

  • J. Pitman and M. Yor, The two-parameter Poisson–Dirichlet distribution derived from a stable subordinator, Ann. Probab. 25(2):855–900, 1997. https://doi.org/10.1214/aop/1024404422
  • M. Perman, J. Pitman and M. Yor, Size-biased sampling of Poisson point processes and excursions, Probab. Theory Related Fields 92:21–39, 1992. https://doi.org/10.1007/BF01205234
  • J. G. Wendel, Zero-free intervals of semi-stable Markov processes, Math. Scand. 14:21–34, 1964. https://doi.org/10.7146/math.scand.a-10703
  • J. F. C. Kingman, Random discrete distributions, J. Roy. Statist. Soc. Ser. B 37:1–22, 1975. https://doi.org/10.1111/j.2517-6161.1975.tb01024.x
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Algorithmic Game TheoryAnalysisOperations Research+1·Captain: mikedeng1

Cooperative Fuzzy Games 3: The Diagonal Formula Is the Unique Continuous Linear Pareto-Optimal, Symmetric and Atomic Value of Smooth Fuzzy GamesResearch Paper

Motivation

A value for cooperative games assigns to every game a payoff vector, chosen by axioms rather than by bargaining. Shapley's value (1953) does this for finite games with side payments, and Aumann and Shapley (Values of Non-Atomic Games, 1974) extended it to games with a continuum of players, where it is given by a diagonal formula: a player's value is the average of their marginal worth along the diagonal from the empty coalition to the grand coalition. Aubin's Cooperative Fuzzy Games (Math. Oper. Res. 6(1), 1981, doi:10.1287/moor.6.1.1) brings this formula to finitely many players who may participate in coalitions at fractional rates, and characterises it by axioms in §8.

The result matters in cost allocation: the Aumann–Shapley price mechanism (Billera, Heath and Raanan 1978; Mirman and Tauman 1982) shares the cost of a bundle of products by exactly this diagonal formula, applied to a smooth cost function of the quantities produced. Theorem 8.1 is the finite-player, fuzzy-coalition version of the axiomatic justification behind that mechanism.

Setting

There are nnn players N={1,…,n}N=\{1,\dots,n\}N={1,…,n}. A fuzzy coalition is a vector τ∈[0,1]n\tau\in[0,1]^nτ∈[0,1]n, where τi\tau_iτi​ is the rate at which player iii participates; an ordinary coalition AAA is its indicator vector τA\tau^AτA, and τN=(1,…,1)\tau^N=(1,\dots,1)τN=(1,…,1) is the grand coalition.

A smooth fuzzy game is a coalitional worth function v:[0,1]n→Rv:[0,1]^n\to\mathbb Rv:[0,1]n→R that is continuously differentiable and satisfies v(0)=0v(0)=0v(0)=0. These form the space VnV^nVn, a Banach space under the C1C^1C1 norm sup⁡[0,1]n∣v∣+sup⁡[0,1]n∥Dv∥\sup_{[0,1]^n}|v|+\sup_{[0,1]^n}\|Dv\|sup[0,1]n​∣v∣+sup[0,1]n​∥Dv∥.

A sequence of fuzzy values is a family of continuous linear operators ψn:Vn→Rn\psi_n:V^n\to\mathbb R^nψn​:Vn→Rn satisfying three axioms.

  • Pareto optimality: ∑i∈N(ψnv)i=v(τN)\sum_{i\in N}(\psi_n v)_i=v(\tau^N)∑i∈N​(ψn​v)i​=v(τN).
  • Symmetry: for a permutation θ\thetaθ of NNN, with (θ∗v)(τ)=v(τθ−1(1),…,τθ−1(n))(\theta^*v)(\tau)=v(\tau_{\theta^{-1}(1)},\dots,\tau_{\theta^{-1}(n)})(θ∗v)(τ)=v(τθ−1(1)​,…,τθ−1(n)​) and (θ∗c)i=cθ(i)(\theta^*c)_i=c_{\theta(i)}(θ∗c)i​=cθ(i)​, one has ψn(θ∗v)=θ∗(ψnv)\psi_n(\theta^*v)=\theta^*(\psi_n v)ψn​(θ∗v)=θ∗(ψn​v).
  • Atomicity: a partition P={A1,…,Am}P=\{A_1,\dots,A_m\}P={A1​,…,Am​} of NNN into nonempty types sends a fuzzy coalition σ∈[0,1]m\sigma\in[0,1]^mσ∈[0,1]m of types to the fuzzy coalition (P⋅σ)i=σj(P\cdot\sigma)_i=\sigma_j(P⋅σ)i​=σj​ for i∈Aji\in A_ji∈Aj​, and an nnn-player game vvv to the mmm-type game (P∗v)(σ)=v(P⋅σ)(P^*v)(\sigma)=v(P\cdot\sigma)(P∗v)(σ)=v(P⋅σ). The axiom requires ψm(P∗v)j=∑i∈Aj(ψnv)i\psi_m(P^*v)_j=\sum_{i\in A_j}(\psi_nv)_iψm​(P∗v)j​=∑i∈Aj​​(ψn​v)i​: a type receives what its members receive.

The core of a game vvv with side payments is the set of c∈Rnc\in\mathbb R^nc∈Rn with ∑ici=v(τN)\sum_ic_i=v(\tau^N)∑i​ci​=v(τN) and ∑iτici≥v(τ)\sum_i\tau_ic_i\ge v(\tau)∑i​τi​ci​≥v(τ) for every τ∈[0,1]n\tau\in[0,1]^nτ∈[0,1]n (§2 (4)).

Formalization targets

Goal: Theorem 8.1

There exists a unique sequence of fuzzy values, given by the diagonal formula

ψnv=∫01Dv(tτN) dt(v∈Vn).(4)\psi_n v=\int_0^1 Dv(t\tau^N)\,dt\qquad(v\in V^n).\tag{4}ψn​v=∫01​Dv(tτN)dt(v∈Vn).(4)

For every linear A:Rm→RnA:\mathbb R^m\to\mathbb R^nA:Rm→Rn with AτM=τNA\tau^M=\tau^NAτM=τN,

ψm(v∘A)=A∗ψnv(v∈Vn),(5)\psi_m(v\circ A)=A^*\psi_n v\qquad(v\in V^n),\tag{5}ψm​(v∘A)=A∗ψn​v(v∈Vn),(5)

where A∗A^*A∗ is the transpose of AAA. If v∈Vnv\in V^nv∈Vn is concave and positively homogeneous, then ψnv\psi_nvψn​v is the unique element of the core.

Milestones

These are the steps of the proof in the paper (pp. 10–11), in attack order:

  1. the maps (4) are linear, continuous and satisfy (5);
  2. they satisfy the Pareto optimality, symmetry and atomicity axioms;
  3. the monomials τ1k1⋯τnkn\tau_1^{k_1}\cdots\tau_n^{k_n}τ1k1​​⋯τnkn​​ (k≠0k\ne0k=0) span a dense subspace of VnV^nVn;
  4. Pareto optimality and symmetry force ψn(τ1⋯τn)=1nτN\psi_n(\tau_1\cdots\tau_n)=\frac1n\tau^Nψn​(τ1​⋯τn​)=n1​τN;
  5. the three axioms force (ψnτk)i=ki/(k1+⋯+kn)(\psi_n\tau^k)_i=k_i/(k_1+\dots+k_n)(ψn​τk)i​=ki​/(k1​+⋯+kn​), which is also the value of (4);
  6. for positively homogeneous vvv, Dv(tτN)=Dv(τN)Dv(t\tau^N)=Dv(\tau^N)Dv(tτN)=Dv(τN), so ψnv=Dv(τN)\psi_nv=Dv(\tau^N)ψn​v=Dv(τN);
  7. (Remark 8.2) ψn\psi_nψn​ applied to Owen's multilinear extension of a game with side payments is its Shapley value.

Significance

The result. Theorem 8.1 singles out the diagonal formula among all ways of valuing smooth fuzzy games, using only efficiency, anonymity and invariance under merging players into types. Property (5) shows that the value transforms correctly under every linear change of coordinates fixing the grand coalition. The core statement links the value to stability: for concave homogeneous games (for instance, market games), the value is the only allocation no fuzzy coalition can improve upon. Through Owen's extension, the classical Shapley value is recovered as a special case.

Formalizing it. The theorem is proved in the paper, briefly, and its proof leans on an unproved density claim and on a short appeal to atomicity. A formalization makes the uniqueness argument complete: in particular, how atomicity, which only allows nonempty types, determines the value of a monomial in which some player has exponent 000. No machine-checked version of the Aumann–Shapley diagonal formula or its axiomatisation is known to us. Mathlib has the Stone–Weierstrass theorem for continuous functions but no C1C^1C1 density of polynomials on a cube; the latter is reusable well beyond game theory.

Difficulty

Existence (milestones 1–2) is calculus: differentiation under the integral sign and the chain rule. The difficulty sits in uniqueness. The first idea, computing ψn\psi_nψn​ on monomials by symmetry alone, fails as soon as the exponents differ: symmetry relates only games that are permutations of each other. Atomicity relates games with different numbers of players, and its types must be nonempty, so a player with exponent 000 cannot simply be merged away. Uniqueness on all of VnV^nVn then needs density of polynomials in the C1C^1C1 norm, not merely the uniform norm: without continuity in the C1C^1C1 norm, linear maps that agree on polynomials can disagree elsewhere, and the theorem is false.

Formalization scope

  • Players are Fin n, fuzzy coalitions and payoff vectors are Fin n → ℝ, and the cube is Set.Icc 0 1 in the product order.
  • VnV^nVn is a submodule of functions on all of Rn\mathbb R^nRn that are C1C^1C1 there and vanish at 000. Every C1C^1C1 function on the cube extends to such a function, and only values and derivatives on the cube enter the norm and the axioms. The global domain makes v∘Av\circ Av∘A meaningful for every linear AAA.
  • "Continuous" means ∥ψnv∥≤C ∥v∥C1\|\psi_nv\|\le C\,\|v\|_{C^1}∥ψn​v∥≤C∥v∥C1​ with the C1C^1C1 seminorm of the cube (sup norm on Rn\mathbb R^nRn, operator norm on DvDvDv). This is the continuity of the Banach space VnV^nVn. Continuity for the uniform norm alone would make formula (4) discontinuous, and dropping continuity would make uniqueness false.
  • The axioms are stated for all n≥1n\ge1n≥1; the paper's "∀n∈N\forall n\in N∀n∈N" in the symmetry axiom is read as n≥1n\ge1n≥1. In the atomicity axiom (3), the paper's "∀v∈Vm\forall v\in V^m∀v∈Vm" is read as v∈Vnv\in V^nv∈Vn, because P∗vP^*vP∗v is defined by (2) for an nnn-player game. A partition into nonempty types is a surjection Fin n → Fin m. The symbols τθ−1(i)\tau_{\theta-1(i)}τθ−1(i)​ are τθ−1(i)\tau_{\theta^{-1}(i)}τθ−1(i)​.
  • The games θ∗v\theta^*vθ∗v, P∗vP^*vP∗v and v∘Av\circ Av∘A are passed as elements of VnV^nVn, VmV^mVm together with their defining identities; they always lie in those spaces.
  • In the core statement, concavity and positive homogeneity (v(tτ)=tv(τ)v(t\tau)=tv(\tau)v(tτ)=tv(τ) for t>0t>0t>0, τ≥0\tau\ge0τ≥0) are required on the orthant R+n\mathbb R^n_+R+n​, to which §2 (2) extends vvv; the core quantifies over the cube, as in §2 (4)(a). The paper's "VNV^NVN" there is VnV^nVn.
  • Remark 8.2 is stated for games defined on all coalitions with v(∅)=0v(\emptyset)=0v(∅)=0, since formula (7) uses v(A∖{i})v(A\setminus\{i\})v(A∖{i}) for every AAA. The Shapley value is the published platform definition Supermodularity.Cooperative.ShapleyValue, whose formula is (7) re-indexed by S=A∖{i}S=A\setminus\{i\}S=A∖{i}. The Cornet extension of the same remark is left out because it is not C1C^1C1 on the boundary of the cube.
  • A trivializing reading is ruled out: the goal asserts both existence of a sequence satisfying all axioms with C1C^1C1 continuity and uniqueness among all such sequences, so neither an empty axiom system nor a vacuous continuity requirement makes it hold.

Infrastructure that a complete development needs, and that is welcome as separate contributions: C1C^1C1 approximation of functions on a cube by polynomials; differentiation under the integral sign for the diagonal integral; Euler's identity and the supergradient inequality for concave homogeneous C1C^1C1 functions.

Selected references

  • J.-P. Aubin, Cooperative Fuzzy Games, Mathematics of Operations Research 6(1) (1981) 1–13. https://doi.org/10.1287/moor.6.1.1
  • R. J. Aumann and L. S. Shapley, Values of Non-Atomic Games, Princeton University Press, 1974. https://doi.org/10.1515/9781400867080
  • L. S. Shapley, A Value for n-Person Games, in Contributions to the Theory of Games II, Annals of Mathematics Studies 28 (1953) 307–317. https://doi.org/10.1515/9781400881970-018
  • G. Owen, Multilinear Extensions of Games, Management Science 18(5) (1972) P64–P79. https://doi.org/10.1287/mnsc.18.5.64
  • L. J. Billera, D. C. Heath and J. Raanan, Internal Telephone Billing Rates — A Novel Application of Non-Atomic Game Theory, Operations Research 26(6) (1978) 956–965. https://doi.org/10.1287/opre.26.6.956
  • L. J. Mirman and Y. Tauman, Demand Compatible Equitable Cost Sharing Prices, Mathematics of Operations Research 7(1) (1982) 40–56. https://doi.org/10.1287/moor.7.1.40
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Numerical AnalysisOptimization·Captain: mikedeng1

Convergence Properties of the Nelder–Mead Simplex Method in Low Dimensions III: In Dimension 2, the Standard Method's Vertex Values Share One Limit and Simplex Diameters Tend to ZeroResearch Paper

Motivation

The Nelder–Mead simplex method (Nelder and Mead, 1965) minimizes a function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R using function values only. It is among the most widely used derivative-free methods in practice, built into standard numerical libraries, and for decades it had essentially no convergence theory. Lagarias, Reeds, Wright and Wright (1998) gave the first systematic analysis of the method with fully specified tie-breaking rules. Their results are limited to low dimensions, and the limits are genuine: McKinnon (1998) constructed strictly convex functions on R2\mathbb R^2R2 with continuous derivatives on which the method converges to a point that is not the minimizer.

This mission formalizes the paper's two-dimensional analysis (§5) together with the general-dimension facts of §3 on which it rests. A companion series of missions treats the one-dimensional results of §4.

Setting

Fix coefficients of reflection ρ\rhoρ, expansion χ\chiχ, contraction γ\gammaγ and shrinkage σ\sigmaσ with

ρ>0,χ>1,χ>ρ,0<γ<1,0<σ<1(2.1).\rho>0,\quad \chi>1,\quad \chi>\rho,\quad 0<\gamma<1,\quad 0<\sigma<1\qquad(2.1).ρ>0,χ>1,χ>ρ,0<γ<1,0<σ<1(2.1).

A simplex in Rn\mathbb R^nRn is a list of n+1n+1n+1 vertices x1,…,xn+1x_1,\dots,x_{n+1}x1​,…,xn+1​, ordered so that f(x1)≤⋯≤f(xn+1)f(x_1)\le\dots\le f(x_{n+1})f(x1​)≤⋯≤f(xn+1​); x1x_1x1​ is the best, xnx_nxn​ the next-worst and xn+1x_{n+1}xn+1​ the worst vertex, and fi=f(xi)f_i=f(x_i)fi​=f(xi​). With xˉ=1n∑i≤nxi\bar x=\frac1n\sum_{i\le n}x_ixˉ=n1​∑i≤n​xi​, the trial points are z(τ)=(1+τ)xˉ−τxn+1z(\tau)=(1+\tau)\bar x-\tau x_{n+1}z(τ)=(1+τ)xˉ−τxn+1​; reflection, expansion, outside and inside contraction use τ=ρ, ρχ, ργ, −γ\tau=\rho,\ \rho\chi,\ \rho\gamma,\ -\gammaτ=ρ, ρχ, ργ, −γ.

One iteration of Algorithm NM computes fr=f(z(ρ))f_r=f(z(\rho))fr​=f(z(ρ)) and then: accepts xrx_rxr​ if f1≤fr<fnf_1\le f_r<f_nf1​≤fr​<fn​; if fr<f1f_r<f_1fr​<f1​, accepts the better of xe=z(ρχ)x_e=z(\rho\chi)xe​=z(ρχ) and xrx_rxr​ (the expansion point only if fe<frf_e<f_rfe​<fr​); if fn≤fr<fn+1f_n\le f_r<f_{n+1}fn​≤fr​<fn+1​, accepts xc=z(ργ)x_c=z(\rho\gamma)xc​=z(ργ) if fc≤frf_c\le f_rfc​≤fr​; if fr≥fn+1f_r\ge f_{n+1}fr​≥fn+1​, accepts xcc=z(−γ)x_{cc}=z(-\gamma)xcc​=z(−γ) if fcc<fn+1f_{cc}<f_{n+1}fcc​<fn+1​. If no point is accepted, it shrinks: every vertex xix_ixi​ is replaced by x1+σ(xi−x1)x_1+\sigma(x_i-x_1)x1​+σ(xi​−x1​). An accepted point replaces xn+1x_{n+1}xn+1​ and is inserted after every remaining vertex with value ≤\le≤ its own; after a shrink, the new vertices are reordered, with x1x_1x1​ kept first if no new vertex beats it. A run is a sequence Δ0,Δ1,…\Delta_0,\Delta_1,\dotsΔ0​,Δ1​,… of simplices produced by successive iterations.

The edge matrix of a simplex is M=(x1−xn+1 ⋯ xn−xn+1)M=(x_1-x_{n+1}\ \cdots\ x_n-x_{n+1})M=(x1​−xn+1​ ⋯ xn​−xn+1​), the simplex is nondegenerate if det⁡M≠0\det M\ne0detM=0, its volume is vol⁡(Δ)=∣det⁡M∣/n!\operatorname{vol}(\Delta)=|\det M|/n!vol(Δ)=∣detM∣/n!, and its diameter is diam⁡(Δ)=max⁡i≠j∥xi−xj∥\operatorname{diam}(\Delta)=\max_{i\neq j}\|x_i-x_j\|diam(Δ)=maxi=j​∥xi​−xj​∥. A function has bounded level sets if every {x:f(x)≤μ}\{x:f(x)\le\mu\}{x:f(x)≤μ} is bounded. The standard method has ρ=1\rho=1ρ=1, χ=2\chi=2χ=2, γ=12\gamma=\tfrac12γ=21​.

Formalization targets

Goal: Theorem 5.2 (p. 144)

For fff strictly convex on R2\mathbb R^2R2 with bounded level sets and the standard coefficients, from any nondegenerate initial triangle,

lim⁡k→∞diam⁡(Δk)=0.\lim_{k\to\infty}\operatorname{diam}(\Delta_k)=0.k→∞lim​diam(Δk​)=0.

The theorem does not claim that the triangles converge to a point, and the formalization does not claim it either.

Milestones

  • General nnn (§3). Lemma 3.3 (monotonicity of vertex values, existence and ordering of the limits fi∗f_i^*fi∗​); Lemma 3.4 (broken convergence: fj∗<fj+1∗f_j^*<f_{j+1}^*fj∗​<fj+1∗​ freezes the first jjj vertices); Corollary 3.1 (if the best vertex moves infinitely often, all fi∗f_i^*fi∗​ coincide); Lemma 3.5 (no shrink on a strictly convex fff); Lemma 3.6 (fn∗=fn+1∗f_n^*=f_{n+1}^*fn∗​=fn+1∗​ when ργ<1\rho\gamma<1ργ<1); Lemma 3.1 (vol⁡(Δk+1)=∣τ∣vol⁡(Δk)\operatorname{vol}(\Delta_{k+1})=|\tau|\operatorname{vol}(\Delta_k)vol(Δk+1​)=∣τ∣vol(Δk​) after a step of type τ\tauτ, σnvol⁡(Δk)\sigma^n\operatorname{vol}(\Delta_k)σnvol(Δk​) after a shrink).
  • Dimension 2 (§5). Lemma 5.1 (if the best vertex never moves, the triangles converge to it); Theorem 5.1 (f1∗=f2∗=f3∗f_1^*=f_2^*=f_3^*f1∗​=f2∗​=f3∗​ for ρ=1\rho=1ρ=1, γ=12\gamma=\tfrac12γ=21​); Lemma 5.2 (vol⁡(Δk)→0\operatorname{vol}(\Delta_k)\to0vol(Δk​)→0 for the standard method).

Significance

Theorem 5.1 and Theorem 5.2 are among the few positive convergence statements for the Nelder–Mead method beyond dimension one. They show that on strictly convex functions in the plane the standard method cannot stall with a triangle of positive size; together with McKinnon's examples they delimit what can be proved: the simplices collapse, but not necessarily at the minimizer. The general-dimension lemmas of §3 (volume change, impossibility of shrinks on strictly convex functions, broken convergence) are used throughout the later literature on the method and its variants.

The results are proved on paper; no machine-checked proof of them is known. The formalization adds a precise, executable-in-principle definition of Algorithm NM with the paper's tie-breaking rules, and checked versions of statements whose printed form has small errors (see Formalization scope). The definition layer is reusable for any later work on simplex-based direct search.

Difficulty

The §3 lemmas are elementary but require bookkeeping of orderings, ties and change indices across iterations. The two-dimensional results are not. When the best vertex is eventually fixed (Lemma 5.1), the obvious measure of progress, the distance of the other vertices to it, is not monotone: reflections and outside contractions can move a vertex away, and contractions alternate in sign. Volume is also not monotone, because expansions double it. Lemma 5.2 and Theorem 5.2 depend on the precise acceptance rules: they are not known to hold for the original 1965 rule, which may accept an expansion point worse than the reflection point.

Formalization scope

Points are EuclideanSpace ℝ (Fin n); a simplex is Fin (n+1) → E n with 0-based indices, so index 0 is x1x_1x1​, n-1 is xnx_nxn​ and Fin.last n is xn+1x_{n+1}xn+1​. Runs are a relation: the paper leaves the ordering after a shrink partly open ("whatever rule"), so every theorem quantifies over all runs satisfying the iteration relation from an ordered start. Every theorem assumes (2.1) and a nondegenerate start; §3 lemmas assume exactly what each states about fff (bounded below, strictly convex, or nothing), and every §5 item assumes strict convexity and bounded level sets. Limits fi∗f_i^*fi∗​ are asserted as existence of limits or taken as Tendsto hypotheses, never through a default-valued limit operator. Volume and diameter are a determinant and a finite maximum, never a supremum over an unbounded set.

Committed conventions and corrections:

  • The nonshrink ordering rule prints j=max⁡{ℓ∣f(v)<f(xℓ+1)}j=\max\{\ell\mid f(v)<f(x_{\ell+1})\}j=max{ℓ∣f(v)<f(xℓ+1​)}, which always yields the last position and contradicts the paper's own example on p. 118; it is encoded with min⁡\minmin (insertion after all vertices of value ≤f(v)\le f(v)≤f(v)).
  • Lemma 3.3 (3)(ii) is stated for iterations after the last shrink; as printed ("for all kkk") it fails when an earlier shrink raised vertex values.
  • Lemma 3.6 (2) is stated for n≥2n\ge2n≥2; for n=1n=1n=1 the next-worst vertex is the best vertex, which can stay fixed forever.
  • Theorem 5.1 and Lemma 5.1 name only ρ=1\rho=1ρ=1, γ=12\gamma=\tfrac12γ=21​ and are stated with χ\chiχ general under (2.1); throughout §5, σ∈(0,1)\sigma\in(0,1)σ∈(0,1) is general instead of 12\tfrac1221​. Shrinks never occur on strictly convex functions, so this is a harmless strengthening.

A run relation that no sequence satisfies would make every theorem vacuous; it is satisfiable from every ordered start, and the hypotheses of the goal are jointly satisfied by f=∥x∥2f=\|x\|^2f=∥x∥2 and a concrete triangle (checked in Lean, not part of the mission). Welcome contributions: proofs of the §3 lemmas, which are independent of each other except through Lemma 3.3, and the reusable facts behind them (volume of a simplex under the Nelder–Mead moves, strict convexity along trial lines).

Selected references

  • J. C. Lagarias, J. A. Reeds, M. H. Wright, P. E. Wright, Convergence properties of the Nelder–Mead simplex method in low dimensions, SIAM J. Optim. 9(1):112–147, 1998. https://doi.org/10.1137/S1052623496303470
  • J. A. Nelder, R. Mead, A simplex method for function minimization, Computer Journal 7(4):308–313, 1965. https://doi.org/10.1093/comjnl/7.4.308
  • K. I. M. McKinnon, Convergence of the Nelder–Mead simplex method to a nonstationary point, SIAM J. Optim. 9(1):148–158, 1998. https://doi.org/10.1137/S1052623496303482
  • V. Torczon, On the convergence of pattern search algorithms, SIAM J. Optim. 7(1):1–25, 1997. https://doi.org/10.1137/S1052623493250780
12 thms2 active usersReviewed
AnalysisOperations ResearchProbability+1·Captain: mikedeng1

Implicit Renewal Theory and Tails of Solutions of Random Equations 3: Rate of Approach — t^κP(R > t) Equals C₊ Minus a Contour Integral Plus O(t^{−β/2})Research Paper

Motivation

Random equations of the form R=LΨ(R)R \overset{\mathcal L}{=} \Psi(R)R=LΨ(R), with Ψ\PsiΨ a random function independent of RRR, describe the stationary laws of many stochastic recursions: perpetuities in insurance and finance, the stationary law of ARCH-type volatility models, random difference equations R=Q+MRR = Q + MRR=Q+MR, and the stationary workload of certain queueing and storage models. When Ψ(t)\Psi(t)Ψ(t) acts like multiplication by a random variable MMM for large ∣t∣|t|∣t∣, and E∣M∣κ=1\mathbf E|M|^\kappa = 1E∣M∣κ=1 for some κ>0\kappa > 0κ>0, the solution has power-law tails: P(R>t)∼C+t−κP(R > t) \sim C_+ t^{-\kappa}P(R>t)∼C+​t−κ. This is the implicit renewal theorem of Goldie (Ann. Appl. Probab. 1991, Theorem 2.3), which recovers and extends Kesten's 1973 theorem on random difference equations.

A tail asymptotic alone says nothing about how fast tκP(R>t)t^\kappa P(R > t)tκP(R>t) approaches C+C_+C+​. For tail estimation, for the accuracy of extreme-quantile approximations used in risk management, and for second-order regular variation, the rate matters. Section 3 of the same paper answers this: under an exponential moment condition slightly beyond the Cramér condition, the error has an explicit second-order term determined by the zeros of 1−η^1 - \hat\eta1−η^​, where η\etaη is a tilted law of log⁡M\log MlogM, plus a remainder O(t−β/2)O(t^{-\beta/2})O(t−β/2).

Timeline: Kesten (1973) proved power tails for random difference equations; Grincevičius (1975) developed an implicit-renewal approach; Stone (1966) decomposed exponentially decaying renewal measures into an absolutely continuous part with explicit asymptotics and a finite part; Ganelius (1962) proved the Tauberian remainder theorem used to unsmooth; Goldie (1991) combined these into the rate result formalized here.

Setting

Let (Ω,A,P)(\Omega, \mathcal A, P)(Ω,A,P) be a probability space carrying independent real random variables M≥0M \ge 0M≥0 and RRR. Fix κ>0\kappa > 0κ>0 with EMκ=1\mathbf E M^\kappa = 1EMκ=1 (the Cramér condition, (2.3)) and β>0\beta > 0β>0 with EMκ+β<∞\mathbf E M^{\kappa+\beta} < \inftyEMκ+β<∞ (3.3).

The tilted law of MMM is the probability measure η(dx)=eκxP(log⁡M∈dx)\eta(dx) = e^{\kappa x} P(\log M \in dx)η(dx)=eκxP(logM∈dx) on R\mathbb RR, computed on {M>0}\{M > 0\}{M>0}. Its transforms are η~(β)=∫eβtη(dt)\tilde\eta(\beta) = \int e^{\beta t}\eta(dt)η~​(β)=∫eβtη(dt) for real β\betaβ and η^(θ)=∫eiθtη(dt)\hat\eta(\theta) = \int e^{i\theta t}\eta(dt)η^​(θ)=∫eiθtη(dt) for complex θ\thetaθ; for a function fff, f^(θ)=∫eiθtf(t) dt\hat f(\theta) = \int e^{i\theta t} f(t)\,dtf^​(θ)=∫eiθtf(t)dt. Convolution powers are η(0)=δ0\eta^{(0)} = \delta_0η(0)=δ0​, η(n+1)=η(n)∗η\eta^{(n+1)} = \eta^{(n)} * \etaη(n+1)=η(n)∗η, and the renewal measure is ν=∑n≥0η(n)\nu = \sum_{n \ge 0}\eta^{(n)}ν=∑n≥0​η(n). A law is spread out when some convolution power has a nonzero absolutely continuous component; (3.4) asks this of the conditional law of log⁡M\log MlogM given M≠0M \ne 0M=0.

Set m=EMκlog⁡Mm = \mathbf E M^\kappa \log Mm=EMκlogM and

g1(t)=eκt(P(R>et)−P(MR>et)),C+=1m∫0∞(P(R>t)−P(MR>t))tκ−1 dt,g_1(t) = e^{\kappa t}\big(P(R > e^t) - P(MR > e^t)\big), \qquad C_+ = \frac1m\int_0^\infty \big(P(R > t) - P(MR > t)\big) t^{\kappa - 1}\,dt,g1​(t)=eκt(P(R>et)−P(MR>et)),C+​=m1​∫0∞​(P(R>t)−P(MR>t))tκ−1dt,

with g−1g_{-1}g−1​ and C−C_-C−​ defined the same way for the lower tail. The strip is D={θ:−β<ℑθ<0}D = \{\theta : -\beta < \Im\theta < 0\}D={θ:−β<ℑθ<0}, and C\mathscr CC denotes a positively oriented closed contour in DDD enclosing every zero of 1−η^1 - \hat\eta1−η^​ in DDD.

Formalization targets

Goal: Theorem 3.2

If, in addition, η(n0)=(1−δ)φ0+δφ1\eta^{(n_0)} = (1 - \delta)\varphi_0 + \delta\varphi_1η(n0​)=(1−δ)φ0​+δφ1​ for some n0n_0n0​, with δ∈[0,1)\delta \in [0, 1)δ∈[0,1), φ0\varphi_0φ0​ absolutely continuous and δφ~1(β)<1\delta\tilde\varphi_1(\beta) < 1δφ~​1​(β)<1, and η^≠1\hat\eta \ne 1η^​=1 on ℑθ=−β\Im\theta = -\betaℑθ=−β, then ∫0∞∣P(R>t)−P(MR>t)∣ tκ+β−1dt<∞\int_0^\infty |P(R > t) - P(MR > t)|\,t^{\kappa+\beta-1}dt < \infty∫0∞​∣P(R>t)−P(MR>t)∣tκ+β−1dt<∞ implies

tκP(R>t)=C+−12π ℜ∮Ce−iθlog⁡t g^1(θ)1−η^(θ) dθ+O(t−β/2),t→∞,t^\kappa P(R > t) = C_+ - \frac1{2\pi}\,\Re\oint_{\mathscr C} e^{-i\theta\log t}\,\frac{\hat g_1(\theta)}{1 - \hat\eta(\theta)}\,d\theta + O(t^{-\beta/2}), \qquad t \to \infty,tκP(R>t)=C+​−2π1​ℜ∮C​e−iθlogt1−η^​(θ)g^​1​(θ)​dθ+O(t−β/2),t→∞,

with the analogous statement for P(R<−t)P(R < -t)P(R<−t); and if R=LΨ(R)R \overset{\mathcal L}{=} \Psi(R)R=LΨ(R) with RRR independent of (M,Ψ)(M, \Psi)(M,Ψ), the integrability hypotheses may be replaced by E∣(Ψ(R)±)κ+β−((MR)±)κ+β∣<∞\mathbf E|(\Psi(R)^\pm)^{\kappa+\beta} - ((MR)^\pm)^{\kappa+\beta}| < \inftyE∣(Ψ(R)±)κ+β−((MR)±)κ+β∣<∞. The theorem also asserts that η\etaη is a spread-out probability measure.

Milestones

  1. Lemma 9.5: Stone's inversion formula for the density of ∑nχ∗μ(n)\sum_n \chi * \mu^{(n)}∑n​χ∗μ(n).
  2. Theorem 3.1: the renewal measure splits as ν=ν0+ν1\nu = \nu_0 + \nu_1ν=ν0​+ν1​, ν1\nu_1ν1​ finite with ν~1(β)<∞\tilde\nu_1(\beta) < \inftyν~1​(β)<∞, ν0\nu_0ν0​ with continuous bounded density
p(t)=1m−12π∮Ce−iθtdθ1−η^(θ)+o(e−βt).p(t) = \frac1m - \frac1{2\pi}\oint_{\mathscr C} e^{-i\theta t}\frac{d\theta}{1 - \hat\eta(\theta)} + o(e^{-\beta t}).p(t)=m1​−2π1​∮C​e−iθt1−η^​(θ)dθ​+o(e−βt).
  1. (9.23) and (9.24): the smoothed identity and the smoothed rate K∗ℜr1(t)=o(e−βt)K * \Re r_1(t) = o(e^{-\beta t})K∗ℜr1​(t)=o(e−βt) for the kernel K(t)=be−bt1t>0K(t) = be^{-bt}\mathbf 1_{t>0}K(t)=be−bt1t>0​.
  2. Theorem 9.6: the Beurling–Ganelius Tauberian remainder theorem.

Significance

Theorem 3.2 turns the first-order tail asymptotic of the implicit renewal theorem into an expansion: the second-order terms are finitely many terms of the form (log⁡t)j−1tℑθl(\log t)^{j-1}t^{\Im\theta_l}(logt)j−1tℑθl​ times oscillating factors, one family for each zero θl\theta_lθl​ of 1−η^1 - \hat\eta1−η^​ with 0<−ℑθl≤β/20 < -\Im\theta_l \le \beta/20<−ℑθl​≤β/2, and their form does not depend on the unknown law of RRR. It applies to every random equation covered by the implicit renewal theorem once the stronger moment condition holds, including perpetuities and the random difference equation. Theorem 3.1 is of independent use: it is an explicit-rate version of Stone's decomposition of renewal measures with exponential moments.

The results are proved in the paper; none is formalized. Mathlib has the Fourier transform on the real line, convolution of measures, and rectangle Cauchy theorems, but no renewal theory, no Stone decomposition, and no Tauberian remainder theorem. Formalizing the mission produces a machine-checked renewal density expansion and a checked Beurling–Ganelius theorem, both reusable outside this paper.

Difficulty

The first-order theorem follows from the key renewal theorem applied to r(t)=eκtP(R>et)r(t) = e^{\kappa t}P(R > e^t)r(t)=eκtP(R>et). That route gives no rate: the key renewal theorem has no remainder, and the integrability hypothesis yields eβtg1∈L1e^{\beta t}g_1 \in L^1eβtg1​∈L1 but not eβtg1(t)=o(1)e^{\beta t}g_1(t) = o(1)eβtg1​(t)=o(1), so a remainder cannot be read off directly even with a spread-out step law. The proof therefore works with a smoothed version of rrr, where Stone's decomposition with the contour expansion of the renewal density gives an o(e−βt)o(e^{-\beta t})o(e−βt) remainder, and has to unsmooth. Unsmoothing is the Tauberian step: it requires a one-sided regularity condition on the unsmoothed function, verified for rrr and for the contour term, and costs half the exponent. The contour expansion itself requires showing that 1−η^1 - \hat\eta1−η^​ has finitely many zeros in the strip and handling their orders through residues.

Formalization scope

All objects live in the namespace GoldieRenewal.Rates. Random variables are measurable maps Ω→R\Omega \to \mathbb RΩ→R on a probability space; M≥0M \ge 0M≥0 almost surely; independence is IndepFun. Tail probabilities are real numbers P.real {ω | t < R ω}. Moments such as EMκ+β\mathbf E M^{\kappa+\beta}EMκ+β and μ~(β)\tilde\mu(\beta)μ~​(β) are lower Lebesgue integrals in [0,∞][0, \infty][0,∞]. The transforms μ^\hat\muμ^​ and f^\hat ff^​ are Bochner integrals at complex arguments with the +i+i+i sign of the paper. Asymptotic statements use Asymptotics.IsBigO and IsLittleO along atTop.

The contour. A contour C\mathscr CC is the positively oriented boundary of an axis-parallel rectangle whose closure lies in DDD and whose interior contains every zero of 1−η^1 - \hat\eta1−η^​ in DDD; the contour integral is the sum of the four edge integrals (RectangleIntegral, from the published ResidueCalcOnRectangles_defs). Expansions are stated for every such rectangle.

The variable in (3.8) and (3.10). The paper prints e−iθte^{-i\theta t}e−iθt in the contour term, but its proof establishes the expansion in the logarithmic variable s=log⁡ts = \log ts=logt. The targets are stated with e−iθlog⁡te^{-i\theta\log t}e−iθlogt, which is what the proof gives. With the printed e−iθte^{-i\theta t}e−iθt the contour term would decay exponentially and the statement would claim tκP(R>t)=C++O(t−β/2)t^\kappa P(R > t) = C_+ + O(t^{-\beta/2})tκP(R>t)=C+​+O(t−β/2), which is not what is proved. Hypothesis (3.7) is printed with P(R>−t)P(R > -t)P(R>−t) and is read with P(R>t)P(R > t)P(R>t).

Excluded trivializations. The contour term may not be dropped; the hypotheses do not exclude zeros of 1−η^1 - \hat\eta1−η^​ in DDD; and the contour must enclose all zeros in the strip, not a chosen subset.

Theorem 9.6 is stated for a complex-valued kernel and a finite strip width aaa; the application with a=∞a = \inftya=∞ follows by restricting to a finite strip. Lemma 9.5 carries an added hypothesis that the density of χ\chiχ has compact support, which the proof uses and the application provides.

Contributions welcome: renewal-measure infrastructure (convolution powers, Blackwell-type limits), Fourier analysis of measures at complex arguments, residue computations on rectangles, and Tauberian remainder theory. Each is reusable well beyond this paper.

Selected references

  • C. M. Goldie, Implicit renewal theory and tails of solutions of random equations, Ann. Appl. Probab. 1(1):126–166, 1991. https://doi.org/10.1214/aoap/1177005985
  • H. Kesten, Random difference equations and renewal theory for products of random matrices, Acta Math. 131:207–248, 1973. https://doi.org/10.1007/BF02392040
  • C. Stone, On absolutely continuous components and renewal theory, Ann. Math. Statist. 37(1):271–275, 1966. https://doi.org/10.1214/aoms/1177699617
  • T. H. Ganelius, The remainder in Wiener's Tauberian theorem, Acta Univ. Gothoburgensis, Mathematica Gothoburgensia 1, 1962 (cited in Goldie 1991).
  • A. K. Grincevičius, One limit distribution for a random walk on the line, Lithuanian Math. J. 15:580–589, 1975 (cited in Goldie 1991).
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Control TheoryProbabilityStochastic Systems·Captain: mikedeng1

Backward-Forward Stochastic Differential Equations 3: A Linear Backward-Forward System with Lipschitz Constant 1 Has No Solution on a Horizon T ≥ 1Research Paper

Motivation

A forward equation evolves from an initial random value, while a backward equation is constrained by a terminal random value. When the two unknown processes appear in both equations, these boundary conditions can be incompatible. Such coupled systems occur in stochastic control, where a state moves forward and a cost or adjoint variable is determined backward. Antonelli's 1993 paper studies existence and uniqueness for a class of backward–forward stochastic differential equations and gives explicit examples showing why its smallness assumption on the coefficients cannot be discarded (Antonelli 1993, §§1 and 3).

This mission formalizes the first of those examples. It is a deliberately small two-equation system: both integrators are ordinary time, the coefficients are deterministic, and the Lipschitz constant is one. Nevertheless, the system has no solution when the time horizon reaches one. The claim identifies a genuine boundary for the paper's existence result rather than a failure caused by exotic stochastic integration. Antonelli presents it immediately after the existence theorem to show what can go wrong beyond the theorem's coefficient bound (Antonelli 1993, Theorem 3.1 and Example 1).

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) and a filtration (Ft)t≥0(\mathcal F_t)_{t\ge0}(Ft​)t≥0​. The filtration satisfies the usual hypotheses: it is right-continuous, and F0\mathcal F_0F0​ contains every subset of every PPP-null set. Let T>0T>0T>0 be a deterministic horizon. The initial random variable J0J_0J0​ is F0\mathcal F_0F0​-measurable, and the terminal random variable YYY is FT\mathcal F_TFT​-measurable. Both are integrable and strictly positive almost surely. These choices specialize the filtered space and input assumptions of §3 to Example 1 (Antonelli 1993, pp. 777, 785, 790).

The unknowns are two real-valued stochastic processes U=(Ut)U=(U_t)U=(Ut​) and V=(Vt)V=(V_t)V=(Vt​). Their norm is

∥X∥L1(dt⊗P)=EP ⁣[∫0T∣Xt∣ dt].\|X\|_{L^1(dt\otimes P)}=E_P\!\left[\int_0^T |X_t|\,dt\right].∥X∥L1(dt⊗P)​=EP​[∫0T​∣Xt​∣dt].

Thus a solution is a pair in L1(dt⊗P)2L^1(dt\otimes P)^2L1(dt⊗P)2 of adapted processes satisfying a forward integral equation and a backward conditional-expectation equation almost surely at each time t≤Tt\le Tt≤T. Under the usual hypotheses every L1L^1L1-class solution has such a representative, so this is the paper's L1(μ)⊗L1(μ)L^1(\mu)\otimes L^1(\mu)L1(μ)⊗L1(μ) solution class. The system uses At=Ct=tA_t=C_t=tAt​=Ct​=t and the constant input process Jt=J0J_t=J_0Jt​=J0​. In this specialization, the measure μ\muμ used in the paper is dt⊗Pdt\otimes Pdt⊗P, and the variation control process is Dt=tD_t=tDt​=t (Antonelli 1993, (3.1)–(3.3), pp. 785–786).

The forward coefficient is f(u,v)=u+∣v∣f(u,v)=u+|v|f(u,v)=u+∣v∣ and the backward coefficient is g(u,v)=u+vg(u,v)=u+vg(u,v)=u+v. Each has Lipschitz constant one with respect to ∣u−u′∣+∣v−v′∣|u-u'|+|v-v'|∣u−u′∣+∣v−v′∣. The absolute value is part of the example: it appears in the forward equation and does not appear in the backward equation (Antonelli 1993, (3.6)–(3.7), p. 790).

Formalization targets

Main goal

For every horizon T≥1T\ge1T≥1 and all data satisfying the assumptions above, there is no pair (U,V)∈L1(dt⊗P)2(U,V)\in L^1(dt\otimes P)^2(U,V)∈L1(dt⊗P)2 satisfying

Ut=J0+∫0t(Us+∣Vs∣) ds,Vt=EP ⁣[∫tT(Us+Vs) ds+Y∣Ft].U_t=J_0+\int_0^t(U_s+|V_s|)\,ds,\qquad V_t=E_P\!\left[\int_t^T(U_s+V_s)\,ds+Y\mid\mathcal F_t\right].Ut​=J0​+∫0t​(Us​+∣Vs​∣)ds,Vt​=EP​[∫tT​(Us​+Vs​)ds+Y∣Ft​].

This is Example 1's conclusion, including the boundary case T=1T=1T=1 (Antonelli 1993, pp. 790–791).

Intermediate targets

The milestones follow the four statements written in the example: representations of UUU and VVV in terms of each other, positivity and passage to the linear system (3.8)–(3.9), the martingale identity for their sum, and the identity β(1−T)=EP[J0+Y]>0\beta(1-T)=E_P[J_0+Y]>0β(1−T)=EP​[J0​+Y]>0 for its constant mean β\betaβ. Their full text and page provenance are attached to the milestone list. The goal remains nonexistence for every T≥1T\ge1T≥1; it does not assert a particular formula for a solution.

Significance

The preceding existence theorem assumes a coefficient bound that becomes kT<1kT<1kT<1 in this time-integrator case. Example 1 has k=1k=1k=1 and shows that the system can fail to have a solution as soon as that strict inequality fails. At T=1T=1T=1, the obstruction is already present, so replacing T≥1T\ge1T≥1 by T>1T>1T>1 would lose part of the paper's conclusion (Antonelli 1993, p. 791).

A formalization would make the failure precise for the same L1L^1L1 solution class used by the paper. The current mission contains compile-checked Lean statements and definitions; the theorem proofs are still open. A complete development would also provide reusable statements about jointly measurable conditional-expectation versions, finite-horizon time integrals of processes, and martingales arising from coupled equations. These can support the paper's neighboring existence and nonsingular-example missions.

Difficulty

The main difficulty is the coupling between the two boundary conditions. The forward equation starts at J0J_0J0​, while the backward equation ends at YYY; neither equation can be treated as an independent ordinary differential equation. The absolute value in the forward coefficient also prevents the coupled system from being treated as a linear system at the outset. A second difficulty for Lean is that conditional expectation is defined only up to almost-sure equality at each fixed time, whereas the solution equations are equalities over time and probability together. The formal statement must connect these two kinds of almost-everywhere equality without strengthening the theorem to an identity at every time on every sample path.

Formalization scope

Time is represented by R≥0\mathbb R_{\ge0}R≥0​, with only (0,T](0,T](0,T] used in the L1L^1L1 norm. Time integration is Lebesgue integration on (s,t](s,t](s,t]; endpoints have zero dtdtdt mass. The norm is an extended nonnegative lintegral, so a nonintegrable process cannot be assigned the value zero by a real-valued integral's fallback convention. The random variable inside each conditional expectation is required to be integrable. The conditional-expectation process is a jointly measurable version whose value at each time agrees almost surely with the conditional expectation. The solution predicate asks, for each t≤Tt\le Tt≤T, that UtU_tUt​ and VtV_tVt​ be Ft\mathcal F_tFt​-measurable, that the two equations hold PPP-almost surely, and that the time integrands be integrable along almost every path. Any L1L^1L1-class solution can be replaced by such a representative, J0+∫0tf(Us,Vs) dsJ_0+\int_0^t f(U_s,V_s)\,dsJ0​+∫0t​f(Us​,Vs​)ds and the conditional-expectation version, so non-existence in this class is non-existence in the paper's class. For the Lipschitz coefficients in this example, finite L1(dt⊗P)L^1(dt\otimes P)L1(dt⊗P) norm gives pathwise integrability almost surely for the time integrals used in the equations.

The paper calls J0J_0J0​ and YYY “positive.” Here that means strictly positive almost surely. The weaker nonnegative reading would admit the zero pair when both data are zero and would falsify the target. Integrability of J0J_0J0​ makes explicit §3's standing bound on the constant input process. The completeness and right-continuity of the filtration are also explicit. The solution class and equations are defined for general T>0T>0T>0; the restriction T≥1T\ge1T≥1 belongs only to the nonexistence theorem. For example, on a one-point probability space with T=1/2T=1/2T=1/2, J0=Y=1J_0=Y=1J0​=Y=1, the deterministic pair Ut=1+4tU_t=1+4tUt​=1+4t, Vt=3−4tV_t=3-4tVt​=3−4t solves the equations on [0,1/2][0,1/2][0,1/2]. This rules out a definition that makes all solutions impossible by construction.

The development needs Mathlib's filtration, conditional expectation, probability measure, and integration APIs. Contributions proving the milestone statements or supplying reusable lemmas for their L1L^1L1 and martingale interfaces fit the mission. No semimartingale stochastic integral is required for this example.

Selected references

  • F. Antonelli, Backward-forward stochastic differential equations, Annals of Applied Probability 3(3), 777–793, 1993. DOI: 10.1214/aoap/1177005363.
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Control TheoryOperations ResearchProbability+1·Captain: mikedeng1

Reflected Solutions of Backward SDE's, and Related Obstacle Problems for PDE's 2: With a Concave Coefficient, the Reflected BSDE Is the Value of a Minimax Optimal Stopping–Control ProblemResearch Paper

Motivation

A backward stochastic differential equation (BSDE) prescribes the terminal value of an adapted process instead of its initial value. Pardoux and Peng (1990) proved existence and uniqueness for Lipschitz coefficients, and BSDEs have since become a standard tool in stochastic control, mathematical finance and the probabilistic treatment of semilinear PDEs. El Karoui, Kapoudjian, Pardoux, Peng and Quenez (1997) introduced the reflected BSDE, whose solution is constrained to stay above a given obstacle process. Reflected BSDEs describe the price of American options in nonlinear markets (El Karoui, Pardoux and Quenez 1997), Dynkin games (Cvitanić and Karatzas 1996), and obstacle problems for parabolic PDEs.

In §7 of the 1997 paper the coefficient is assumed concave. Then the solution of the reflected BSDE is the value of a game: one player chooses a stopping time, the other chooses a control that sets the discount rate and the change of measure, and the value does not depend on which player moves first. This mission formalizes that statement (Theorem 7.2) and the results its proof uses.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) carry a ddd-dimensional standard Brownian motion BBB, fix a horizon T≥0T\ge0T≥0, and let Ft\mathcal F_tFt​ be the natural filtration of BBB augmented by the PPP-null sets. Write L2\mathbb L^2L2 for the square-integrable FT\mathcal F_TFT​-measurable random variables, H2\mathbb H^2H2 for the progressively measurable processes φ\varphiφ with E∫0T∣φt∣2dt<∞E\int_0^T|\varphi_t|^2dt<\inftyE∫0T​∣φt​∣2dt<∞, and S2\mathcal S^2S2 for those with Esup⁡t≤T∣φt∣2<∞E\sup_{t\le T}|\varphi_t|^2<\inftyEsupt≤T​∣φt​∣2<∞.

The data are a terminal value ξ∈L2\xi\in\mathbb L^2ξ∈L2; a coefficient f(ω,t,y,z)f(\omega,t,y,z)f(ω,t,y,z), y∈Ry\in\mathbb Ry∈R, z∈Rdz\in\mathbb R^dz∈Rd, with f(⋅,y,z)∈H2f(\cdot,y,z)\in\mathbb H^2f(⋅,y,z)∈H2 for every (y,z)(y,z)(y,z) and Lipschitz in (y,z)(y,z)(y,z) with a constant KKK; and a continuous progressively measurable obstacle SSS with Esup⁡t(St+)2<∞E\sup_t(S_t^+)^2<\inftyEsupt​(St+​)2<∞ and ST≤ξS_T\le\xiST​≤ξ. A solution of the reflected BSDE is a triple (Y,Z,K)(Y,Z,K)(Y,Z,K) of progressively measurable processes with Z∈H2Z\in\mathbb H^2Z∈H2, Y∈S2Y\in\mathcal S^2Y∈S2, KT∈L2K_T\in\mathbb L^2KT​∈L2, and

Yt=ξ+∫tTf(s,Ys,Zs) ds+KT−Kt−∫tT(Zs,dBs),Yt≥St,Y_t=\xi+\int_t^Tf(s,Y_s,Z_s)\,ds+K_T-K_t-\int_t^T(Z_s,dB_s),\qquad Y_t\ge S_t,Yt​=ξ+∫tT​f(s,Ys​,Zs​)ds+KT​−Kt​−∫tT​(Zs​,dBs​),Yt​≥St​,

where KKK is continuous, nondecreasing, K0=0K_0=0K0​=0 and ∫0T(Yt−St) dKt=0\int_0^T(Y_t-S_t)\,dK_t=0∫0T​(Yt​−St​)dKt​=0: KKK pushes YYY up only when YYY touches SSS.

For t≤Tt\le Tt≤T, Tt\mathcal T_tTt​ is the set of stopping times vvv with t≤v≤Tt\le v\le Tt≤v≤T. When f(ω,t,⋅,⋅)f(\omega,t,\cdot,\cdot)f(ω,t,⋅,⋅) is concave, its conjugate is

F(ω,t,β,γ)=sup⁡(y,z)[f(ω,t,y,z)−βy−⟨γ,z⟩]∈(−∞,+∞].F(\omega,t,\beta,\gamma)=\sup_{(y,z)}\big[f(\omega,t,y,z)-\beta y-\langle\gamma,z\rangle\big]\in(-\infty,+\infty].F(ω,t,β,γ)=(y,z)sup​[f(ω,t,y,z)−βy−⟨γ,z⟩]∈(−∞,+∞].

The admissible controls A\mathcal AA are the bounded progressively measurable (βt,γt)(\beta_t,\gamma_t)(βt​,γt​) with E∫0TF(t,βt,γt)2dt<∞E\int_0^TF(t,\beta_t,\gamma_t)^2dt<\inftyE∫0T​F(t,βt​,γt​)2dt<∞. Each (β,γ)∈A(\beta,\gamma)\in\mathcal A(β,γ)∈A gives the affine coefficient fβ,γ(t,y,z)=F(t,βt,γt)+βty+⟨γt,z⟩f^{\beta,\gamma}(t,y,z)=F(t,\beta_t,\gamma_t)+\beta_ty+\langle\gamma_t,z\ranglefβ,γ(t,y,z)=F(t,βt​,γt​)+βt​y+⟨γt​,z⟩, its reflected BSDE solution Yβ,γY^{\beta,\gamma}Yβ,γ, the process Γt,sβ,γ\Gamma^{\beta,\gamma}_{t,s}Γt,sβ,γ​ solving dΓt,s=Γt,s(βsds+(γs,dBs))d\Gamma_{t,s}=\Gamma_{t,s}(\beta_sds+(\gamma_s,dB_s))dΓt,s​=Γt,s​(βs​ds+(γs​,dBs​)), Γt,t=1\Gamma_{t,t}=1Γt,t​=1, and the payoff

Φ(t,v,β,γ)=Γt,vβ,γ[Sv1{v<T}+ξ1{v=T}]+∫tvΓt,sβ,γF(s,βs,γs) ds.\Phi(t,v,\beta,\gamma)=\Gamma^{\beta,\gamma}_{t,v}\big[S_v1_{\{v<T\}}+\xi1_{\{v=T\}}\big]+\int_t^v\Gamma^{\beta,\gamma}_{t,s}F(s,\beta_s,\gamma_s)\,ds.Φ(t,v,β,γ)=Γt,vβ,γ​[Sv​1{v<T}​+ξ1{v=T}​]+∫tv​Γt,sβ,γ​F(s,βs​,γs​)ds.

Formalization targets

Goal: Theorem 7.2 (p. 725)

For every t∈[0,T]t\in[0,T]t∈[0,T] and (β,γ)∈A(\beta,\gamma)\in\mathcal A(β,γ)∈A, Ytβ,γ=ess sup⁡v∈TtE[Φ(t,v,β,γ)∣Ft]Y^{\beta,\gamma}_t=\operatorname{ess\,sup}_{v\in\mathcal T_t}E[\Phi(t,v,\beta,\gamma)\mid\mathcal F_t]Ytβ,γ​=esssupv∈Tt​​E[Φ(t,v,β,γ)∣Ft​], and

Yt=ess inf⁡AYtβ,γ=ess inf⁡Aess sup⁡v∈TtE[Φ∣Ft]=ess sup⁡v∈Ttess inf⁡AE[Φ∣Ft].Y_t=\operatorname*{ess\,inf}_{\mathcal A}Y^{\beta,\gamma}_t=\operatorname*{ess\,inf}_{\mathcal A}\operatorname*{ess\,sup}_{v\in\mathcal T_t}E[\Phi\mid\mathcal F_t]=\operatorname*{ess\,sup}_{v\in\mathcal T_t}\operatorname*{ess\,inf}_{\mathcal A}E[\Phi\mid\mathcal F_t].Yt​=Aessinf​Ytβ,γ​=Aessinf​v∈Tt​esssup​E[Φ∣Ft​]=v∈Tt​esssup​Aessinf​E[Φ∣Ft​].

The last equality, the interchange of the two essential extrema, is the minimax content.

Milestones

  1. Theorem 4.1 (p. 712): comparison. If ξ≤ξ′\xi\le\xi'ξ≤ξ′, f≤f′f\le f'f≤f′ and S≤S′S\le S'S≤S′, and one of f,f′f,f'f,f′ is Lipschitz, then Y≤Y′Y\le Y'Y≤Y′.
  2. §7 conjugacy (p. 724): a concave Lipschitz fff equals min⁡(β,γ)∈DtF{F(t,β,γ)+βy+⟨γ,z⟩}\min_{(\beta,\gamma)\in D^F_t}\{F(t,\beta,\gamma)+\beta y+\langle\gamma,z\rangle\}min(β,γ)∈DtF​​{F(t,β,γ)+βy+⟨γ,z⟩}, the minimum is attained, and the domain DtFD^F_tDtF​ of FFF is a.s. bounded.
  3. Proposition 7.1 (p. 724): for an affine coefficient δt+βty+⟨γt,z⟩\delta_t+\beta_ty+\langle\gamma_t,z\rangleδt​+βt​y+⟨γt​,z⟩, ΓtYt=ess sup⁡v∈TtE[Γvξ1{v=T}+ΓvSv1{v<T}+∫tvΓsδsds∣Ft]\Gamma_tY_t=\operatorname{ess\,sup}_{v\in\mathcal T_t}E[\Gamma_v\xi1_{\{v=T\}}+\Gamma_vS_v1_{\{v<T\}}+\int_t^v\Gamma_s\delta_sds\mid\mathcal F_t]Γt​Yt​=esssupv∈Tt​​E[Γv​ξ1{v=T}​+Γv​Sv​1{v<T}​+∫tv​Γs​δs​ds∣Ft​].
  4. §7 optimal control (p. 725): some (β∗,γ∗)∈A(\beta^*,\gamma^*)\in\mathcal A(β∗,γ∗)∈A satisfies f(t,Yt,Zt)=F(t,βt∗,γt∗)+βt∗Yt+⟨γt∗,Zt⟩f(t,Y_t,Z_t)=F(t,\beta^*_t,\gamma^*_t)+\beta^*_tY_t+\langle\gamma^*_t,Z_t\ranglef(t,Yt​,Zt​)=F(t,βt∗​,γt∗​)+βt∗​Yt​+⟨γt∗​,Zt​⟩ dt×dPdt\times dPdt×dP-a.e., so (Y,Z,K)(Y,Z,K)(Y,Z,K) solves the reflected BSDE with coefficient fβ∗,γ∗f^{\beta^*,\gamma^*}fβ∗,γ∗.

Significance

Theorem 7.2 identifies the solution of a nonlinear reflected BSDE with the value of a zero-sum game between a stopper and a controller. In finance, with fff the driver of a pricing rule under constraints or ambiguity, it says that the nonlinear price of an American claim is the worst case, over a family of discount rates and changes of measure, of linear American prices; and the stopper may announce the stopping rule first without changing the value. Concave drivers include the hedging equations with different borrowing and lending rates. The representation reduces questions about the nonlinear equation to a family of linear ones, which is how monotonicity, convexity and stability properties of nonlinear American prices are usually derived.

All four results and the goal are proved in the paper, with references to standard convex analysis and a measurable section theorem for two steps. None of them has a machine-checked proof. Mathlib has Brownian motion, filtrations, stopping times and conditional expectation, but no stochastic integral; the mission uses the Itô integral of the published Peng1990.SMP.Stochastic layer. A formal proof would give, beyond the theorem, a reusable comparison theorem for reflected BSDEs, a Snell-envelope representation for linear reflected BSDEs, and a measurable selection of supergradients along a process.

Difficulty

The inequality Yt≤Ytβ,γY_t\le Y^{\beta,\gamma}_tYt​≤Ytβ,γ​ for each control is a direct consequence of comparison, since f≤fβ,γf\le f^{\beta,\gamma}f≤fβ,γ. The difficulty is the reverse inequality, which needs a single admissible control that attains the conjugate representation along the solution (Y,Z)(Y,Z)(Y,Z) for almost every (t,ω)(t,\omega)(t,ω). Choosing a supergradient pointwise is easy; choosing it progressively measurable, bounded, and with F(t,βt∗,γt∗)F(t,\beta^*_t,\gamma^*_t)F(t,βt∗​,γt∗​) square integrable is a measurable-selection problem. The interchange of ess inf and ess sup does not follow from a general minimax theorem: the family A\mathcal AA is not compact and the payoff is not convex–concave in any usable topology. It uses a specific stopping time, the first time YYY touches SSS, together with comparison on the random interval before it. Proposition 7.1 requires the linear change of variables ΓtYt\Gamma_tY_tΓt​Yt​, whose transformed equation lacks the square integrability of the original one, so the Snell-envelope argument has to be rerun with weaker moments.

Formalization scope

  • Time and spaces. Time is R≥0\mathbb R_{\ge0}R≥0​ with T:R≥0T:\mathbb R_{\ge0}T:R≥0​, and time integrals run over [t,T]⊂R[t,T]\subset\mathbb R[t,T]⊂R. H2\mathbb H^2H2 is the published L2F (progressive in place of predictable); S2\mathcal S^2S2 and the obstacle condition are lower Lebesgue integrals in [0,∞][0,\infty][0,∞].
  • Filtration. The natural filtration of BBB joined with the σ-algebra of PPP-null sets.
  • Norms. ∣z∣|z|∣z∣ is the Euclidean norm and ⟨γ,z⟩=∑jγjzj\langle\gamma,z\rangle=\sum_j\gamma_jz_j⟨γ,z⟩=∑j​γj​zj​.
  • Lipschitz condition. Read as: almost surely, for all t≤Tt\le Tt≤T and all y,y′,z,z′y,y',z,z'y,y′,z,z′.
  • Solutions. Solutions are in the square-integrable class (v)–(viii). YYY has continuous paths. Equation (vi) holds for each ttt almost surely, and Y≥SY\ge SY≥S holds almost surely for all ttt. KKK is continuous and nondecreasing on every path. ∫0T(Y−S) dK=0\int_0^T(Y-S)\,dK=0∫0T​(Y−S)dK=0 is taken against the Lebesgue–Stieltjes measure of the path of KKK.
  • Extended values. FFF takes values in the extended reals. F2F^2F2 in the definition of A\mathcal AA is taken in [0,∞][0,\infty][0,∞], so admissibility forces F<∞F<\inftyF<∞ almost everywhere along the control.
  • Stochastic exponential. Γt,sβ,γ\Gamma^{\beta,\gamma}_{t,s}Γt,sβ,γ​ is the Doléans-Dade exponential, built from Itô integrals of γ\gammaγ with continuous paths.
  • Essential extrema. They are predicates relative to Ft\mathcal F_tFt​, real valued: the essential infimum is the published MultiperiodRisk.Bellman.EssInf, and the essential supremum is its mirror image.
  • Added hypothesis. S∈S2S\in\mathcal S^2S∈S2 is assumed wherever a conditional expectation of the payoff appears (Remark 3.2: without loss of generality). Otherwise the payoff may fail to be integrable, and Lean's conditional expectation of a non-integrable function is 000.
  • Hypothesized families. The solutions Yβ,γY^{\beta,\gamma}Yβ,γ and the Itô integrals defining Γβ,γ\Gamma^{\beta,\gamma}Γβ,γ are hypotheses indexed by A\mathcal AA. They exist by the existence theorem of the first mission of this series and by continuity of Itô integrals.

Several formalizations of the goal would make it trivial, and each is ruled out. The conjugate is not a real-valued supremum, which takes a junk value when unbounded. The essential infimum over A\mathcal AA is not a pointwise infimum. The interchange of ess inf and ess sup is not dropped. The coefficient is a random field f(ω,t,y,z)f(\omega,t,y,z)f(ω,t,y,z), not a deterministic or Markovian one.

The closing gloss of Theorem 7.2, that the triple (β∗,γ∗,Dt)(\beta^*,\gamma^*,D_t)(β∗,γ∗,Dt​) is optimal, is not stated separately; milestone 4 is its control half. Contributions are welcome on a continuous version of the Itô integral, Itô's formula for products with Γ\GammaΓ, the Snell envelope in continuous time, and measurable selection of supergradients; all of these are reusable beyond this mission.

Selected references

  • N. El Karoui, C. Kapoudjian, É. Pardoux, S. Peng, M.-C. Quenez, Reflected solutions of backward SDE's, and related obstacle problems for PDE's, Ann. Probab. 25(2), 1997, 702–737. https://doi.org/10.1214/aop/1024404416
  • É. Pardoux, S. Peng, Adapted solution of a backward stochastic differential equation, Systems Control Lett. 14, 1990, 55–61. https://doi.org/10.1016/0167-6911(90)90082-6
  • N. El Karoui, S. Peng, M.-C. Quenez, Backward stochastic differential equations in finance, Math. Finance 7(1), 1997, 1–71. https://doi.org/10.1111/1467-9965.00022
  • J. Cvitanić, I. Karatzas, Backward stochastic differential equations with reflection and Dynkin games, Ann. Probab. 24(4), 1996, 2024–2056. https://doi.org/10.1214/aop/1041903216
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28(4), 1990, 966–979. https://doi.org/10.1137/0328054
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Operations ResearchProbabilityStatistics·Captain: mikedeng1

Simulation Output Analysis Using Standardized Time Series 3: No g in 𝓜 Makes g(σB) Almost Surely Constant, So the Length Bound Is Not AttainedResearch Paper

Motivation

A steady-state simulation produces a single long output path Y={Y(t):t≥0}Y=\{Y(t):t\ge0\}Y={Y(t):t≥0}, and the quantity of interest is its long-run mean μ\muμ. The central difficulty of simulation output analysis is that the observations are correlated, so the classical confidence interval Yˉn(1)±z σ^/n\bar Y_n(1)\pm z\,\hat\sigma/\sqrt nYˉn​(1)±zσ^/n​ needs a consistent estimate of the time-average variance constant σ2\sigma^2σ2, which is hard to obtain. The method of standardized time series (STS), introduced by Schruben (1983) and put on a general footing by Glynn and Iglehart (Math. Oper. Res. 15 (1990)), avoids estimating σ\sigmaσ: it divides the centred sample mean by a functional ggg of the whole sample path that scales like σ\sigmaσ, so that σ\sigmaσ cancels in the limit. Batch means, the area estimator and other procedures used in simulation software are all instances of this construction.

Cancelling σ\sigmaσ has a price. Glynn and Iglehart show (their Corollary 4.16) that every STS interval has asymptotic expected length at least 2σΦ−1(1−δ/2)/n2\sigma\Phi^{-1}(1-\delta/2)/\sqrt n2σΦ−1(1−δ/2)/n​, the length of the interval that knows σ\sigmaσ, and (4.23) that this bound is the infimum over all admissible ggg. This mission formalizes the next question the paper asks and answers: is the infimum attained? Proposition 4.26 says it is not, and the companion results quantify the residual randomness of the interval length.

Setting

C[0,1]C[0,1]C[0,1] is the space of continuous real functions on [0,1][0,1][0,1] with the uniform metric ρ(x,y)=sup⁡t∣x(t)−y(t)∣\rho(x,y)=\sup_t|x(t)-y(t)|ρ(x,y)=supt​∣x(t)−y(t)∣ and its Borel σ\sigmaσ-algebra; k(t)=tk(t)=tk(t)=t, and C0[0,1]={x∈C[0,1]:x(0)=0}C_0[0,1]=\{x\in C[0,1]:x(0)=0\}C0​[0,1]={x∈C[0,1]:x(0)=0}. For g:C[0,1]→Rg:C[0,1]\to\mathbb Rg:C[0,1]→R, D(g)D(g)D(g) is the set of points at which ggg is not continuous. On a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P), BBB is a standard Brownian motion, viewed as a random element of C[0,1]C[0,1]C[0,1].

Assumption (2.1). There are finite constants μ\muμ and σ>0\sigma>0σ>0 such that Xn⇒σBX_n\Rightarrow\sigma BXn​⇒σB in C[0,1]C[0,1]C[0,1], where

Xn(t)=n1/2(Yˉn(t)−μt),Yˉn(t)=1n∫0ntY(s) ds,0≤t≤1.X_n(t)=n^{1/2}\big(\bar Y_n(t)-\mu t\big),\qquad \bar Y_n(t)=\frac1n\int_0^{nt}Y(s)\,ds,\quad 0\le t\le1 .Xn​(t)=n1/2(Yˉn​(t)−μt),Yˉn​(t)=n1​∫0nt​Y(s)ds,0≤t≤1.

The class M\mathcal MM (2.3) consists of the measurable g:C[0,1]→Rg:C[0,1]\to\mathbb Rg:C[0,1]→R with

  1. g(ax)=a g(x)g(ax)=a\,g(x)g(ax)=ag(x) for a>0a>0a>0;
  2. g(x−βk)=g(x)g(x-\beta k)=g(x)g(x−βk)=g(x) for β∈R\beta\in\mathbb Rβ∈R;
  3. P{g(B)>0}=1P\{g(B)>0\}=1P{g(B)>0}=1;
  4. P{B∈D(g)}=0P\{B\in D(g)\}=0P{B∈D(g)}=0.

With H(x)=P{B(1)/g(B)≤x}H(x)=P\{B(1)/g(B)\le x\}H(x)=P{B(1)/g(B)≤x} and α,β\alpha,\betaα,β chosen so that H(β)−H(α)=1−δH(\beta)-H(\alpha)=1-\deltaH(β)−H(α)=1−δ, the interval [Yˉn(1)−g(Yˉn)β, Yˉn(1)−g(Yˉn)α][\bar Y_n(1)-g(\bar Y_n)\beta,\ \bar Y_n(1)-g(\bar Y_n)\alpha][Yˉn​(1)−g(Yˉn​)β, Yˉn​(1)−g(Yˉn​)α] (2.10) is an asymptotic 100(1−δ)%100(1-\delta)\%100(1−δ)% confidence interval for μ\muμ, of width Ln=g(Yˉn)(β−α)L_n=g(\bar Y_n)(\beta-\alpha)Ln​=g(Yˉn​)(β−α).

Formalization targets

Goal: Proposition 4.26

For every σ>0\sigma>0σ>0 there is no g∈Mg\in\mathcal Mg∈M such that, for some α>0\alpha>0α>0,

P{g(σB)=ασ}=1.(4.25)P\{g(\sigma B)=\alpha\sigma\}=1. \qquad (4.25)P{g(σB)=ασ}=1.(4.25)

By the paper's discussion before (4.25), attaining the lower bound of Corollary 4.16 with some g∈Mg\in\mathcal Mg∈M requires (4.25); the goal therefore says that the bound is attained by no g∈Mg\in\mathcal Mg∈M. The goal is stated in terms of (4.25) and not of the limit (4.24), so it does not depend on the expected-length machinery of Corollary 4.16.

Milestones (the steps of the proof, pp. 13–14)

  1. For ∣z∣<η|z|<\eta∣z∣<η: P{∣B(t)−z∣<η, max⁡0≤s≤t∣B(s)∣<2η}>0P\{|B(t)-z|<\eta,\ \max_{0\le s\le t}|B(s)|<2\eta\}>0P{∣B(t)−z∣<η, max0≤s≤t​∣B(s)∣<2η}>0.
  2. (4.27): P{ρ(σB,x)<ε}>0P\{\rho(\sigma B,x)<\varepsilon\}>0P{ρ(σB,x)<ε}>0 for every x∈C0[0,1]x\in C_0[0,1]x∈C0​[0,1] and ε>0\varepsilon>0ε>0.
  3. If the range of ggg over every ε\varepsilonε-neighbourhood of xxx contains {ασ:σ>0}\{\alpha\sigma:\sigma>0\}{ασ:σ>0}, then x∈D(g)x\in D(g)x∈D(g).
  4. Under (2.3i) and (4.25), C0[0,1]⊆D(g)C_0[0,1]\subseteq D(g)C0​[0,1]⊆D(g).

Companions

  • g(B)g(B)g(B) is nondegenerate for every g∈Mg\in\mathcal Mg∈M (p. 14).
  • Proposition 4.32: if {g2(Xn)}\{g^2(X_n)\}{g2(Xn​)} is uniformly integrable, then
lim⁡n→∞nE(Ln−ELn)2=σ2E(g(B)−Eg(B))2(β−α)2>0.\lim_{n\to\infty}nE(L_n-EL_n)^2=\sigma^2E\big(g(B)-Eg(B)\big)^2(\beta-\alpha)^2>0 .n→∞lim​nE(Ln​−ELn​)2=σ2E(g(B)−Eg(B))2(β−α)2>0.

Significance

The result closes the expected-length analysis of STS intervals: the bound 2σΦ−1(1−δ/2)2\sigma\Phi^{-1}(1-\delta/2)2σΦ−1(1−δ/2) is the exact infimum over M\mathcal MM but no single standardization reaches it, so every STS procedure is strictly worse, in expected length, than the interval with known σ\sigmaσ. The companion results explain why: g(B)g(B)g(B) is never degenerate, so n1/2Lnn^{1/2}L_nn1/2Ln​ converges to a nondegenerate random limit and the interval length fluctuates at order n−1/2n^{-1/2}n−1/2, while intervals built on a consistent estimator of σ\sigmaσ (the regenerative method, Proposition 4.34) fluctuate only at order n−1n^{-1}n−1. This is the quantitative trade-off a practitioner faces when choosing between STS and variance-estimation methods.

The paper's results are proved; none of them is formalized. The mission produces machine-checked versions of a support property of Wiener measure on C[0,1]C[0,1]C[0,1] (every path started at 000 is in the support), which is reusable well beyond simulation, and of the deterministic step that turns such a support property into everywhere-discontinuity of a functional.

Difficulty

The goal's statement is elementary, but its proof needs a quantitative fact about Brownian paths: the law of σB\sigma BσB charges every uniform ball around every path in C0[0,1]C_0[0,1]C0​[0,1]. The natural first attempt, using that ggg is continuous PPP-almost everywhere and constant almost surely on σB\sigma BσB, fails without this fact, because almost-sure statements say nothing about any particular path xxx. Mathlib provides Brownian finite-dimensional laws and independent increments, but no small-ball or support estimate for Brownian motion in the uniform metric, so (4.27) has to be built from scratch. A second subtlety is that (4.25) is given for one σ\sigmaσ only; the homogeneity (2.3i) is what upgrades it to all scales, and that upgrade is what makes the range of ggg near xxx unbounded.

Proposition 4.32 needs, in addition, the passage from weak convergence of g(Xn)g(X_n)g(Xn​) to convergence of second moments under uniform integrability, in the space C[0,1]C[0,1]C[0,1].

Formalization scope

  • C[0,1]C[0,1]C[0,1] is C(unitInterval, ℝ) with its sup norm; ρ\rhoρ is dist. Mathlib has no measurable structure on it at this commit, so the Borel σ\sigmaσ-algebra is declared in the mission's definitions file.
  • BBB is a measurable map Ω→C[0,1]\Omega\to C[0,1]Ω→C[0,1] whose coordinates agree, for every ω\omegaω, with a process satisfying Mathlib's IsBrownianReal. "Measurable" in M\mathcal MM means Borel measurable.
  • D(g)D(g)D(g) is the set where ggg is not continuous; P{B∈D(g)}P\{B\in D(g)\}P{B∈D(g)} is the outer measure of the preimage, so no measurability of D(g)D(g)D(g) is assumed.
  • Assumption (2.1) is a structure: joint measurability of YYY, local integrability of its paths (the implicit condition that makes Yˉn\bar Y_nYˉn​ defined), Yˉn\bar Y_nYˉn​ pinned pointwise by its integral formula, σ>0\sigma>0σ>0, and convergence in distribution of XnX_nXn​ to σB\sigma BσB. The index nnn ranges over N\mathbb NN.
  • P{⋅}=1P\{\cdot\}=1P{⋅}=1 is "almost surely". 0<δ<10<\delta<10<δ<1 is added where the confidence level appears.
  • The paper writes "D(g)=C0[0,1]D(g)=C_0[0,1]D(g)=C0​[0,1]" at the end of the proof of Proposition 4.26; its argument proves only C0[0,1]⊆D(g)C_0[0,1]\subseteq D(g)C0​[0,1]⊆D(g), which is what milestone 4 states.
  • Proposition 4.32 uses Bochner integrals; its uniform-integrability hypothesis makes every integral there finite.

The goal is a negation of an existence statement, so it would be trivially true if M\mathcal MM were empty or if the Brownian hypothesis were unsatisfiable. Neither holds: M\mathcal MM contains the batch-means functionals of the paper's Example 3.1 (p. 5), and the goal assumes nothing about small balls, (4.27) or continuity of ggg. Those appear only as milestones.

Contributions welcome: the support theorem for Brownian motion in C[0,1]C[0,1]C[0,1] (milestones 1–2), any of the deterministic steps, and the moment-convergence argument of Proposition 4.32.

Selected references

  • P. W. Glynn and D. L. Iglehart, Simulation output analysis using standardized time series, Mathematics of Operations Research 15(1):1–16, 1990. https://doi.org/10.1287/moor.15.1.1
  • L. Schruben, Confidence interval estimation using standardized time series, Operations Research 31(6):1090–1108, 1983. https://doi.org/10.1287/opre.31.6.1090
  • P. Billingsley, Convergence of Probability Measures, Wiley, 1968. https://doi.org/10.1002/9780470316962
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Bandit AlgorithmsMachine LearningOperations Research+1·Captain: mikedeng1

MNL-Bandit: A Dynamic Learning Approach to Assortment Selection III: On Instances Separated by Δ(v) the UCB Policy Has Regret at Most B₁N² log T/Δ(v) + B₂Research Paper

Motivation

A retailer with limited shelf or screen space must choose which subset of its products to show each arriving customer. Which assortment earns the most depends on customer preferences, and those are unknown at first: the seller learns them from the purchases it observes. This is dynamic assortment selection, and it is a standard model in online retail and revenue management. Agrawal, Avadhanula, Goyal and Zeevi (Oper. Res. 67(5), 2019; preprint arXiv:1706.03880v2) study it under the multinomial logit (MNL) choice model as the MNL-Bandit problem. They propose an epoch-based upper-confidence-bound policy (Algorithm 1) that needs no prior knowledge of the parameters.

Their worst-case guarantee (Theorem 1) is regret of order NTlog⁡NT\sqrt{NT\log NT}NTlogNT​. Many instances are easier than the worst case: the best assortment beats every other feasible assortment by a fixed margin. For such well-separated instances, earlier policies obtained logarithmic regret, but only when told a lower bound on that margin:

  • Rusmevichientong, Shen and Shmoys (2010), O(N2log⁡2T)O(N^2\log^2 T)O(N2log2T);
  • Sauré and Zeevi (2013), O(Nlog⁡T)O(N\log T)O(NlogT) for fixed cardinality.

This mission formalizes the paper's §6.1, which shows that the same parameter-free Algorithm 1 adapts to the separation.

Setting

There are NNN products with known revenues ri∈[0,1]r_i\in[0,1]ri​∈[0,1] and unknown attraction parameters vi≥0v_i\ge0vi​≥0. The no-purchase option has weight v0=1v_0=1v0​=1. Offered an assortment SSS, a customer buys i∈Si\in Si∈S with probability vi/(1+∑j∈Svj)v_i/(1+\sum_{j\in S}v_j)vi​/(1+∑j∈S​vj​) and buys nothing with probability 1/(1+∑j∈Svj)1/(1+\sum_{j\in S}v_j)1/(1+∑j∈S​vj​) (2.1). The expected revenue of SSS is

R(S,v)=∑i∈Srivi1+∑j∈Svj(2.2).R(S,\mathbf v)=\frac{\sum_{i\in S}r_iv_i}{1+\sum_{j\in S}v_j}\quad(2.2).R(S,v)=1+∑j∈S​vj​∑i∈S​ri​vi​​(2.2).

Feasible assortments form a family S\mathcal SS defined by totally unimodular constraints A x(S)≤bA\,x(S)\le bAx(S)≤b (2.3). Assumption 4.1 asks that vi≤v0=1v_i\le v_0=1vi​≤v0​=1 for all iii and that S\mathcal SS be closed under taking subsets.

A policy chooses St∈SS_t\in\mathcal SSt​∈S from the past choices. The regret after TTT customers is Regπ(T,v)=T R(S∗,v)−Eπ∑t=1TR(St,v)\mathrm{Reg}_\pi(T,\mathbf v)=T\,R(S^*,\mathbf v)-\mathbb E_\pi\sum_{t=1}^TR(S_t,\mathbf v)Regπ​(T,v)=TR(S∗,v)−Eπ​∑t=1T​R(St​,v), where S∗S^*S∗ maximizes R(⋅,v)R(\cdot,\mathbf v)R(⋅,v) over S\mathcal SS (2.6).

Algorithm 1 works in epochs: epoch ℓ\ellℓ offers one assortment SℓS_\ellSℓ​ until a customer buys nothing. It keeps three statistics for each product iii:

  • Ti(ℓ)T_i(\ell)Ti​(ℓ), the number of epochs up to ℓ\ellℓ that offered iii;
  • vˉi,ℓ\bar v_{i,\ell}vˉi,ℓ​, the average number of purchases of iii per such epoch;
  • the upper confidence bound vi,ℓUCB=vˉi,ℓ+vˉi,ℓ 48log⁡(Nℓ+1)/Ti(ℓ)+48log⁡(Nℓ+1)/Ti(ℓ)v^{\mathrm{UCB}}_{i,\ell}=\bar v_{i,\ell}+\sqrt{\bar v_{i,\ell}\,48\log(\sqrt N\ell+1)/T_i(\ell)}+48\log(\sqrt N\ell+1)/T_i(\ell)vi,ℓUCB​=vˉi,ℓ​+vˉi,ℓ​48log(N​ℓ+1)/Ti​(ℓ)​+48log(N​ℓ+1)/Ti​(ℓ).

The next epoch offers an assortment maximizing the MNL revenue computed with vUCBv^{\mathrm{UCB}}vUCB in place of v\mathbf vv.

The separation of an instance is the gap between the optimal and the second-best expected revenue among feasible assortments,

Δ(v)=min⁡S∈S: R(S,v)≠R(S∗,v)(R(S∗,v)−R(S,v))(6.1).\Delta(\mathbf v)=\min_{S\in\mathcal S:\,R(S,\mathbf v)\neq R(S^*,\mathbf v)}\big(R(S^*,\mathbf v)-R(S,\mathbf v)\big)\quad(6.1).Δ(v)=S∈S:R(S,v)=R(S∗,v)min​(R(S∗,v)−R(S,v))(6.1).

The analysis uses the threshold τ=4NClog⁡NT/Δ2(v)\tau=4NC\log NT/\Delta^2(\mathbf v)τ=4NClogNT/Δ2(v) (6.2), with C=max⁡{C12,C2}C=\max\{C_1^2,C_2\}C=max{C12​,C2​}, C1=72+24C_1=\sqrt{72}+\sqrt{24}C1​=72​+24​ and C2=144C_2=144C2​=144. It also uses good epochs: those in which every vi,ℓUCBv^{\mathrm{UCB}}_{i,\ell}vi,ℓUCB​ lies above viv_ivi​ and within the confidence width of Lemma 4.1.

Formalization targets

Goal: Theorem 3 (p. 20)

There are absolute constants B1,B2B_1,B_2B1​,B2​ such that for every instance satisfying Assumption 4.1 with ri∈[0,1]r_i\in[0,1]ri​∈[0,1], every tie-breaking rule and every TTT,

Regπ(T,v)≤B1 N2log⁡TΔ(v)+B2.\mathrm{Reg}_\pi(T,\mathbf v)\le B_1\,\frac{N^2\log T}{\Delta(\mathbf v)}+B_2.Regπ​(T,v)≤B1​Δ(v)N2logT​+B2​.

The constants are not fixed, so the goal survives any improvement of them.

Milestones

  • Lemma 4.1 (p. 13): vi,ℓUCB≥viv^{\mathrm{UCB}}_{i,\ell}\ge v_ivi,ℓUCB​≥vi​ with probability ≥1−6/(Nℓ)\ge1-6/(N\ell)≥1−6/(Nℓ), and vi,ℓUCB−vi≤C1vilog⁡(Nℓ+1)/Ti(ℓ)+C2log⁡(Nℓ+1)/Ti(ℓ)v^{\mathrm{UCB}}_{i,\ell}-v_i\le C_1\sqrt{v_i\log(\sqrt N\ell+1)/T_i(\ell)}+C_2\log(\sqrt N\ell+1)/T_i(\ell)vi,ℓUCB​−vi​≤C1​vi​log(N​ℓ+1)/Ti​(ℓ)​+C2​log(N​ℓ+1)/Ti​(ℓ) with probability ≥1−7/(Nℓ)\ge1-7/(N\ell)≥1−7/(Nℓ).
  • Lemma 4.3 (p. 14): (1+∑j∈Svj)(R~(S)−R(S,v))(1+\sum_{j\in S}v_j)(\tilde R(S)-R(S,\mathbf v))(1+∑j∈S​vj​)(R~(S)−R(S,v)) is at most the sum of these widths over the offered set, with probability ≥1−13/ℓ\ge1-13/\ell≥1−13/ℓ.
  • Lemma 6.1 (p. 20): in a good epoch, if every offered product has Ti(ℓ)≥τT_i(\ell)\ge\tauTi​(ℓ)≥τ, the offered assortment is optimal.
  • Lemma 6.2 (p. 20): at most NτN\tauNτ good epochs offer a sub-optimal assortment.
  • Corollary C.1 (p. 48): at most Nlog⁡NTN\log NTNlogNT epochs offer a product with Ti(ℓ)<log⁡NTT_i(\ell)<\log NTTi​(ℓ)<logNT.
  • (C.5) (p. 48): the regret is at most Eπ∑ℓ≤L(1+V(Sℓ))(R(S∗,v)−R(Sℓ,v))\mathbb E_\pi\sum_{\ell\le L}(1+V(S_\ell))(R(S^*,\mathbf v)-R(S_\ell,\mathbf v))Eπ​∑ℓ≤L​(1+V(Sℓ​))(R(S∗,v)−R(Sℓ​,v)).

Companion: Corollary 6.1 (p. 21)

Under the cardinality constraint ∣S∣≤K|S|\le K∣S∣≤K: Regπ(T,v)≤B1 NKlog⁡NT/Δ(v)+B2\mathrm{Reg}_\pi(T,\mathbf v)\le B_1\,NK\log NT/\Delta(\mathbf v)+B_2Regπ​(T,v)≤B1​NKlogNT/Δ(v)+B2​.

Significance

The result. Theorem 3 shows that one policy is simultaneously near-optimal in the worst case (Theorem 1, O~(NT)\tilde O(\sqrt{NT})O~(NT​), matched by the lower bound of Theorem 2 up to logarithms) and logarithmic on separated instances. It does so without being told Δ(v)\Delta(\mathbf v)Δ(v), which the separation-based policies of Rusmevichientong et al. and Sauré–Zeevi require. Under a cardinality constraint, Corollary 6.1 matches the order of Sauré–Zeevi's bound.

Formalizing it. The theorem is proved in the paper (Appendix C), and no machine-checked version exists. A formal proof has to make several things precise:

  • Algorithm 1 as a function of the observed history;
  • the epoch structure of a finite horizon;
  • the pathwise counting arguments of Lemmas 6.1–6.2 and Corollary C.1;
  • the probabilistic estimates inherited from the worst-case analysis.

Two printed details need care, and the formal statements fix them: Appendix C defines good epochs with "or" where both inequalities are meant, and Lemma 6.2's proof skips one case.

Difficulty

The counting part looks routine but depends on indexing. The bounds that are good at the end of epoch ℓ\ellℓ select the assortment of epoch ℓ+1\ell+1ℓ+1, so "a good epoch offering a sub-optimal set" pairs two consecutive epochs. A per-product count of under-sampled epochs is then off by one per product, so the printed bound NτN\tauNτ does not follow from the statement of Lemma 6.1 by counting alone.

The probabilistic part is the harder one. The per-epoch purchase counts are geometric with mean viv_ivi​ only conditionally on adaptively chosen assortments. The confidence statements must hold uniformly over a random number of samples, and the regret must be converted from customers to epochs, whose lengths are random and truncated at TTT. A union bound over all epochs costs a factor log⁡T\log TlogT, and that factor has to stay within the claimed N2log⁡T/ΔN^2\log T/\DeltaN2logT/Δ.

Formalization scope

Products are Fin N (0-based), and choices are Option (Fin N) with none the no-purchase option. A policy maps the past choices to an assortment. The law of a length-TTT history is the product of MNL probabilities, so every expectation is a finite sum. Revenue is the published ChoiceCDLP.MNL.mnlObjective v r 1, and R(S∗,v)R(S^*,\mathbf v)R(S∗,v) is a Finset.sup' over the nonempty family S\mathcal SS. Algorithm 1 is defined as an explicit state machine and never reads v\mathbf vv. Ties in its argmax are broken by an arbitrary selector, and every statement quantifies over all selectors.

Standing assumptions carried by every statement:

  • 0≤vi≤10\le v_i\le10≤vi​≤1;
  • ri∈[0,1]r_i\in[0,1]ri​∈[0,1];
  • the totally unimodular form of S\mathcal SS;
  • closure under subsets;
  • nonemptiness of S\mathcal SS (needed for S∗S^*S∗ to exist).

Disclosed conventions:

  • UCB before sampling. vi,ℓUCB=1v^{\mathrm{UCB}}_{i,\ell}=1vi,ℓUCB​=1 while Ti(ℓ)=0T_i(\ell)=0Ti​(ℓ)=0.
  • Degenerate separation. Δ(v)=1\Delta(\mathbf v)=1Δ(v)=1 when every feasible assortment is optimal; the regret is then 000.
  • Lemma 4.1 constants. C1,C2C_1,C_2C1​,C2​ take the values established in the proof of Lemma 4.1.
  • Probabilistic lemmas. They are stated for every horizon TTT as probabilities that epoch ℓ\ellℓ is completed and the bound fails.
  • Lemma 4.3. The printed free index iii is read as the sum over the offered set, and R~\tilde RR~ uses the bounds of the preceding epoch.
  • (C.5). It is stated as "≤\le≤", since the last epoch is truncated at TTT.

The constants B1,B2B_1,B_2B1​,B2​ are quantified before every other object. A constant depending on NNN, v\mathbf vv or Δ\DeltaΔ would make the theorem say only that regret is finite. The policy is pinned to Algorithm 1, not to any optimistic rule.

Contributions are welcome at every level:

  • the pathwise lemmas (6.1, 6.2, C.1), which need no probability;
  • the epoch rewriting (C.5);
  • the concentration Lemmas 4.1 and 4.3, shared with the companion mission on Theorem 1;
  • reusable infrastructure: MNL choice probabilities and finite-horizon history laws for adaptive policies.

Selected references

  • S. Agrawal, V. Avadhanula, V. Goyal, A. Zeevi, MNL-Bandit: A Dynamic Learning Approach to Assortment Selection, Operations Research 67(5):1453–1485, 2019. https://doi.org/10.1287/opre.2018.1832 ; preprint arXiv:1706.03880v2. https://arxiv.org/abs/1706.03880v2
  • P. Rusmevichientong, Z.-J. M. Shen, D. B. Shmoys, Dynamic assortment optimization with a multinomial logit choice model and capacity constraint, Operations Research 58(6):1666–1680, 2010. https://doi.org/10.1287/opre.1100.0866
  • D. Sauré, A. Zeevi, Optimal dynamic assortment planning with demand learning, Manufacturing & Service Operations Management 15(3):387–404, 2013. https://doi.org/10.1287/msom.2013.0429
  • K. Talluri, G. van Ryzin, Revenue management under a general discrete choice model of consumer behavior, Management Science 50(1):15–33, 2004. https://doi.org/10.1287/mnsc.1030.0147
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Functional AnalysisMarkov ChainProbability·Captain: mikedeng1

Logarithmic Sobolev Inequalities for Finite Markov Chains 3: Lower Bound α ≥ (1 − 2/q)λ / 2(λt_q + log M_q + (q − 2)/q) from a Bound on ‖H_{t_q}‖_{2→q}Research Paper

Motivation

A finite Markov chain describes a system that changes state according to fixed transition probabilities. For a chain that settles toward an equilibrium distribution, a central question is how quickly the effect of its starting state disappears. The logarithmic Sobolev constant supplies quantitative control of this convergence and, through hypercontractive estimates, also governs how the continuous-time transition operator changes the size of functions measured in different norms. Diaconis and Saloff-Coste's 1996 paper develops these relations for finite chains and uses them to study mixing on graphs and product spaces.

The constant can be hard to calculate directly. Its definition is an infimum over all nonconstant functions, while a particular Markov semigroup may admit an accessible bound from ℓ2\ell^2ℓ2 to ℓq\ell^qℓq at one time. Theorem 3.9 turns such an operator estimate into a numerical lower bound for the log-Sobolev constant. This mission formalizes that result, including both finite qqq and the supremum-norm endpoint.

Setting

Let X\mathcal XX be a finite state space. A Markov kernel K(x,y)K(x,y)K(x,y) is nonnegative, with ∑yK(x,y)=1\sum_yK(x,y)=1∑y​K(x,y)=1 for every xxx. A strictly positive stationary distribution π\piπ satisfies ∑xπ(x)K(x,y)=π(y)\sum_x\pi(x)K(x,y)=\pi(y)∑x​π(x)K(x,y)=π(y) and ∑xπ(x)=1\sum_x\pi(x)=1∑x​π(x)=1. The chain is reversible when π(x)K(x,y)=π(y)K(y,x)\pi(x)K(x,y)=\pi(y)K(y,x)π(x)K(x,y)=π(y)K(y,x) for every pair of states. Its continuous-time heat semigroup is Ht=e−t(I−K)H_t=e^{-t(I-K)}Ht​=e−t(I−K), acting on a function fff by HtfH_tfHt​f. These conventions follow §§2.1–2.3 of the source paper.

For a real function on X\mathcal XX, write ∥f∥p=(∑x∣f(x)∣pπ(x))1/p\|f\|_p=(\sum_x|f(x)|^p\pi(x))^{1/p}∥f∥p​=(∑x​∣f(x)∣pπ(x))1/p when ppp is finite, and ∥f∥∞=max⁡x∣f(x)∣\|f\|_\infty=\max_x|f(x)|∥f∥∞​=maxx​∣f(x)∣. The Dirichlet form is E(f,g)=∑x(f(x)−Kf(x))g(x)π(x)\mathcal E(f,g)=\sum_x(f(x)-Kf(x))g(x)\pi(x)E(f,g)=∑x​(f(x)−Kf(x))g(x)π(x). The quadratic entropy functional is L(f)=∑x∣f(x)∣2log⁡(∣f(x)∣2/∥f∥22)π(x)\mathcal L(f)=\sum_x|f(x)|^2\log(|f(x)|^2/\|f\|_2^2)\pi(x)L(f)=∑x​∣f(x)∣2log(∣f(x)∣2/∥f∥22​)π(x), with a zero contribution where f(x)=0f(x)=0f(x)=0. Write Ef=∑xf(x)π(x)Ef=\sum_xf(x)\pi(x)Ef=∑x​f(x)π(x) and Var⁡π(f)=∥f−Ef∥22\operatorname{Var}_\pi(f)=\|f-Ef\|_2^2Varπ​(f)=∥f−Ef∥22​.

The spectral gap in this mission is the variational constant λ=inf⁡Var⁡π(f)≠0E(f,f)/Var⁡π(f)\lambda=\inf_{\operatorname{Var}_\pi(f)\ne0}\mathcal E(f,f)/\operatorname{Var}_\pi(f)λ=infVarπ​(f)=0​E(f,f)/Varπ​(f), as in (2.4). The log-Sobolev constant is α=inf⁡L(f)≠0E(f,f)/L(f)\alpha=\inf_{\mathcal L(f)\ne0}\mathcal E(f,f)/\mathcal L(f)α=infL(f)=0​E(f,f)/L(f), as in (3.1). These definitions specify the quantities that Theorem 3.9 relates; in particular, λ\lambdaλ is the paper's variational quantity, rather than an eigenvalue expression imported from a different convention.

Formalization targets

Theorem 3.9: a single heat-operator estimate bounds α\alphaα

Suppose 2<q<∞2<q<\infty2<q<∞, tq>0t_q>0tq​>0, and MqM_qMq​ satisfy ∥Htqf∥q≤Mq∥f∥2\|H_{t_q}f\|_q\le M_q\|f\|_2∥Htq​​f∥q​≤Mq​∥f∥2​ for every function fff. The paper's theorem asserts

α≥(1−2/q)λ2(λtq+log⁡Mq+(q−2)/q).\alpha\ge\frac{(1-2/q)\lambda}{2\left(\lambda t_q+\log M_q+(q-2)/q\right)}.α≥2(λtq​+logMq​+(q−2)/q)(1−2/q)λ​.

It also covers q=∞q=\inftyq=∞: the hypothesis then uses ∥Htqf∥∞\|H_{t_q}f\|_\infty∥Htq​​f∥∞​, and the two fractions involving qqq in the displayed bound become 111.

Companion results

Theorem 3.10 replaces HtqH_{t_q}Htq​​ in the norm hypothesis with Htq−EH_{t_q}-EHtq​​−E, where EEE sends a function to its constant mean. Corollary 3.11 relates α\alphaα to τ\tauτ, the first time at which every heat-kernel density htx(y)=Ht(x,y)/π(y)h_t^x(y)=H_t(x,y)/\pi(y)htx​(y)=Ht​(x,y)/π(y) is within 1/e1/e1/e of 111 in ℓ2(π)\ell^2(\pi)ℓ2(π):

12α≤τ≤4+log⁡log⁡(1/π∗)4α,π∗=min⁡xπ(x).\frac1{2\alpha}\le\tau\le\frac{4+\log\log(1/\pi_*)}{4\alpha}, \qquad \pi_*=\min_x\pi(x).2α1​≤τ≤4α4+loglog(1/π∗​)​,π∗​=xmin​π(x).

The three milestones reproduce the interpolation estimate (3.6), the resulting entropy inequality, and the centering inequality (3.7). Theorem 3.10's printed finite-qqq denominator contains (q−2)/2(q-2)/2(q−2)/2; its displayed proof and the q=∞q=\inftyq=∞ use in Corollary 3.11 require (q−2)/q(q-2)/q(q−2)/q. That proof also needs log⁡Mq+(q−2)/q≥0\log M_q+(q-2)/q\ge0logMq​+(q−2)/q≥0, which the page does not state and without which the printed statement fails on a four-state product chain. The formal companion records both corrections, while the main goal follows the printed Theorem 3.9 exactly.

Significance

Theorem 3.9 makes a norm bound at a chosen time useful beyond that time: it yields a bound on a functional inequality that holds for every function on the state space. Thus estimates obtained from an explicit heat kernel or another analytic method can be compared across chains using the same constant α\alphaα. The centered version and the bound for τ\tauτ connect this functional viewpoint back to convergence from a point mass, as the paper explains in §3.4.

The mathematical results are proved in the 1996 paper. Here the remaining work is to give their finite-state objects, norm hypotheses, and constants machine-checked meanings, then formalize the proofs. The definition layer and the centering inequality have use beyond this mission: they can support other statements about entropy decay and heat-kernel convergence in the same paper.

Difficulty

A bound for HtH_tHt​ in the same norm is too weak to recover the displayed lower bound: the information here is the change from an ℓ2\ell^2ℓ2 input to an ℓq\ell^qℓq output. The dependence of the exponent on time must retain the factors (1−2/q)(1-2/q)(1−2/q) and (q−2)/q(q-2)/q(q−2)/q exactly. The endpoint q=∞q=\inftyq=∞ also requires a separate norm statement, since a real exponent cannot represent infinity. The centering inequality (3.7) is another substantial step; the paper points to earlier proofs rather than treating it as immediate.

Formalization scope

The state space is a finite Lean type, the kernel a real matrix, and the invariant law a positive real-valued probability vector. Reversibility is detailed balance, and irreducibility is retained from the standing setting of §3.1. The heat semigroup uses the already published Poissonized heat kernel. Operator norms are represented by inequalities quantified over every real function. The finite-qqq and q=∞q=\inftyq=∞ conclusions are separate clauses of the goal. Time is real; tq>0t_q>0tq​>0 makes explicit the positive-time convention used in §3.4. Theorem 3.10 carries the condition Mq≥e−(q−2)/qM_q\ge e^{-(q-2)/q}Mq​≥e−(q−2)/q (and M∞≥e−1M_\infty\ge e^{-1}M∞​≥e−1) described above; Corollary 3.11 is stated without any extra condition.

The variational constants are real infima, the logarithms and real powers use Lean's total operations, and the supremum norm is a supremum over the finite state space. The stationary probability hypothesis rules out an empty state space; the operator hypothesis on the constant function forces Mq≥1M_q\ge1Mq​≥1 in Theorem 3.9. These facts prevent the bound from arising from a zero norm, an empty operator test, an invalid logarithm, or an eigenvalue convention different from (2.4). Useful contributions include finite-state entropy inequalities, interpolation machinery, estimates for the heat operator, and proofs of the three stated milestones.

Selected references

  • P. Diaconis and L. Saloff-Coste, Logarithmic Sobolev inequalities for finite Markov chains, Annals of Applied Probability 6 (1996), 695–750. DOI.
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Algorithmic Game TheoryMarkov ChainProbability·Captain: mikedeng1

The Evolution of Conventions III: In 2 × 2 Games with Two Strict Equilibria, the Generically Stable Equilibria of Adaptive Play Are the Weakly Risk Dominant OnesResearch Paper

Motivation

Many games have several strict Nash equilibria, and equilibrium analysis alone does not say which one a population will settle on. Harsanyi and Selten (1988) proposed risk dominance as a selection criterion for 2×22\times22×2 games: of two strict equilibria, select the one whose basin is "larger" in a precise payoff sense. That criterion is axiomatic. H. Peyton Young's The Evolution of Conventions (Econometrica, 1993) derives a selection from a dynamic model instead: boundedly rational players with finite memory, incomplete information about the past and occasional mistakes. Its Theorem 3 says that, in 2×22\times22×2 games, the dynamic selection and risk dominance coincide.

Timeline.

  • 1984. Freidlin and Wentzell develop the theory of small random perturbations of dynamical systems, including the tree characterization of limiting stationary measures.
  • 1990. Foster and Young introduce stochastic stability for evolutionary processes with vanishing noise.
  • 1993. Kandori, Mailath and Rob prove that in symmetric 2×22\times22×2 games with a single population, the long-run equilibrium of a mutation process is the risk dominant one. Young (1993) proves the same selection for adaptive play, a two-population model with sampling from a finite memory, for every 2×22\times22×2 game with two strict equilibria, not only symmetric ones. Its Example 3 shows that in 3×33\times33×3 games the selected equilibrium can differ from both the risk dominant and the Pareto optimal one.

Setting

A finite game Γ\GammaΓ has players iii with finite strategy sets SiS_iSi​ and payoffs ui(s)u_i(s)ui​(s). Fix a memory mmm and a sample size kkk with 1≤k≤m1\le k\le m1≤k≤m. A state is the sequence hhh of the last mmm plays (strategy-tuples), oldest first; a successor of hhh drops the oldest play and appends a new one. In each period each player draws a sample of kkk of the mmm recorded plays and chooses a best reply to it (maximizing total payoff against the sampled plays). The choice probabilities pi(s∣h)p_i(s\mid h)pi​(s∣h) form a best-reply distribution: pi(s∣h)>0p_i(s\mid h)>0pi​(s∣h)>0 exactly when sss is a best reply to some sample of size kkk. This gives adaptive play P0P^0P0, display (1).

With mistakes, each player iii independently experiments with probability ελi\varepsilon\lambda_iελi​ and then plays sss with probability qi(s∣h)>0q_i(s\mid h)>0qi​(s∣h)>0. This gives the perturbed chain PεP^\varepsilonPε of display (2). It has a unique stationary distribution με\mu^\varepsilonμε. A state hhh is stochastically stable if lim⁡ε→0μhε>0\lim_{\varepsilon\to0}\mu^\varepsilon_h>0limε→0​μhε​>0. A convention is mmm repetitions of a strict pure Nash equilibrium. With LΓL_\GammaLΓ​ the longest shortest best-reply path to a strict equilibrium, a strict equilibrium is generically stable if its convention is stochastically stable for all sufficiently large kkk and all mmm with k≤m/(LΓ+2)k\le m/(L_\Gamma+2)k≤m/(LΓ​+2).

For a 2×22\times22×2 game in normal form, with Row's payoffs arca_{rc}arc​ and Column's brcb_{rc}brc​ satisfying a11>a21a_{11}>a_{21}a11​>a21​, b11>b12b_{11}>b_{12}b11​>b12​, a22>a12a_{22}>a_{12}a22​>a12​, b22>b21b_{22}>b_{21}b22​>b21​, set

R1=min⁡{a11−a21a11−a12−a21+a22,b11−b12b11−b12−b21+b22},R2=min⁡{a22−a12a11−a12−a21+a22,b22−b21b11−b12−b21+b22}.R_1=\min\Big\{\tfrac{a_{11}-a_{21}}{a_{11}-a_{12}-a_{21}+a_{22}},\tfrac{b_{11}-b_{12}}{b_{11}-b_{12}-b_{21}+b_{22}}\Big\},\qquad R_2=\min\Big\{\tfrac{a_{22}-a_{12}}{a_{11}-a_{12}-a_{21}+a_{22}},\tfrac{b_{22}-b_{21}}{b_{11}-b_{12}-b_{21}+b_{22}}\Big\}.R1​=min{a11​−a12​−a21​+a22​a11​−a21​​,b11​−b12​−b21​+b22​b11​−b12​​},R2​=min{a11​−a12​−a21​+a22​a22​−a12​​,b11​−b12​−b21​+b22​b22​−b21​​}.

(1,1)(1,1)(1,1) weakly risk dominates (2,2)(2,2)(2,2) if R1≥R2R_1\ge R_2R1​≥R2​.

Formalization targets

Goal: Theorem 3 (p. 72)

(1,1) generically stable  ⟺  R1≥R2,(2,2) generically stable  ⟺  R2≥R1.(1,1)\text{ generically stable}\iff R_1\ge R_2,\qquad (2,2)\text{ generically stable}\iff R_2\ge R_1.(1,1) generically stable⟺R1​≥R2​,(2,2) generically stable⟺R2​≥R1​.

This holds for every 2×22\times22×2 game in normal form, for every best-reply distribution and every admissible experimentation.

Milestones, in the order the proof uses them

  1. PεP^\varepsilonPε is irreducible and aperiodic and has a unique stationary distribution (§6, pp. 67–68).
  2. (2) is a regular perturbation of (1): Pε→P0P^\varepsilon\to P^0Pε→P0, and Phh′εP^\varepsilon_{hh'}Phh′ε​ is of exact order εr(h,h′)\varepsilon^{r(h,h')}εr(h,h′), with r(h,h′)r(h,h')r(h,h′) the number of mistakes (Appendix, p. 77).
  3. Theorem 2 (p. 69): the stochastically stable states are those in the recurrent classes of P0P^0P0 of minimum stochastic potential, independently of λ\lambdaλ and qqq.
  4. Corollary (p. 70): for weakly acyclic games with k≤m/(LΓ+2)k\le m/(L_\Gamma+2)k≤m/(LΓ​+2), the stable states are the conventions of minimum stochastic potential.
  5. The 2×22\times22×2 case is acyclic with LΓ=1L_\Gamma=1LΓ​=1, and for k≤m/3k\le m/3k≤m/3 the recurrent classes of P0P^0P0 are {h1}\{h_1\}{h1​} and {h2}\{h_2\}{h2​} (p. 70).
  6. r12=⌈R1k⌉r_{12}=\lceil R_1k\rceilr12​=⌈R1​k⌉ and 7. r21=⌈R2k⌉r_{21}=\lceil R_2k\rceilr21​=⌈R2​k⌉ (pp. 71–72).
  7. If R1>R2R_1>R_2R1​>R2​, then h1h_1h1​ is the unique stable convention, and if R1=R2R_1=R_2R1​=R2​, both are, for all large kkk and m≥3km\ge3km≥3k (p. 72).

Significance

Theorem 3 gives a dynamic foundation for risk dominance: an equilibrium selection criterion defined from payoffs alone is the long-run outcome of a decentralized learning process with sampling and rare mistakes. It requires no symmetry between the two player roles. Theorem 2 makes stochastic stability computable: a limit of stationary distributions is reduced to a minimum-weight arborescence over recurrent classes. That reduction is what the 2×22\times22×2 computation, and later applications of the method to bargaining and contracting, rely on. The equivalence of the RRR-form with the product form (a11−a21)(b11−b12)≥(a22−a12)(b22−b21)(a_{11}-a_{21})(b_{11}-b_{12})\ge(a_{22}-a_{12})(b_{22}-b_{21})(a11​−a21​)(b11​−b12​)≥(a22​−a12​)(b22​−b21​) of Harsanyi and Selten is elementary algebra and is not a target here.

The results are proved in the paper. To our knowledge none of them has a machine-checked proof. The mission produces formal statements of the model (adaptive play, its perturbation, stochastic stability, resistance and stochastic potential) that are reusable for other stochastic-stability results. Closing the goal also requires formalizing Young's finite version of the Freidlin–Wentzell theorem, the subject of the companion mission The Evolution of Conventions II.

Difficulty

The paper's argument has two hard parts. The first is Theorem 2: identifying the limit of με\mu^\varepsilonμε requires the Markov chain tree theorem (the stationary distribution of an irreducible chain as a ratio of sums over spanning in-trees) together with an order-of-magnitude analysis in ε\varepsilonε. The second is the exact resistance ⌈R1k⌉\lceil R_1k\rceil⌈R1​k⌉. The page constructs a path with that many mistakes (Table 1), but the matching lower bound, that no combination of mistakes by both players does better, is only asserted. It needs an argument about the first period in which some player's best reply switches. A naive count of single-player mistake runs gives only the upper bound. The tie case of (5) also matters: equality makes strategy 2 a best reply, which is why the ceiling and not the floor appears.

Formalization scope

Players are a finite type and strategies finite types. A state is Fin m → (∀ i, S i) with position 0 the oldest play. A sample is a set of kkk positions, and a best reply maximizes the summed payoff against the sampled plays. Transition matrices are Matrix H H ℝ. Stochastic stability is a one-sided limit ε→0+\varepsilon\to0^+ε→0+ of the stationary distributions of PεP^\varepsilonPε, over the admissible range 0<ε0<\varepsilon0<ε, ελi≤1\varepsilon\lambda_i\le1ελi​≤1. Resistances are natural numbers on successor pairs. Recurrent classes are the essential classes of P0P^0P0, and iii-trees are parent maps on the set of classes that reach the root. "k≤m/(LΓ+2)k\le m/(L_\Gamma+2)k≤m/(LΓ​+2)" is the natural-number inequality k(LΓ+2)≤mk(L_\Gamma+2)\le mk(LΓ​+2)≤m. In the 2×22\times22×2 game, players and strategies are Fin 2, with the paper's 1,21,21,2 written as 0, 1.

Two corrected slips are recorded in the statements. On p. 68 the recurrent classes are "of PεP^\varepsilonPε" for P0P^0P0, and on p. 77 "the process PεP^\varepsilonPε defined in (1)" is P0P^0P0.

Trivializing formalizations are ruled out. Stochastic stability is defined from stationary distributions, not from resistances, and generic stability is defined from stochastic stability, not from ⌈R1k⌉\lceil R_1k\rceil⌈R1​k⌉ versus ⌈R2k⌉\lceil R_2k\rceil⌈R2​k⌉. Both definitions quantify over every best-reply distribution and every admissible (λ,q)(\lambda,q)(λ,q) rather than a fixed sampling law. "Sufficiently large kkk" is an eventual statement with a threshold, not "for some kkk".

A complete development needs Markov chain stationary distributions on finite spaces, the Markov chain tree theorem, limits of rational functions of ε\varepsilonε, and the combinatorics of sampling in 2×22\times22×2 games. The perturbation theory (milestones 1–3) is reusable for any finite stochastic-stability model. Contributions to the tree theorem and to the two resistance computations are particularly welcome.

Related platform work: stochastic fictitious play (StochFictPlay.*, Hofbauer–Sandholm) and calibrated learning to correlated equilibrium (CalibratedCE.*, Foster–Vohra) study other learning dynamics in games. The sibling missions The Evolution of Conventions I (Theorem 1, convergence of adaptive play) and II (Theorem 4, regular perturbations of Markov chains) formalize the results this mission's milestones invoke.

Selected references

  • H. P. Young, The Evolution of Conventions, Econometrica 61(1), 1993, 57–84. https://doi.org/10.2307/2951778
  • J. C. Harsanyi and R. Selten, A General Theory of Equilibrium Selection in Games, MIT Press, 1988.
  • M. Kandori, G. J. Mailath and R. Rob, Learning, Mutation, and Long Run Equilibria in Games, Econometrica 61(1), 1993, 29–56. https://doi.org/10.2307/2951777
  • D. Foster and H. P. Young, Stochastic Evolutionary Game Dynamics, Theoretical Population Biology 38, 1990, 219–232. https://doi.org/10.1016/0040-5809(90)90011-J
  • M. I. Freidlin and A. D. Wentzell, Random Perturbations of Dynamical Systems, Springer, 1984. https://doi.org/10.1007/978-1-4684-0176-9
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AnalysisOperations ResearchProbability+1·Captain: mikedeng1

Some Useful Functions for Functional Limit Theorems 4: Time Reversal Is a J₁ Isometry and Reversal from the Origin Is 2-LipschitzResearch Paper

Why time reversal matters

Functional limit theorems describe the behavior of entire time-indexed paths under scaling. In queueing and other stochastic models, a path of departures, workload, or accumulated input may be related to another path by reversing a finite observation window. To carry a limit theorem through that change of viewpoint, one needs to know how reversal acts on the topology of the path space. Ward Whitt's 1980 paper studies composition, reflection, first passage, and time reversal as maps that transfer functional limit theorems to derived processes (Whitt 1980).

The time-reversal result is a precise metric statement. Ordinary reversal preserves the Skorohod J1J_1J1​ distance exactly. A version shifted to begin at the group identity satisfies a bound with constant two. These facts give continuity and, when the random paths satisfy the hypotheses, make reversal available to the continuous mapping theorem. Whitt's introduction explains how deterministic path continuity connects to stochastic-process limits (Whitt 1980, pp. 67–69).

Paths, distances, and reversal

Let SSS be a complete separable metric group, written additively, with identity 000 and metric mmm. The metric is translation invariant: moving both points by the same group element leaves their distance unchanged. Let DDD contain the càdlàg paths x:[0,1]→Sx:[0,1]\to Sx:[0,1]→S, meaning paths that are right continuous and possess left limits. Section 8 additionally requires x(1)=x(1−)x(1)=x(1-)x(1)=x(1−), so the terminal value agrees with the value approached from earlier times. Let Dθ={x∈D:x(0)=0}D_\theta=\{x\in D:x(0)=0\}Dθ​={x∈D:x(0)=0}. These are the spaces Whitt fixes for time reversal (Whitt 1980, p. 83).

The uniform distance is ρ(x,y)=sup⁡0≤t≤1m(x(t),y(t))\rho(x,y)=\sup_{0\le t\le1}m(x(t),y(t))ρ(x,y)=sup0≤t≤1​m(x(t),y(t)). A time change λ∈Λ\lambda\in\Lambdaλ∈Λ is an increasing homeomorphism of [0,1][0,1][0,1] onto itself; e(t)=te(t)=te(t)=t is the identity time change. The J1J_1J1​ distance used in the paper is

d(x,y)=inf⁡λ∈Λmax⁡{ρ(λ,e),ρ(x,y∘λ)}.d(x,y)=\inf_{\lambda\in\Lambda} \max\{\rho(\lambda,e),\rho(x,y\circ\lambda)\}.d(x,y)=λ∈Λinf​max{ρ(λ,e),ρ(x,y∘λ)}.

Two paths may be close when their values can be matched after a small distortion of time. This is the paper's equation (2.1), rather than an unspecified equivalent J1J_1J1​ metric (Whitt 1980, p. 70).

The reverse-time map reads the left limit at the reflected time:

R(x)(t)={x((1−t)−),0≤t<1,x(0),t=1,r(x)(t)=R(x)(t)−x(1).R(x)(t)= \begin{cases} x((1-t)-),&0\le t<1,\\ x(0),&t=1, \end{cases} \qquad r(x)(t)=R(x)(t)-x(1).R(x)(t)={x((1−t)−),x(0),​0≤t<1,t=1,​r(x)(t)=R(x)(t)−x(1).

The left limit is essential: the direct value x(1−t)x(1-t)x(1−t) places jumps on the wrong side and generally does not give a right-continuous reverse path. The terminal convention gives R(x)(0)=x(1)R(x)(0)=x(1)R(x)(0)=x(1), so r(x)(0)=0r(x)(0)=0r(x)(0)=0. Whitt also uses the reflected time change (−r)(λ)(t)=1−λ(1−t)(-r)(\lambda)(t)=1-\lambda(1-t)(−r)(λ)(t)=1−λ(1−t) in the proof (Whitt 1980, pp. 83–84).

Formalization targets

The goal is Whitt's Theorem 8.1. For every x,y∈Dx,y\in Dx,y∈D,

d(Rx,Ry)=d(x,y),d(rx,ry)≤2d(x,y).d(Rx,Ry)=d(x,y),\qquad d(rx,ry)\le 2d(x,y).d(Rx,Ry)=d(x,y),d(rx,ry)≤2d(x,y).

The second inequality also applies when both paths lie in DθD_\thetaDθ​, since Dθ⊆DD_\theta\subseteq DDθ​⊆D. The constant is the paper's printed constant, not a parameter to optimize in this mission (Whitt 1980, Theorem 8.1, p. 83).

The milestones record four claims from the theorem's proof: reversal preserves its path spaces and has inverse behavior on its natural domains; reflected time changes stay in Λ\LambdaΛ; reversal obeys exact and bounded uniform-distance relations; and reversal interacts with time changes through (−r)(λ)(-r)(\lambda)(−r)(λ). Their descriptions reproduce the printed proof sentences. The proof calls the time-change cost a “minimum” once, although equation (2.1) and the displayed calculation use a maximum. The formal target follows equation (2.1) (Whitt 1980, pp. 70, 84).

What the result gives

An isometry preserves every J1J_1J1​ distance, so ordinary reversal preserves convergent and Cauchy sequences in this metric. The bound for rrr makes shifted reversal Lipschitz and therefore continuous. A functional limit theorem for input paths can then be translated into one for the corresponding reversed paths whenever the path-space hypotheses hold. The result is already proved in Whitt's paper; the open work here is a machine-checked development of its definitions, supporting claims, and metric theorem.

Formalizing the result also creates reusable interfaces for endpoint-constrained càdlàg paths, left-limit reversal, uniform path distance, and reflected time changes. Those interfaces may support later statements about reversed stochastic models. This mission does not assert weak convergence of probability laws or Borel measurability; those would require a separate measurable-space development for DDD.

Mathematical difficulty

The immediate idea t↦x(1−t)t\mapsto x(1-t)t↦x(1−t) does not preserve càdlàg paths at jumps: a right-continuous jump becomes left-continuous. The correction uses left limits, but endpoint behavior then matters. Without x(1)=x(1−)x(1)=x(1-)x(1)=x(1−), the shifted reverse path need not start at the identity. The J1J_1J1​ assertion also concerns an infimum over all allowed time changes, so a uniform-distance statement alone does not establish the theorem. These are the points at which reflection of the time axis becomes a claim about the precise path-space topology (Whitt 1980, pp. 83–84).

Formalization scope

Lean represents paths as total functions R→S\mathbb R\to SR→S; all path conditions, metrics, and equality claims read only [0,1][0,1][0,1]. Càdlàg membership requires right continuity and left limits within the interval, with x(1)=x(1−)x(1)=x(1-)x(1)=x(1−) included in DDD. Completeness and separability are explicit because the paper calls SSS a complete separable metric space. The additive metric group is represented by an additive commutative group with an explicit translation-invariance hypothesis. This chooses the commutative reading exemplified by S=RkS=\mathbb R^kS=Rk; the paper uses additive notation but does not separately state commutativity.

The paper's Λ\LambdaΛ is encoded by strict increase, continuity, and surjectivity on [0,1][0,1][0,1], which characterize increasing homeomorphisms there. The paper's ddd is equation (2.1) on both sides of the goal. Lean uses extended nonnegative distances for ρ\rhoρ and ddd, avoiding the default value a real supremum can assign to an empty or unbounded set. The claims do not become trivial by dropping DDD membership: it is an explicit hypothesis, and the zero path over R\mathbb RR satisfies it. A local, sorry-free check confirms that instance. Two easier statements are excluded on purpose: the goal is stated for the J1J_1J1​ distance ddd, not the uniform distance ρ\rhoρ, and RRR reads the left limit x((1−t)−)x((1-t)-)x((1−t)−), not the value x(1−t)x(1-t)x(1−t).

The proof's first sentence says the maps are one-to-one and onto. The map r:D→Dθr:D\to D_\thetar:D→Dθ​ forgets an additive offset and is not injective on all of DDD; the formal milestone expresses involution for RRR on DDD and for the restriction of rrr to DθD_\thetaDθ​. One identity printed for rrr with x∈Dθx\in D_\thetax∈Dθ​ also holds for every x∈Dx\in Dx∈D; the formal milestone uses that broader domain and says so in its item description. Contributions are welcome for the left-limit and time-change infrastructure as well as the four listed statements and the goal.

Selected references

  • Ward Whitt, Some Useful Functions for Functional Limit Theorems, Mathematics of Operations Research 5(1), 1980, pp. 67–85. DOI: 10.1287/moor.5.1.67.
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