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Stochastic Systems

434 missions · 143 completed

The mathematics of systems that evolve under randomness, modeled as families of random variables indexed by time — from Markov chains and martingales to Brownian motion and stochastic differential equations. The field spans stochastic analysis, filtering and optimal control under uncertainty, ergodic behavior of random dynamics, and concentration of measure, with models reaching across physics, engineering, finance, and biology.

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Operations ResearchProbability·Captain: mikedeng1

Martingale Proofs of Many-Server Heavy-Traffic Limits for Markovian Queues 1: The Centered and √n-Scaled M/M/∞ Queue Converges in D to an Ornstein–Uhlenbeck ProcessResearch Paper

Motivation

Large service systems (call centers, hospital wards, cloud server pools) run with many servers, and for many of them no exact formula describes how the number of busy servers moves over time. Heavy-traffic limits replace such a system by a diffusion process that is easier to analyze. The many-server regime, in which the number of servers and the arrival rate grow together, goes back to Halfin and Whitt (1981) and is the basis of square-root staffing rules in call-center practice.

The simplest many-server model is the M/M/∞M/M/\inftyM/M/∞ queue. Its stationary number in system is Poisson with mean λ/μ\lambda/\muλ/μ, so the centered and n\sqrt nn​-scaled stationary count is asymptotically normal when λn=nμ\lambda_n = n\muλn​=nμ. The question here is about the whole process: does the scaled number in system converge, as a random path, to a diffusion? The classical answer, the Ornstein–Uhlenbeck limit, was first established by Iglehart (1965) with Stone's theorem for birth-and-death processes, and was revisited by strong approximation (Mandelbaum, Massey and Reiman 1998) and, for general service times, by Krichagina and Puhalskii (1997).

Pang, Talreja and Whitt (2007) is a tutorial survey that proves this limit, and its finite-waiting-room extension, with martingale methods. The authors present the argument as a template for non-Markovian and network models (Reed 2009; Dai and Tezcan; Gurvich and Whitt). This mission formalizes the M/M/∞M/M/\inftyM/M/∞ result and the steps of the paper's proof.

Setting

Fix a service rate μ>0\mu > 0μ>0. For each n≥1n \ge 1n≥1, the nnn-th system has arrival rate λn=nμ\lambda_n = n\muλn​=nμ. Let AnA_nAn​ and SnS_nSn​ be independent Poisson processes of rate 111, and let Qn(0)Q_n(0)Qn​(0) be a random initial number of customers, independent of AnA_nAn​ and SnS_nSn​. The number in system Qn(t)Q_n(t)Qn​(t) is the N\mathbb NN-valued process with right-continuous paths having left limits that satisfies, almost surely,

Qn(t)=Qn(0)+An(λnt)−Sn(μ∫0tQn(s) ds),t≥0.(12)Q_n(t) = Q_n(0) + A_n(\lambda_n t) - S_n\Big(\mu \int_0^t Q_n(s)\,ds\Big), \qquad t \ge 0. \qquad (12)Qn​(t)=Qn​(0)+An​(λn​t)−Sn​(μ∫0t​Qn​(s)ds),t≥0.(12)

The departure term is a random time change: each of the Qn(s)Q_n(s)Qn​(s) customers in service completes service at rate μ\muμ. The diffusion-scaled process is Xn(t)=(Qn(t)−n)/nX_n(t) = (Q_n(t) - n)/\sqrt nXn​(t)=(Qn​(t)−n)/n​, the paper's (3). The space DDD consists of paths on [0,∞)[0,\infty)[0,∞) that are right-continuous with left limits, and ⇒\Rightarrow⇒ denotes convergence in distribution.

The limit is the Ornstein–Uhlenbeck (OU) process XXX, driven by a standard Brownian motion BBB, with X(0)X(0)X(0) independent of BBB:

X(t)=X(0)+2μ B(t)−μ∫0tX(s) ds,t≥0.(5)X(t) = X(0) + \sqrt{2\mu}\,B(t) - \mu \int_0^t X(s)\,ds, \qquad t \ge 0. \qquad (5)X(t)=X(0)+2μ​B(t)−μ∫0t​X(s)ds,t≥0.(5)

The proof also uses the scaled martingales Mn,1(t)=(An(λnt)−λnt)/nM_{n,1}(t) = (A_n(\lambda_n t) - \lambda_n t)/\sqrt nMn,1​(t)=(An​(λn​t)−λn​t)/n​ and Mn,2(t)=(Sn(μ∫0tQn)−μ∫0tQn)/nM_{n,2}(t) = \big(S_n(\mu\int_0^t Q_n) - \mu\int_0^t Q_n\big)/\sqrt nMn,2​(t)=(Sn​(μ∫0t​Qn​)−μ∫0t​Qn​)/n​, the fluid processes ΨS,n=Qn/n\Psi_{S,n} = Q_n/nΨS,n​=Qn​/n and ΦS,n(t)=μn∫0tQn(s) ds\Phi_{S,n}(t) = \frac{\mu}{n}\int_0^t Q_n(s)\,dsΦS,n​(t)=nμ​∫0t​Qn​(s)ds, and stochastic boundedness. A sequence of real random variables is stochastically bounded if it is tight, and a sequence of processes is stochastically bounded in DDD if sup⁡0≤t≤T∣Xn(t)∣\sup_{0\le t\le T}|X_n(t)|sup0≤t≤T​∣Xn​(t)∣ is, for every T>0T > 0T>0.

Formalization targets

Goal: Theorem 1.1

If Xn(0)⇒X(0)X_n(0) \Rightarrow X(0)Xn​(0)⇒X(0) in R\mathbb RR, with an arbitrary limit law ν\nuν, then

Xn⇒Xin D as n→∞,X_n \Rightarrow X \quad \text{in } D \text{ as } n \to \infty,Xn​⇒Xin D as n→∞,

where XXX is the OU process (5) with X(0)∼νX(0) \sim \nuX(0)∼ν. The goal fixes no initial distribution and assumes no moment condition on Qn(0)Q_n(0)Qn​(0).

Milestones, in the order of the proof

  1. Lemma 2.1, that (12) defines QQQ, and Lemma 3.3, the crude bound Q(t)≤Q(0)+A(λt)Q(t) \le Q(0) + A(\lambda t)Q(t)≤Q(0)+A(λt).
  2. Lemmas 3.1 and 3.2, which identify ⟨M⟩\langle M \rangle⟨M⟩ for compensated counting processes and for random time changes of a Poisson process. Then Theorem 3.4, the martingale representation Xn=Xn(0)+Mn,1−Mn,2−μ∫0⋅XnX_n = X_n(0) + M_{n,1} - M_{n,2} - \mu\int_0^\cdot X_nXn​=Xn​(0)+Mn,1​−Mn,2​−μ∫0⋅​Xn​, with ⟨Mn,1⟩(t)=μt\langle M_{n,1}\rangle(t) = \mu t⟨Mn,1​⟩(t)=μt and ⟨Mn,2⟩=ΦS,n\langle M_{n,2}\rangle = \Phi_{S,n}⟨Mn,2​⟩=ΦS,n​.
  3. Theorem 4.1(i), the continuity of the integral representation; Lemma 4.1, Gronwall's inequality; and Theorem 4.2, the Poisson FCLT.
  4. Lemmas 5.9, 5.5, 5.8 and 6.2, the stochastic-boundedness route to the fluid limit.
  5. Lemmas 4.3 and 4.2, the fluid limits Qn/n⇒1Q_n/n \Rightarrow 1Qn​/n⇒1 and ΦS,n⇒μe\Phi_{S,n} \Rightarrow \mu eΦS,n​⇒μe; then Lemma 4.4, (Mn,1,Mn,2)⇒(μB1,μB2)(M_{n,1}, M_{n,2}) \Rightarrow (\sqrt\mu B_1, \sqrt\mu B_2)(Mn,1​,Mn,2​)⇒(μ​B1​,μ​B2​).

Significance

Theorem 1.1 describes the transient behavior of a large infinite-server system, not only its stationary law: fluctuations of order n\sqrt nn​ around the offered load nnn form a Gaussian Markov process that relaxes at rate μ\muμ. It is the reference case for the Halfin–Whitt regime, whose finite-server version, Theorem 1.2 of the same paper (the M/M/n/mn+MM/M/n/m_n+MM/M/n/mn​+M queue), is the subject of the companion mission. The milestones are general tools reused well beyond queueing: Gronwall's inequality, the Lipschitz integral map, the Poisson FCLT, stochastic boundedness via Lenglart's inequality, and the fluid limit from stochastic boundedness.

The theorem is proved and classical; no machine-checked proof of it, or of the milestones below, is known. No formal library currently has the Poisson functional central limit theorem in DDD, compensators of counting processes, or random time changes of martingales. Formalizing the paper's proof would produce these, plus a template for the martingale method of heavy-traffic analysis. Alternative proofs, such as the paper's §4.3 route without martingales, are equally welcome as solutions.

Difficulty

Equation (12) is a fixed-point equation: QnQ_nQn​ appears inside the argument of SnS_nSn​. The integral map of Theorem 4.1 is continuous, so the obvious argument is to apply the continuous-mapping theorem to the martingale representation. That reduces the goal to the joint convergence of (Mn,1,Mn,2)(M_{n,1}, M_{n,2})(Mn,1​,Mn,2​). But Mn,2M_{n,2}Mn,2​ is a Poisson martingale evaluated at the random time ΦS,n(t)\Phi_{S,n}(t)ΦS,n​(t), and its limit is identified only after the fluid limit ΦS,n⇒μe\Phi_{S,n} \Rightarrow \mu eΦS,n​⇒μe is known. The fluid limit is itself a statement about the whole sequence QnQ_nQn​, and it needs a separate argument, either Gronwall at fluid scale or stochastic boundedness. Lemma 3.2 requires optional stopping at the continuum of stopping times I(t)I(t)I(t), and the moment conditions (22) must be checked through the crude bound. Removing E[Qn(0)]<∞E[Q_n(0)] < \inftyE[Qn​(0)]<∞ needs a truncation of the initial conditions (§6.3).

Formalization scope

  • Time. Paths are functions R→R\mathbb R \to \mathbb RR→R and every condition is for t≥0t \ge 0t≥0. Brownian motions and filtrations are indexed by R≥0\mathbb R_{\ge 0}R≥0​.
  • Probability space. All systems live on one probability space. Each nnn has its own pair of Poisson processes; the paper's single pair is a special case, and weak convergence depends only on laws. Sequences start at n=1n = 1n=1.
  • Weak convergence in DDD to a continuous limit is stated in coupling form (CouplingConverges): a Skorokhod representation with almost-sure uniform convergence on compact intervals. Convergence to a deterministic path is uniform convergence on compacts in probability (UocInProb). Xn(0)⇒νX_n(0) \Rightarrow \nuXn​(0)⇒ν is stated with bounded continuous test functions.
  • The OU process is the published Erlang-A diffusion with β=0\beta = 0β=0 and θ=μ\theta = \muθ=μ, whose drift is −μx-\mu x−μx. A solution has X(0)∼νX(0) \sim \nuX(0)∼ν independent of BBB and is adapted to σ(X(0))∨σ(B(s):s≤t)\sigma(X(0)) \vee \sigma(B(s) : s \le t)σ(X(0))∨σ(B(s):s≤t). The goal asserts existence and that every solution is a limit, which carries uniqueness in law. The limit space is in universe Type.
  • Predictable quadratic variation is a property, since Mathlib has no Doob–Meyer theorem: MMM is square integrable, VVV is adapted, continuous (the paper's "predictable", p. 208), nondecreasing and integrable, and M2−VM^2 - VM2−V is a martingale. Optional quadratic variations [M][M][M] are not stated.
  • Filtrations. The filtration of Theorem 3.4 is the generated history augmented by the measurable null sets.
  • Norms and suprema. The norm on Rk\mathbb R^kRk is ℓ1\ell^1ℓ1, and suprema of paths are taken in [0,∞][0, \infty][0,∞].
  • Added hypotheses. The statements add three things the printed versions need: Mn(0)=0M_n(0) = 0Mn​(0)=0 in Lemma 5.8 (without it the lemma is false), SSS an F\mathbf FF-Poisson process and I(0)=0I(0) = 0I(0)=0 in Lemma 3.2, and integrability of ggg in Lemma 4.1.
  • Not formalized. Theorem 4.1(ii) (J1J_1J1​ continuity) and the birth-and-death clause of Lemma 2.1.

A formalization that fixes Qn(0)=nQ_n(0) = nQn​(0)=n, assumes Xn(0)X_n(0)Xn​(0) converges almost surely, adds E[Qn(0)]<∞E[Q_n(0)] < \inftyE[Qn​(0)]<∞ to the goal, or replaces convergence in DDD by convergence of finite-dimensional distributions proves a weaker theorem and does not close the goal.

Contributions are welcome at every level. The Poisson FCLT, Lenglart's inequality and the composition map are reusable library results, independent of queueing.

Selected references

  • G. Pang, R. Talreja, W. Whitt, Martingale Proofs of Many-Server Heavy-Traffic Limits for Markovian Queues, Probability Surveys 4 (2007) 193–267. https://arxiv.org/abs/0712.4211 (doi:10.1214/06-PS091)
  • D. L. Iglehart, Limit diffusion approximations for the many server queue and the repairman problem, J. Appl. Prob. 2 (1965) 429–441. https://mathscinet.ams.org/mathscinet-getitem?mr=0184302
  • S. Halfin, W. Whitt, Heavy-traffic limits for queues with many exponential servers, Oper. Res. 29 (1981) 567–588. https://mathscinet.ams.org/mathscinet-getitem?mr=0629195
  • A. Mandelbaum, W. A. Massey, M. I. Reiman, Strong approximations for Markovian service networks, Queueing Systems 30 (1998) 149–201. https://mathscinet.ams.org/mathscinet-getitem?mr=1663767
  • E. V. Krichagina, A. A. Puhalskii, A heavy-traffic analysis of a closed queueing system with a GI/∞ service center, Queueing Systems 25 (1997) 235–280. https://mathscinet.ams.org/mathscinet-getitem?mr=1458591
  • S. N. Ethier, T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. https://mathscinet.ams.org/mathscinet-getitem?mr=0838085
23 thms1 active userReviewed
Operations ResearchProbability·Captain: mikedeng1

Martingale Proofs of Many-Server Heavy-Traffic Limits for Markovian Queues 2: In the QED Regime the Scaled M/M/n/mₙ+M Queue Converges to a Diffusion Reflected at the Upper Barrier κResearch Paper

Motivation

Large service systems such as call centers, hospital wards and cloud server pools have many parallel servers, finite buffers and customers who leave when they wait too long. Their performance is usually analysed through heavy-traffic diffusion limits: the number of customers in the system, centred and rescaled, converges as the system grows to a diffusion process whose law is computable. The quality-and-efficiency-driven (QED) regime of Halfin and Whitt (Oper. Res. 29, 1981) is the scaling in which the number of servers nnn and the arrival rate grow together so that the probability of delay stays strictly between 000 and 111. Garnett, Mandelbaum and Reiman (M&SOM 4, 2002) proved the QED limit for the Erlang-A model with unlimited waiting room. Whitt (Math. Oper. Res. 30, 2005) added finite waiting rooms of size of order n\sqrt nn​, which produce a reflecting upper barrier in the limit.

Pang, Talreja and Whitt (Probab. Surveys 4, 2007) give a self-contained martingale proof of these limits. Theorem 1.2 of that paper, the target of this mission, covers the M/M/n/mn+MM/M/n/m_n+MM/M/n/mn​+M model with finite waiting room and abandonment. It contains the Erlang-B (loss) model (mn=0m_n=0mn​=0) and finite-buffer Erlang-C models (θ=0\theta=0θ=0) as special cases.

Setting

Fix a service rate μ>0\mu>0μ>0, an abandonment rate θ≥0\theta\ge 0θ≥0, a constant β∈R\beta\in\mathbb Rβ∈R and a barrier κ≥0\kappa\ge 0κ≥0. For n≥1n\ge 1n≥1, model nnn is an M/M/n/mn+MM/M/n/m_n+MM/M/n/mn​+M queue: nnn servers, a waiting room of mn∈{0,1,2,… }m_n\in\{0,1,2,\dots\}mn​∈{0,1,2,…} places, Poisson arrivals of rate λn\lambda_nλn​, exponential services of rate μ\muμ, first-come first-served service, and an exponential patience of rate θ\thetaθ for each waiting customer. An arrival that finds all n+mnn+m_nn+mn​ places occupied is blocked and lost.

The number in system Qn(t)Q_n(t)Qn​(t) is constructed from independent rate-1 Poisson processes AAA, SSS, RRR and an independent initial value Qn(0)≤n+mnQ_n(0)\le n+m_nQn​(0)≤n+mn​ by

Qn(t)=Qn(0)+A(λnt)−S(μ ⁣∫0t(Qn(s)∧n) ds)−R(θ ⁣∫0t(Qn(s)−n)+ds)−Un(t),Q_n(t)=Q_n(0)+A(\lambda_n t)-S\Big(\mu\!\int_0^t (Q_n(s)\wedge n)\,ds\Big)-R\Big(\theta\!\int_0^t (Q_n(s)-n)^+ds\Big)-U_n(t),Qn​(t)=Qn​(0)+A(λn​t)−S(μ∫0t​(Qn​(s)∧n)ds)−R(θ∫0t​(Qn​(s)−n)+ds)−Un​(t),

where Un(t)=∫(0,t]1{Qn(s−)=n+mn} dA(λns)U_n(t)=\int_{(0,t]}\mathbf 1\{Q_n(s-)=n+m_n\}\,dA(\lambda_n s)Un​(t)=∫(0,t]​1{Qn​(s−)=n+mn​}dA(λn​s) counts blocked arrivals. The QED scaling is

nμ−λnn→βμ,mnn→κ,\frac{n\mu-\lambda_n}{\sqrt n}\to\beta\mu,\qquad \frac{m_n}{\sqrt n}\to\kappa,n​nμ−λn​​→βμ,n​mn​​→κ,

and the scaled process is Xn(t)=(Qn(t)−n)/nX_n(t)=(Q_n(t)-n)/\sqrt nXn​(t)=(Qn​(t)−n)/n​.

The limit is a reflected diffusion: a pair (X,U)(X,U)(X,U) of processes with right-continuous paths with left limits, X≤κX\le\kappaX≤κ, UUU nondecreasing and nonnegative, a standard Brownian motion BBB independent of X(0)X(0)X(0), and

X(t)=X(0)−βμt+2μ B(t)−∫0t[μ(X(s)∧0)+θ(X(s)∨0)]ds−U(t),∫0∞1{X(t)<κ} dU(t)=0.X(t)=X(0)-\beta\mu t+\sqrt{2\mu}\,B(t)-\int_0^t\big[\mu(X(s)\wedge0)+\theta(X(s)\vee0)\big]ds-U(t),\qquad \int_0^\infty\mathbf 1\{X(t)<\kappa\}\,dU(t)=0 .X(t)=X(0)−βμt+2μ​B(t)−∫0t​[μ(X(s)∧0)+θ(X(s)∨0)]ds−U(t),∫0∞​1{X(t)<κ}dU(t)=0.

The regulator UUU increases only when XXX sits at κ\kappaκ.

Formalization targets

Goal: Theorem 1.2

If Xn(0)⇒νX_n(0)\Rightarrow\nuXn​(0)⇒ν in R\mathbb RR, then Xn⇒XX_n\Rightarrow XXn​⇒X in DDD, where XXX solves the reflected equation above with X(0)∼νX(0)\sim\nuX(0)∼ν, and every solution with initial law ν\nuν has the same law:

Xn⇒Xin D[0,∞)(n→∞).X_n\Rightarrow X\quad\text{in } D[0,\infty)\qquad (n\to\infty).Xn​⇒Xin D[0,∞)(n→∞).

The goal fixes no rate of convergence and no stationary quantity; it asserts the process limit and its characterization by (9)–(10).

Milestones

  1. Theorem 7.4: the martingale representation of XnX_nXn​ as Xn(0)X_n(0)Xn​(0) plus scaled Poisson martingales Mn,iM_{n,i}Mn,i​, a drift term, a Lipschitz feedback term and the scaled blocking process Vn=Un/nV_n=U_n/\sqrt nVn​=Un​/n​, with the predictable quadratic variations of the Mn,iM_{n,i}Mn,i​.
  2. (110): the limit noise B1(μt)−B2(μt)−B3(0)B_1(\mu t)-B_2(\mu t)-B_3(0)B1​(μt)−B2​(μt)−B3​(0) of three independent Brownian motions has the law of 2μ B\sqrt{2\mu}\,B2μ​B.
  3. Theorem 7.3 (i): the deterministic reflected integral equation x=b+y+∫0⋅h(x) ds−ux=b+y+\int_0^\cdot h(x)\,ds-ux=b+y+∫0⋅​h(x)ds−u with barrier κ\kappaκ and Lipschitz hhh has a unique solution, depending continuously on (y,b)(y,b)(y,b) for uniform convergence on bounded intervals, and continuous when yyy is.

Significance

The theorem supplies the diffusion approximation behind square-root staffing rules for systems with finite buffers: it says that buffers of order n\sqrt nn​ are visible in the limit as a barrier at κ\kappaκ, and that the limit for κ=0\kappa=0κ=0 (Erlang-B with or without abandonment) is a reflected Ornstein–Uhlenbeck-type process. Stationary blocking and delay probabilities of the limit then approximate those of the large finite system.

The result is proved in the literature (Whitt 2005; Pang, Talreja and Whitt 2007, whose proof of Theorem 1.2 is a sketch built on §7.1). It is not formalized anywhere. A formal proof would supply a checked martingale representation for a birth–death queue with blocking, a checked reflection map with state-dependent drift, and the continuous-mapping step through it. The unlimited-waiting-room case is posed separately on the platform as the Erlang-A limit of Garnett, Mandelbaum and Reiman and is not part of this mission.

Difficulty

The obvious route is the one used for the Erlang-A model: write XnX_nXn​ as a continuous function of the scaled Poisson noise and apply the continuous-mapping theorem. With a finite waiting room this fails as stated, because the blocking process UnU_nUn​ is not a function of the noise alone. It depends on the path of QnQ_nQn​ through the times the system is full. The proof must instead identify (Xn,Vn)(X_n,V_n)(Xn​,Vn​) as the image of the noise under a reflection map with a drift inside it, prove that this map is well defined and continuous, and control the martingale terms through random time changes whose limits are deterministic. The barrier in model nnn is mn/nm_n/\sqrt nmn​/n​, not κ\kappaκ, so the continuous-mapping step has to handle a moving barrier as well.

Formalization scope

  • Paths. Time is real; every path is a function on R\mathbb RR of which only the values at t≥0t\ge0t≥0 are used. "In DDD" is BellWilliams2001.ThresholdPolicy.IsCadlag. Brownian motion is ErlangA.Diffusion.IsStandardBM, indexed by R≥0\mathbb R_{\ge0}R≥0​; martingales are Mathlib Martingales indexed by R≥0\mathbb R_{\ge0}R≥0​.
  • Model. All systems live on one probability space with their own primitives An,Sn,RnA_n,S_n,R_nAn​,Sn​,Rn​; Poisson processes are ManyServerQED.Scheduling.IsPoissonProcess. Qn(0)Q_n(0)Qn​(0) is independent of the primitives and Qn(t)≤n+mnQ_n(t)\le n+m_nQn​(t)≤n+mn​ for all t≥0t\ge0t≥0. Blocked arrivals are counted with the left limit Qn(s−)Q_n(s-)Qn​(s−), correcting (114) as printed. θ=0\theta=0θ=0 and κ=0\kappa=0κ=0 are allowed.
  • Weak convergence. Xn(0)⇒νX_n(0)\Rightarrow\nuXn​(0)⇒ν is convergence of expectations of bounded continuous functions. Xn⇒XX_n\Rightarrow XXn​⇒X in DDD is BellWilliams2001.ThresholdPolicy.CouplingConverges (Skorohod coupling with almost sure uniform convergence on compacts), equivalent to J1J_1J1​ weak convergence for a continuous limit. Uniform distances use supDist on R1\mathbb R^1R1.
  • Limit. The drift is ErlangA.Diffusion.drift; X(0)X(0)X(0) is independent of BBB; XXX and UUU are adapted to the filtration of X(0)X(0)X(0) and BBB; condition (10) is "the Lebesgue–Stieltjes measure of UUU, extended by 000 to negative times, gives zero mass to {t≥0:X(t)<κ}\{t\ge0: X(t)<\kappa\}{t≥0:X(t)<κ}". Uniqueness is uniqueness in law of XXX. The limit space lives in Type.
  • Martingales. "Predictable quadratic variation VVV" means: VVV adapted with continuous, nondecreasing, nonnegative paths and M2−VM^2-VM2−V a martingale. The filtration (118) is augmented by the measurable null sets, as the paper states.
  • Ruled out. Convergence of finite-dimensional distributions, a deterministic or almost surely convergent initial condition, a fixed barrier κ\kappaκ inside the prelimit model, or a solution concept that drops X≤κX\le\kappaX≤κ or the barrier condition (10) would each make the statement weaker or vacuous; none is used.
  • Not in scope. The Skorohod J1J_1J1​ continuity in Theorem 7.3 (ii), the Erlang-A Theorem 7.1, and the non-Markovian arrivals of §7.3.

Contributions welcome: Stieltjes-integral and counting-process lemmas for UnU_nUn​, a reflection map with Lipschitz drift on D[0,∞)D[0,\infty)D[0,∞), the Poisson functional central limit theorem, and martingale facts for randomly time-changed Poisson processes. The last three are reusable well beyond this mission.

Selected references

  • G. Pang, R. Talreja, W. Whitt, Martingale proofs of many-server heavy-traffic limits for Markovian queues, Probability Surveys 4 (2007) 193–267. https://arxiv.org/abs/0712.4211 (v1), https://doi.org/10.1214/06-PS091
  • S. Halfin, W. Whitt, Heavy-traffic limits for queues with many exponential servers, Operations Research 29 (1981) 567–588. https://doi.org/10.1287/opre.29.3.567
  • O. Garnett, A. Mandelbaum, M. Reiman, Designing a call center with impatient customers, Manufacturing & Service Operations Management 4 (2002) 208–227. https://doi.org/10.1287/msom.4.3.208.7753
  • W. Whitt, Heavy-traffic limits for the G/H2∗/n/mG/H_2^*/n/mG/H2∗​/n/m queue, Mathematics of Operations Research 30 (2005) 1–27. https://mathscinet.ams.org/mathscinet-getitem?mr=2125135
  • W. Whitt, Stochastic-Process Limits, Springer, 2002. https://doi.org/10.1007/b97479
11 thms1 active userReviewed
Control TheoryProbability·Captain: mikedeng1

Utility Maximization in Incomplete Markets II: Under Closed Constraints, the Power-Utility Value Is x^γ exp(Y₀)/γ for the Quadratic BSDE (15), and an Optimal Strategy Exists (Theorem 14)Research Paper

Motivation

An investor who trades continuously in a market driven by Brownian motion, and who may only hold portfolios in a prescribed set, wants to maximize the expected utility of terminal wealth. With power utility Uγ(x)=1γxγU_\gamma(x)=\frac1\gamma x^\gammaUγ​(x)=γ1​xγ, γ∈(0,1)\gamma\in(0,1)γ∈(0,1), this is the constant-relative-risk-aversion problem that goes back to Merton (Merton 1971). When there are fewer stocks than sources of noise the market is incomplete, and when portfolio proportions are restricted (no short sales, bounded positions, a fixed allocation) the problem is constrained.

For convex constraints, duality methods settle the problem (Cvitanić–Karatzas 1992; Kramkov–Schachermayer 1999). They do not apply when the constraint set is closed but not convex, as for integer-lot or "all-or-nothing" restrictions. Hu, Imkeller and Müller (2005, arXiv:math/0508448) treat that case by a martingale optimality principle: they build a process that is a supermartingale for every admissible strategy and a martingale for one, and obtain it from a backward stochastic differential equation (BSDE) with a driver that grows quadratically in zzz. The existence theory for such equations is due to Kobylanski (2000).

This mission formalizes the power-utility result, Theorem 14 of the paper. A companion mission treats the exponential-utility result, Theorem 7.

Setting

Fix a horizon T>0T>0T>0 and a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) carrying an mmm-dimensional Brownian motion WWW; F\mathbb FF is the augmentation of its natural filtration. ∣⋅∣|\cdot|∣⋅∣ is the Euclidean norm, and λ\lambdaλ is Lebesgue measure on [0,T][0,T][0,T].

Market. There is a bond with zero interest and d≤md\le md≤m stocks with prices dSti/Sti=bti dt+σti dWtdS^i_t/S^i_t=b^i_t\,dt+\sigma^i_t\,dW_tdSti​/Sti​=bti​dt+σti​dWt​. The rates bt∈Rdb_t\in\mathbb R^dbt​∈Rd and the volatility σt∈Rd×m\sigma_t\in\mathbb R^{d\times m}σt​∈Rd×m are predictable and uniformly bounded, and KId≥σtσttr≥εIdKI_d\ge\sigma_t\sigma_t^{\mathrm{tr}}\ge\varepsilon I_dKId​≥σt​σttr​≥εId​ for constants K>ε>0K>\varepsilon>0K>ε>0. The market price of risk is θt=σttr(σtσttr)−1bt∈Rm\theta_t=\sigma_t^{\mathrm{tr}}(\sigma_t\sigma_t^{\mathrm{tr}})^{-1}b_t\in\mathbb R^mθt​=σttr​(σt​σttr​)−1bt​∈Rm.

Constraints. A closed set C~⊆R1×d\tilde C\subseteq\mathbb R^{1\times d}C~⊆R1×d of row vectors constrains the proportions ρ~t\tilde\rho_tρ~​t​ of wealth held in the stocks. In the variable ρt=ρ~tσt∈R1×m\rho_t=\tilde\rho_t\sigma_t\in\mathbb R^{1\times m}ρt​=ρ~​t​σt​∈R1×m the constraint reads ρt∈Ct(ω)=C~σt(ω)\rho_t\in C_t(\omega)=\tilde C\sigma_t(\omega)ρt​∈Ct​(ω)=C~σt​(ω). For a closed C⊆RmC\subseteq\mathbb R^mC⊆Rm, dist⁡C(a)=min⁡b∈C∣a−b∣\operatorname{dist}_C(a)=\min_{b\in C}|a-b|distC​(a)=minb∈C​∣a−b∣, and ΠC(a)={b∈C:∣a−b∣=dist⁡C(a)}\Pi_C(a)=\{b\in C:|a-b|=\operatorname{dist}_C(a)\}ΠC​(a)={b∈C:∣a−b∣=distC​(a)} is the (possibly multi-valued) projection.

Wealth and admissible strategies. From initial capital x>0x>0x>0 the wealth (11) is

Xt(ρ)=xexp⁡(∫0tρs dWs+∫0tρsθs ds−12∫0t∣ρs∣2 ds).X^{(\rho)}_t=x\exp\Big(\int_0^t\rho_s\,dW_s+\int_0^t\rho_s\theta_s\,ds-\tfrac12\int_0^t|\rho_s|^2\,ds\Big).Xt(ρ)​=xexp(∫0t​ρs​dWs​+∫0t​ρs​θs​ds−21​∫0t​∣ρs​∣2ds).

The admissible class A~\tilde{\mathcal A}A~ (Definition 13) consists of predictable ρ\rhoρ with ρt∈Ct\rho_t\in C_tρt​∈Ct​ for λ⊗P\lambda\otimes Pλ⊗P-a.e. (t,ω)(t,\omega)(t,ω) and ∫0T∣ρs∣2 ds<∞\int_0^T|\rho_s|^2\,ds<\infty∫0T​∣ρs​∣2ds<∞ a.s. The value is (12), Vˉ(x)=sup⁡ρ∈A~E[Uγ(XT(ρ))]\bar V(x)=\sup_{\rho\in\tilde{\mathcal A}}E[U_\gamma(X^{(\rho)}_T)]Vˉ(x)=supρ∈A~​E[Uγ​(XT(ρ)​)].

The BSDE. H∞(R)\mathcal H^\infty(\mathbb R)H∞(R) is the class of predictable, λ⊗P\lambda\otimes Pλ⊗P-a.e. bounded processes and H2(Rm)\mathcal H^2(\mathbb R^m)H2(Rm) that of predictable ZZZ with E∫0T∣Zt∣2 dt<∞E\int_0^T|Z_t|^2\,dt<\inftyE∫0T​∣Zt​∣2dt<∞. The BSDE (15) is

Yt=0−∫tTZs dWs−∫tTf(s,Zs) ds,f(t,z)=γ(1−γ)2dist⁡2(z+θt1−γ,Ct)−γ∣z+θt∣22(1−γ)−12∣z∣2.Y_t=0-\int_t^TZ_s\,dW_s-\int_t^Tf(s,Z_s)\,ds,\qquad f(t,z)=\frac{\gamma(1-\gamma)}2\operatorname{dist}^2\Big(\frac{z+\theta_t}{1-\gamma},C_t\Big)-\frac{\gamma|z+\theta_t|^2}{2(1-\gamma)}-\frac12|z|^2 .Yt​=0−∫tT​Zs​dWs​−∫tT​f(s,Zs​)ds,f(t,z)=2γ(1−γ)​dist2(1−γz+θt​​,Ct​)−2(1−γ)γ∣z+θt​∣2​−21​∣z∣2.

A BMO martingale ∫0⋅ξ dW\int_0^\cdot\xi\,dW∫0⋅​ξdW is one with sup⁡τ∥E[∫τT∣ξs∣2ds∣Fτ]∥∞<∞\sup_\tau\|E[\int_\tau^T|\xi_s|^2ds\mid\mathcal F_\tau]\|_\infty<\inftysupτ​∥E[∫τT​∣ξs​∣2ds∣Fτ​]∥∞​<∞ over stopping times τ≤T\tau\le Tτ≤T (equation (2)).

Formalization targets

Goal: Theorem 14

(15) has a unique solution (Y,Z)∈H∞(R)×H2(Rm)(Y,Z)\in\mathcal H^\infty(\mathbb R)\times\mathcal H^2(\mathbb R^m)(Y,Z)∈H∞(R)×H2(Rm), and for x>0x>0x>0

Vˉ(x)=1γ xγexp⁡(Y0),\bar V(x)=\frac1\gamma\,x^\gamma\exp(Y_0),Vˉ(x)=γ1​xγexp(Y0​),

attained by some ρ∗∈A~\rho^*\in\tilde{\mathcal A}ρ∗∈A~ with

ρt∗∈ΠCt(ω)(11−γ(Zt+θt)).(16)\rho^*_t\in\Pi_{C_t(\omega)}\Big(\frac1{1-\gamma}(Z_t+\theta_t)\Big).\qquad(16)ρt∗​∈ΠCt​(ω)​(1−γ1​(Zt​+θt​)).(16)

The page prints V(x)=xγexp⁡(Y0)V(x)=x^\gamma\exp(Y_0)V(x)=xγexp(Y0​); its proof measures utility by xγx^\gammaxγ, so the value of (12) with Uγ=1γxγU_\gamma=\frac1\gamma x^\gammaUγ​=γ1​xγ carries the factor 1γ\frac1\gammaγ1​ (see Formalization scope).

Milestones

  1. (14), p. 17: for ρ∈C\rho\in Cρ∈C, γρθ−12γ∣ρ∣2+f(z)≤−12∣γρ+z∣2\gamma\rho\theta-\frac12\gamma|\rho|^2+f(z)\le-\frac12|\gamma\rho+z|^2γρθ−21​γ∣ρ∣2+f(z)≤−21​∣γρ+z∣2, with equality on ΠC(z+θ1−γ)\Pi_C\big(\frac{z+\theta}{1-\gamma}\big)ΠC​(1−γz+θ​).
  2. (H1), p. 18: ∣f(t,z)∣≤c0+c1∣z∣2|f(t,z)|\le c_0+c_1|z|^2∣f(t,z)∣≤c0​+c1​∣z∣2.
  3. Existence and 4. uniqueness for (15), p. 18.
  4. Lemma 17, p. 20: ∫Z dW\int Z\,dW∫ZdW and ∫ρ∗dW\int\rho^*dW∫ρ∗dW are BMO martingales.
  5. Optimality of ρ∗\rho^*ρ∗, p. 18: ρ∗∈A~\rho^*\in\tilde{\mathcal A}ρ∗∈A~ and E[(XT(ρ∗))γ]=xγexp⁡(Y0)E[(X^{(\rho^*)}_T)^\gamma]=x^\gamma\exp(Y_0)E[(XT(ρ∗)​)γ]=xγexp(Y0​).
  6. Comparison, p. 18: E[(XT(ρ))γ]≤xγexp⁡(Y0)E[(X^{(\rho)}_T)^\gamma]\le x^\gamma\exp(Y_0)E[(XT(ρ)​)γ]≤xγexp(Y0​) for every ρ∈A~\rho\in\tilde{\mathcal A}ρ∈A~.

Significance

The theorem gives the value of a constrained power-utility problem in closed form through one scalar, Y0Y_0Y0​, of a BSDE, and identifies an optimal strategy as a measurable selection of a projection onto the constraint set. Convexity of the constraint is not needed; when C~\tilde CC~ is a convex cone the result recovers the strategy obtained by other methods (Remark 16 of the paper). The same scheme handles exponential and logarithmic utility in the paper's other sections, and the dynamic programming principle of Proposition 15 follows from it.

The result is proved in the paper. As far as the platform's records show, none of it is formalized: there is no quadratic BSDE, no BMO martingale and no continuous-time utility-maximization statement on the platform. A complete formalization would add an existence and uniqueness theory for BSDEs with quadratic growth, the BMO criterion for stochastic exponentials, and a verification theorem for constrained portfolio problems, each reusable well beyond this paper.

Difficulty

The verification argument is short on paper; its inputs are not. Existence for (15) rests on Kobylanski's existence theorem for drivers of quadratic growth, which is not in Mathlib; the Lipschitz theory does not cover a driver growing like ∣z∣2|z|^2∣z∣2. Uniqueness needs a comparison principle for such drivers. Lemma 17 and the martingale property of R~(ρ∗)\tilde R^{(\rho^*)}R~(ρ∗) need the theory of BMO martingales and of their stochastic exponentials, also absent. The comparison milestone concerns processes that are only local supermartingales. A naive attempt that treats R~(ρ)\tilde R^{(\rho)}R~(ρ) as a martingale for every admissible ρ\rhoρ fails: for a general ρ∈A~\rho\in\tilde{\mathcal A}ρ∈A~, which is only locally square integrable, it is merely a local supermartingale.

Formalization scope

All declarations live in HuImkellerMuller.Power. Time is ℝ≥0; vectors of R1×m\mathbb R^{1\times m}R1×m are EuclideanSpace ℝ (Fin m), with products zθz\thetazθ as inner products; C~\tilde CC~ is a Set (Fin d → ℝ). The Brownian motion, the augmented filtration, the measure λ⊗P\lambda\otimes Pλ⊗P and the Itô-integral operator I are reused from published definitions (EthierKurtz_IsStandardBrownian, CvitanicKaratzas92_Optimality_Market). The wealth is constructed from I, ρ\rhoρ and θ\thetaθ; θ\thetaθ is computed from bbb and σ\sigmaσ.

Conventions and disclosed readings:

  • The factor 1γ\frac1\gammaγ1​. The goal states Vˉ(x)=1γxγexp⁡(Y0)\bar V(x)=\frac1\gamma x^\gamma\exp(Y_0)Vˉ(x)=γ1​xγexp(Y0​) for (12) with UγU_\gammaUγ​; milestones 6–7 state E[(XT)γ]E[(X_T)^\gamma]E[(XT​)γ] against xγexp⁡(Y0)x^\gamma\exp(Y_0)xγexp(Y0​), as the proof does.
  • Added hypothesis C~≠∅\tilde C\neq\emptysetC~=∅ (needed for (4) and for ΠCt≠∅\Pi_{C_t}\neq\emptysetΠCt​​=∅).
  • Strategies are written in ρ=ρ~σ∈Rm\rho=\tilde\rho\sigma\in\mathbb R^mρ=ρ~​σ∈Rm (Definition 13 says "ddd-dimensional"); §3's "Cˉ2⊆Rd\bar C_2\subseteq\mathbb R^dCˉ2​⊆Rd" and C~\tilde CC~ are one closed set.
  • (16) and the constraint hold λ⊗P\lambda\otimes Pλ⊗P-a.e.; "ρ∗\rho^*ρ∗ given by (16)" means any predictable selection.
  • Y0Y_0Y0​ is a.s. constant; the value identity holds for PPP-a.e. ω\omegaω.
  • Uniqueness means Yt1=Yt2Y^1_t=Y^2_tYt1​=Yt2​ a.s. for every ttt and Z1=Z2Z^1=Z^2Z1=Z2 λ⊗P\lambda\otimes Pλ⊗P-a.e.
  • Expectations of nonnegative quantities are lower integrals in [0,∞][0,\infty][0,∞]; the value is a supremum in [0,∞][0,\infty][0,∞].
  • Ellipticity holds for PPP-a.e. ω\omegaω and every t≤Tt\le Tt≤T; boundedness of bbb, σ\sigmaσ holds everywhere.

The value is a supremum of lower integrals, never of Bochner integrals: a Bochner expectation of a non-integrable Uγ(XT)U_\gamma(X_T)Uγ​(XT​) is 000 and would make the supremum meaningless. The goal asserts existence of a solution of (15) and does not take one as a hypothesis, so it cannot hold vacuously.

Contributions welcome: a theory of BSDEs with quadratic growth (Kobylanski), BMO martingales and Kazamaki's criterion, measurable selection of metric projections, and proofs of the deterministic milestone (14) and the growth bound (H1).

Selected references

  • Y. Hu, P. Imkeller, M. Müller, Utility maximization in incomplete markets, Ann. Appl. Probab. 15(3), 2005, 1691–1712. https://doi.org/10.1214/105051605000000188 (arXiv:math/0508448v1, https://arxiv.org/abs/math/0508448)
  • M. Kobylanski, Backward stochastic differential equations and partial differential equations with quadratic growth, Ann. Probab. 28(2), 2000, 558–602. https://doi.org/10.1214/aop/1019160253
  • N. Kazamaki, Continuous Exponential Martingales and BMO, Lecture Notes in Math. 1579, Springer, 1994. https://doi.org/10.1007/BFb0073585
  • J. Cvitanić, I. Karatzas, Convex duality in constrained portfolio optimization, Ann. Appl. Probab. 2(4), 1992, 767–818. https://doi.org/10.1214/aoap/1177005576
  • D. Kramkov, W. Schachermayer, The asymptotic elasticity of utility functions and optimal investment in incomplete markets, Ann. Appl. Probab. 9(3), 1999, 904–950. https://doi.org/10.1214/aoap/1029962818
  • R. C. Merton, Optimum consumption and portfolio rules in a continuous-time model, J. Econom. Theory 3, 1971, 373–413. https://doi.org/10.1016/0022-0531(71)90038-X
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Control TheoryProbability·Captain: mikedeng1

Utility Maximization in Incomplete Markets I: Under Closed Constraints, the Exponential-Utility Value Is −exp(−α(x − Y₀)) for the Quadratic BSDE (7), and an Optimal Strategy Exists (Theorem 7)Research Paper

Motivation

An investor who trades in a market with fewer stocks than sources of randomness cannot hedge every risk: the market is incomplete. If the investor also faces a liability FFF due at the horizon TTT and has to respect trading constraints (no short sales, limits on positions in certain stocks, a ban on trading some assets altogether), the question of how to trade optimally becomes a constrained stochastic control problem. With exponential utility U(x)=−exp⁡(−αx)U(x)=-\exp(-\alpha x)U(x)=−exp(−αx), its value function gives the investor's utility indifference price of FFF, a standard pricing rule in incomplete markets.

Earlier treatments needed convexity. Cvitanić and Karatzas (Ann. Appl. Probab. 2 (1992)) proved existence and uniqueness for utility maximization in a Brownian filtration with convex constraints, by convex duality. Delbaen, Grandits, Rheinländer, Samperi, Schweizer and Stricker (Math. Finance 12 (2002)) related exponential utility maximization to the martingale measure of minimal relative entropy. El Karoui and Rouge (Math. Finance 10 (2000)) computed the value function and optimal strategy for exponential utility by backward stochastic differential equations (BSDEs), for strategies confined to a convex cone; Sekine (preprint, 2002) obtained the same BSDE from the Cvitanić–Karatzas duality. Hu, Imkeller and Müller (Ann. Appl. Probab. 15 (2005)) gave a direct BSDE solution that works for closed, possibly nonconvex constraint sets, with a bounded liability. The tool is a BSDE whose driver grows quadratically in the control variable, whose solvability rests on Kobylanski's existence theorem for quadratic BSDEs (Ann. Probab. 28 (2000)).

Setting

Fix T>0T>0T>0 and an mmm-dimensional Brownian motion WWW on a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P), and let F=(Ft)\mathbb F=(\mathcal F_t)F=(Ft​) be the PPP-augmentation of the filtration generated by WWW. There are d≤md\le md≤m stocks with prices dSti/Sti=bti dt+σti dWtdS^i_t/S^i_t=b^i_t\,dt+\sigma^i_t\,dW_tdSti​/Sti​=bti​dt+σti​dWt​; the drift bbb and the d×md\times md×m volatility matrix σ\sigmaσ are predictable and uniformly bounded, and KId≥σσtr≥εIdKI_d\ge\sigma\sigma^{\mathrm{tr}}\ge\varepsilon I_dKId​≥σσtr≥εId​ for constants K>ε>0K>\varepsilon>0K>ε>0. The market price of risk is θt=σttr(σtσttr)−1bt∈Rm\theta_t=\sigma^{\mathrm{tr}}_t(\sigma_t\sigma^{\mathrm{tr}}_t)^{-1}b_t\in\mathbb R^mθt​=σttr​(σt​σttr​)−1bt​∈Rm.

A strategy is an R1×m\mathbb R^{1\times m}R1×m-valued predictable process pt=πtσtp_t=\pi_t\sigma_tpt​=πt​σt​, where πt\pi_tπt​ is the vector of amounts held in the stocks. Its wealth from initial capital xxx is

Xt(p)=x+∫0tpu (dWu+θu du).X^{(p)}_t=x+\int_0^tp_u\,(dW_u+\theta_u\,du).Xt(p)​=x+∫0t​pu​(dWu​+θu​du).

The constraint is a closed set C~⊆R1×d\tilde C\subseteq\mathbb R^{1\times d}C~⊆R1×d, not necessarily convex; in terms of ppp it reads pt∈Ct:=C~σtp_t\in C_t:=\tilde C\sigma_tpt​∈Ct​:=C~σt​. A strategy is admissible, p∈Ap\in\mathcal Ap∈A, when E∫0T∣pt∣2dt<∞E\int_0^T|p_t|^2dt<\inftyE∫0T​∣pt​∣2dt<∞, pt∈Ctp_t\in C_tpt​∈Ct​ for λ⊗P\lambda\otimes Pλ⊗P-a.e. (t,ω)(t,\omega)(t,ω), and {exp⁡(−αXτ(p)):τ≤T a stopping time}\{\exp(-\alpha X^{(p)}_\tau):\tau\le T\text{ a stopping time}\}{exp(−αXτ(p)​):τ≤T a stopping time} is uniformly integrable. The value function is

V(x)=sup⁡p∈AE[−exp⁡(−α(XT(p)−F))],V(x)=\sup_{p\in\mathcal A}E\Big[-\exp\Big(-\alpha\big(X^{(p)}_T-F\big)\Big)\Big],V(x)=p∈Asup​E[−exp(−α(XT(p)​−F))],

with α>0\alpha>0α>0 and a bounded FT\mathcal F_TFT​-measurable liability FFF. For a closed set CCC, dist⁡C(a)=min⁡b∈C∣a−b∣\operatorname{dist}_C(a)=\min_{b\in C}|a-b|distC​(a)=minb∈C​∣a−b∣ and ΠC(a)={b∈C:∣a−b∣=dist⁡C(a)}\Pi_C(a)=\{b\in C:|a-b|=\operatorname{dist}_C(a)\}ΠC​(a)={b∈C:∣a−b∣=distC​(a)} is the set of nearest points.

Formalization targets

Goal: Theorem 7

Let f(t,z)=−α2dist⁡2(z+1αθt,Ct)+zθt+12α∣θt∣2f(t,z)=-\frac\alpha2\operatorname{dist}^2\big(z+\frac1\alpha\theta_t,C_t\big)+z\theta_t+\frac1{2\alpha}|\theta_t|^2f(t,z)=−2α​dist2(z+α1​θt​,Ct​)+zθt​+2α1​∣θt​∣2. The BSDE

Yt=F−∫tTZs dWs−∫tTf(s,Zs) ds,t∈[0,T],Y_t=F-\int_t^TZ_s\,dW_s-\int_t^Tf(s,Z_s)\,ds,\qquad t\in[0,T],Yt​=F−∫tT​Zs​dWs​−∫tT​f(s,Zs​)ds,t∈[0,T],

has a unique solution (Y,Z)∈H∞(R)×H2(Rm)(Y,Z)\in\mathcal H^\infty(\mathbb R)\times\mathcal H^2(\mathbb R^m)(Y,Z)∈H∞(R)×H2(Rm), the value function is

V(x)=−exp⁡(−α(x−Y0)),V(x)=-\exp\big(-\alpha(x-Y_0)\big),V(x)=−exp(−α(x−Y0​)),

and there is an optimal strategy p∗∈Ap^*\in\mathcal Ap∗∈A with pt∗∈ΠCt(Zt+1αθt)p^*_t\in\Pi_{C_t}\big(Z_t+\frac1\alpha\theta_t\big)pt∗​∈ΠCt​​(Zt​+α1​θt​).

Milestones

In the order of the proof: the bound (4) on CtC_tCt​ and its closedness; the measurable selection Lemma 11 (a), (b); the identity on p. 8 that dictates fff; the growth bound (9) and the local Lipschitz estimate of fff; existence and uniqueness for (7); the BMO property of Lemma 12; admissibility and optimality of any predictable selection p∗p^*p∗; and the comparison E[−exp⁡(−α(XT(p)−F))]≤−exp⁡(−α(x−Y0))E[-\exp(-\alpha(X^{(p)}_T-F))]\le-\exp(-\alpha(x-Y_0))E[−exp(−α(XT(p)​−F))]≤−exp(−α(x−Y0​)) for every p∈Ap\in\mathcal Ap∈A.

Significance

The theorem reduces a constrained, nonconvex control problem to a single quadratic BSDE: the value is read off the initial value Y0Y_0Y0​, and the optimal strategy is a pointwise nearest-point selection from the constraint set. It requires neither convexity nor duality, and it exhibits non-uniqueness of the optimal strategy when ΠCt\Pi_{C_t}ΠCt​​ has several points. It is the starting point of the quadratic-BSDE approach to utility maximization, indifference pricing and related equilibrium problems.

The result is proved in the paper; nothing in it is open. As far as is known, none of it is formalized: Mathlib has no stochastic integral against Brownian motion, no BSDE theory and no BMO martingales. A complete development would be the first machine-checked solution of a continuous-time portfolio optimization problem by BSDE methods, and its intermediate results (measurable selection of nearest points, the BMO bound for quadratic BSDEs, the verification argument) are reusable.

Difficulty

The deterministic steps (the identity behind the choice of fff, the growth and Lipschitz bounds) are short. The hard steps are elsewhere. Existence rests on Kobylanski's theorem for BSDEs with quadratic growth, whose proof is a monotone approximation argument with exponential transforms; the Lipschitz theory of Pardoux–Peng does not apply. Uniqueness and the optimality of p∗p^*p∗ need the BMO property of ∫Z dW\int Z\,dW∫ZdW and a Girsanov change of measure with a stochastic exponential of a BMO martingale. The selection Lemma 11 (b) cannot use a projection map because C~\tilde CC~ is not convex; a measurable choice from a possibly multivalued nearest-point set is required. Finally the verification argument is a localization: R(p)R^{(p)}R(p) is only a local supermartingale, and passing to the limit uses the uniform integrability built into admissibility.

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​ with T>0T>0T>0; row vectors of R1×m\mathbb R^{1\times m}R1×m are EuclideanSpace ℝ (Fin m) (so ∣⋅∣|\cdot|∣⋅∣ is Euclidean) and products such as zθz\thetazθ are inner products. The Brownian motion is the published EthierKurtz.IsStandardBrownian; the filtration and the stochastic integral come from the published module CvitanicKaratzas92_Optimality_Market (IsAugmentedBrownianFiltration, lebP for λ⊗P\lambda\otimes Pλ⊗P, and an Itô-integral operator I). Predictability is measurability for Mathlib's Filtration.predictable. The market price of risk θ\thetaθ and the wealth X(p)X^{(p)}X(p) are computed from the data, not assumed.

Expectations of −exp⁡(⋅)-\exp(\cdot)−exp(⋅) are minus lower integrals in [0,∞][0,\infty][0,∞], and V(x)V(x)V(x) is an extended real: a Bochner expectation would assign the junk value 000 to non-integrable strategies and make them optimal, which is the trivializing formalization to avoid. Existence and uniqueness of the BSDE solution are part of the goal, not hypotheses, and the optimal strategy is a predictable selection of the nearest-point set, not of a choice function.

Disclosed readings: C~≠∅\tilde C\neq\emptysetC~=∅ is assumed (otherwise A=∅\mathcal A=\emptysetA=∅); constraints and (8) are read λ⊗P\lambda\otimes Pλ⊗P-a.e.; ellipticity holds for PPP-a.e. ω\omegaω and all t≤Tt\le Tt≤T; Y0Y_0Y0​ is a.s. constant and the value identity holds a.s.; uniqueness is in YtY_tYt​ a.s. for each ttt and ZZZ λ⊗P\lambda\otimes Pλ⊗P-a.e.; "p∗p^*p∗ given by Lemma 11" is read as any predictable selection; Lemma 11 (b) assumes full rank of σt(ω)\sigma_t(\omega)σt​(ω). The equivalence of the π\piπ- and ppp-formulations (Remark 5), the dynamic principle (Proposition 9) and Remarks 2–10 are out of scope.

Needed infrastructure: Itô calculus for continuous semimartingales, stochastic exponentials, BMO martingales and Kazamaki's criterion, Girsanov's theorem, quadratic BSDEs, and measurable selection. Contributions to any of these are welcome; they serve the companion power-utility mission (Theorem 14) as well.

Selected references

  • Y. Hu, P. Imkeller, M. Müller, Utility maximization in incomplete markets, Ann. Appl. Probab. 15(3), 1691–1712, 2005. https://doi.org/10.1214/105051605000000188 (arXiv: https://arxiv.org/abs/math/0508448)
  • M. Kobylanski, Backward stochastic differential equations and partial differential equations with quadratic growth, Ann. Probab. 28(2), 558–602, 2000. https://doi.org/10.1214/aop/1019160253
  • J. Cvitanić, I. Karatzas, Convex duality in constrained portfolio optimization, Ann. Appl. Probab. 2(4), 767–818, 1992. https://doi.org/10.1214/aoap/1177005576
  • E. Pardoux, S. Peng, Adapted solution of a backward stochastic differential equation, Systems Control Lett. 14(1), 55–61, 1990. https://doi.org/10.1016/0167-6911(90)90082-6
  • N. El Karoui, R. Rouge, Pricing via utility maximization and entropy, Math. Finance 10(2), 259–276, 2000. https://doi.org/10.1111/1467-9965.00093
  • F. Delbaen, P. Grandits, T. Rheinländer, D. Samperi, M. Schweizer, C. Stricker, Exponential hedging and entropic penalties, Math. Finance 12(2), 99–123, 2002. https://doi.org/10.1111/1467-9965.02001
  • N. Kazamaki, Continuous Exponential Martingales and BMO, Lecture Notes in Math. 1579, Springer, 1994. https://doi.org/10.1007/BFb0073585
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Functional AnalysisProbability·Captain: mikedeng1

Affine Processes on Positive Semidefinite Matrices II: Every Admissible Parameter Set Determines a Unique Affine Process on the PSD Cone with Generator (2.12)Research Paper

Motivation

Stochastic models of covariance matrices need processes that stay in the cone of positive semidefinite matrices. Wishart processes (Bru, 1991) and their extensions underlie multivariate stochastic-volatility and term-structure models in finance (see §1 of Cuchiero et al. for the literature). They are used because their Laplace transforms are explicit: they are exponential-affine in the initial state, and their exponents solve matrix Riccati equations. Cuchiero, Filipović, Mayerhofer and Teichmann (arXiv:0910.0137, Ann. Appl. Probab. 2011) classify all such affine processes on the cone. Theorem 2.4 of that paper says that affine processes on Sd+S_d^+Sd+​ correspond one-to-one to admissible parameter sets. This mission formalizes the converse direction of that correspondence: every admissible parameter set is realized by exactly one affine process.

Timeline:

  • Bru (1991, MR1132135) constructs Wishart processes for specific parameters.
  • Duffie, Filipović and Schachermayer (Ann. Appl. Probab. 2003, MR1994043) characterize affine processes on the canonical state space R+m×Rn\mathbb R_+^m\times\mathbb R^nR+m​×Rn, with existence through the martingale problem.
  • Cuchiero et al. (2011) give the full characterization on Sd+S_d^+Sd+​. The necessity of admissibility and the existence-and-uniqueness converse are proved in separate sections (§4 and §5).

Setting

Let SdS_dSd​ be the real symmetric d×dd\times dd×d matrices with ⟨x,y⟩=Tr⁡(xy)\langle x,y\rangle=\operatorname{Tr}(xy)⟨x,y⟩=Tr(xy), let Sd+S_d^+Sd+​ be the positive semidefinite cone, and let Sd++S_d^{++}Sd++​ be its interior. Write x⪯yx\preceq yx⪯y when y−x∈Sd+y-x\in S_d^+y−x∈Sd+​. A time-homogeneous, possibly killed Markov process on Sd+S_d^+Sd+​ with transition kernels pt(x,dξ)p_t(x,d\xi)pt​(x,dξ) is affine if it is stochastically continuous and

∫Sd+e−⟨u,ξ⟩pt(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+,\int_{S_d^+}e^{-\langle u,\xi\rangle}p_t(x,d\xi)=e^{-\varphi(t,u)-\langle\psi(t,u),x\rangle},\qquad t\ge0,\ u,x\in S_d^+,∫Sd+​​e−⟨u,ξ⟩pt​(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+​,

for functions φ≥0\varphi\ge0φ≥0 and ψ∈Sd+\psi\in S_d^+ψ∈Sd+​.

An admissible parameter set (α,b,βij,c,γ,m,μ)(\alpha,b,\beta^{ij},c,\gamma,m,\mu)(α,b,βij,c,γ,m,μ) (Definition 2.3) consists of the following:

  • a diffusion matrix α∈Sd+\alpha\in S_d^+α∈Sd+​;
  • a drift b⪰(d−1)αb\succeq(d-1)\alphab⪰(d−1)α;
  • killing rates c≥0c\ge0c≥0 and γ∈Sd+\gamma\in S_d^+γ∈Sd+​;
  • a jump measure mmm with ∫(∥ξ∥∧1) m(dξ)<∞\int(\|\xi\|\wedge1)\,m(d\xi)<\infty∫(∥ξ∥∧1)m(dξ)<∞;
  • a matrix of finite measures μ\muμ, which gives the state-dependent jump kernel M(x,dξ)=⟨x,μ(dξ)⟩/(∥ξ∥2∧1)M(x,d\xi)=\langle x,\mu(d\xi)\rangle/(\|\xi\|^2\wedge1)M(x,dξ)=⟨x,μ(dξ)⟩/(∥ξ∥2∧1);
  • linear drift coefficients βij\beta^{ij}βij, with the inward-pointing conditions (2.9) and (2.11) on ∂Sd+\partial S_d^+∂Sd+​.

These data define the operator (2.12),

Af(x)=12∑Aijkl(x)∂ij,kl2f+∑(bij+Bij(x))∂ijf−(c+⟨γ,x⟩)f+∫(f(x+ξ)−f(x))m(dξ)+∫(f(x+ξ)−f(x)−⟨χ(ξ),∇f⟩)M(x,dξ),\mathcal Af(x)=\tfrac12\sum A_{ijkl}(x)\partial^2_{ij,kl}f+\sum(b_{ij}+B_{ij}(x))\partial_{ij}f-(c+\langle\gamma,x\rangle)f+\int(f(x+\xi)-f(x))m(d\xi)+\int(f(x+\xi)-f(x)-\langle\chi(\xi),\nabla f\rangle)M(x,d\xi),Af(x)=21​∑Aijkl​(x)∂ij,kl2​f+∑(bij​+Bij​(x))∂ij​f−(c+⟨γ,x⟩)f+∫(f(x+ξ)−f(x))m(dξ)+∫(f(x+ξ)−f(x)−⟨χ(ξ),∇f⟩)M(x,dξ),

with Aijkl(x)=xikαjl+xilαjk+xjkαil+xjlαikA_{ijkl}(x)=x_{ik}\alpha_{jl}+x_{il}\alpha_{jk}+x_{jk}\alpha_{il}+x_{jl}\alpha_{ik}Aijkl​(x)=xik​αjl​+xil​αjk​+xjk​αil​+xjl​αik​. They also define the functions F(u)F(u)F(u) and R(u)R(u)R(u) of (2.16)–(2.17), which drive the generalized Riccati equations ∂tφ=F(ψ)\partial_t\varphi=F(\psi)∂t​φ=F(ψ), φ(0,u)=0\varphi(0,u)=0φ(0,u)=0 and ∂tψ=R(ψ)\partial_t\psi=R(\psi)∂t​ψ=R(ψ), ψ(0,u)=u\psi(0,u)=uψ(0,u)=u.

Formalization targets

Goal: Theorem 2.4, second part (= Proposition 5.9)

For every admissible parameter set there is a transition family (pt)(p_t)(pt​) and there are exponents (φ,ψ)(\varphi,\psi)(φ,ψ) such that:

(i) p is affine with exponents (φ,ψ);(ii) S+⊂D(Ap), Apf=(2.12);(iii) (φ,ψ) solves (2.14)–(2.15);\text{(i) } p \text{ is affine with exponents } (\varphi,\psi);\quad\text{(ii) } \mathcal S_+\subset D(\mathcal A_p),\ \mathcal A_pf=\text{(2.12)};\quad\text{(iii) } (\varphi,\psi) \text{ solves (2.14)–(2.15)};(i) p is affine with exponents (φ,ψ);(ii) S+​⊂D(Ap​), Ap​f=(2.12);(iii) (φ,ψ) solves (2.14)–(2.15); (iv) every affine p′ whose generator equals (2.12) on S+ satisfies pt′=pt for t≥0.\text{(iv) every affine } p' \text{ whose generator equals (2.12) on } \mathcal S_+ \text{ satisfies } p'_t=p_t \text{ for } t\ge0.(iv) every affine p′ whose generator equals (2.12) on S+​ satisfies pt′​=pt​ for t≥0.

Milestones, in attack order

  1. Theorem 4.8: a comparison theorem for matrix ODEs whose vector field is quasi-monotone increasing (Volkmann).
  2. Lemma 5.1: RRR is analytic on Sd++S_d^{++}Sd++​ and quasi-monotone increasing on Sd+S_d^+Sd+​.
  3. Lemma 5.2: the growth bound ⟨u,R(u)⟩≤K2(∥u∥2+1)\langle u,R(u)\rangle\le\frac K2(\|u\|^2+1)⟨u,R(u)⟩≤2K​(∥u∥2+1).
  4. Proposition 5.3: unique global R+×Sd++\mathbb R_+\times S_d^{++}R+​×Sd++​-valued Riccati solutions, analytic in (t,u)(t,u)(t,u).
  5. Lemma 5.5: the regularized operators Aε,δ,n\mathcal A^{\varepsilon,\delta,n}Aε,δ,n converge to A\mathcal AA uniformly on S+\mathcal S_+S+​.
  6. Lemma 5.7 (second part): the boundary condition ⟨b−12∑Dσklσkl,u⟩≥0\langle b-\frac12\sum D\sigma^{kl}\sigma^{kl},u\rangle\ge0⟨b−21​∑Dσklσkl,u⟩≥0 on ∂Sd+\partial S_d^+∂Sd+​.
  7. Lemma 5.6: the regularized martingale problems have Sd+S_d^+Sd+​-valued càdlàg solutions.
  8. Lemma 5.8: the martingale problem for A\mathcal AA has an Sd+∪{Δ}S_d^+\cup\{\Delta\}Sd+​∪{Δ}-valued càdlàg solution.

Significance

Together with the necessity direction (companion mission I in this series), the goal makes admissibility an exact characterization. Every admissible parameter set, including those with jumps of infinite activity and state-dependent killing, defines a well-posed Markov model on Sd+S_d^+Sd+​. Its Laplace transform is then given by the Riccati flow, which is what makes the model computationally tractable. The intermediate results are reusable on their own:

  • the matrix comparison theorem applies to any ODE on symmetric matrices;
  • the Riccati well-posedness on Sd++S_d^{++}Sd++​ holds for vector fields that need not be Lipschitz at ∂Sd+\partial S_d^+∂Sd+​;
  • the martingale-problem framework on a one-point compactification is used beyond this paper.

The theorem is proved in the paper; it is not formalized anywhere. No formal library contains affine processes, generalized Riccati equations on matrix cones, quasi-monotone comparison theorems or martingale problems with jumps. Formalizing them requires all of that infrastructure.

Difficulty

The obvious route is to solve the Riccati equation (2.15) on Sd+S_d^+Sd+​ by Picard iteration and to show invariance of the cone from the inward-pointing condition. That route fails because RRR need not be Lipschitz at ∂Sd+\partial S_d^+∂Sd+​: the integral term can have unbounded derivative there (Remark 5.4). Standard invariance theorems therefore do not apply. Instead, quasi-monotonicity keeps the solution away from the boundary.

The obvious construction of the process is also blocked. Stroock's existence and uniqueness theory for martingale problems needs Rn\mathbb R^nRn and a uniformly elliptic diffusion part, and neither holds on the cone, where the diffusion degenerates at the boundary. Existence must go through regularized operators with bounded smooth coefficients, then tightness in the Skorokhod space of Sd+∪{Δ}S_d^+\cup\{\Delta\}Sd+​∪{Δ} and a limit. Uniqueness in law comes from the Riccati solutions. The killing terms ccc and γ\gammaγ are added last.

Formalization scope

Conventions committed to in Lean:

  • MdM_dMd​ is the function type Fin d → Fin d → ℝ, with ⟨x,y⟩=∑ijxijyji\langle x,y\rangle=\sum_{ij}x_{ij}y_{ji}⟨x,y⟩=∑ij​xij​yji​ and its norm.
  • Sd+S_d^+Sd+​ is the subtype of positive semidefinite matrices, with the subspace topology and Borel structure.
  • Partial derivatives ∂/∂xij\partial/\partial x_{ij}∂/∂xij​ are taken in the symmetrized directions 12(Eij+Eji)\tfrac12(E^{ij}+E^{ji})21​(Eij+Eji).
  • The matrix measure μ\muμ is encoded as H dνH\,d\nuHdν with a finite measure ν\nuν and a positive semidefinite density HHH. This encoding is equivalent; take ν=∑iμii\nu=\sum_i\mu_{ii}ν=∑i​μii​.
  • The test space S+\mathcal S_+S+​ is represented by Schwartz functions on MdM_dMd​, restricted to the cone. The generator is the uniform limit of (Ptf−f)/t(P_tf-f)/t(Pt​f−f)/t.
  • Transition families are indexed by t∈Rt\in\mathbb Rt∈R, and only t≥0t\ge0t≥0 enters. Uniqueness is equality for t≥0t\ge0t≥0, never ∃!.
  • Analyticity on Sd++S_d^{++}Sd++​ is analyticity of y↦G((y+y⊤)/2)y\mapsto G((y+y^\top)/2)y↦G((y+y⊤)/2) on an open subset of MdM_dMd​.
  • Martingale problems carry an existentially quantified probability space, the natural filtration and càdlàg paths (the platform predicate EthierKurtz.HasCadlagPaths).
  • The cut-offs ϕn\phi_nϕn​ and ηε\eta_\varepsilonηε​ of §5.2 are arbitrary functions with the properties the paper lists. The paper fixes some and uses only those properties.
  • The case condition of (5.7) is tested on ϕn(x)x\phi_n(x)xϕn​(x)x, the argument of ηε\eta_\varepsilonηε​, rather than on xxx as printed. The printed reading makes sε,ns_{\varepsilon,n}sε,n​ discontinuous off Sd+S_d^+Sd+​, which contradicts the paper's claim sε,n∈Cb∞(Sd,Sd)s_{\varepsilon,n}\in C_b^\infty(S_d,S_d)sε,n​∈Cb∞​(Sd​,Sd​). The two readings agree on Sd+S_d^+Sd+​.
  • In Theorem 4.8, "locally Lipschitz" is read as Lipschitz in the state variable, locally uniformly in time. This is weaker than joint local Lipschitz continuity in (t,x)(t,x)(t,x).
  • Every statement that contains one of the integrals of (2.12), (2.16), (2.17) or (5.10) also asserts that its integrand is integrable.
  • Hypotheses not present on the page: none. Lemmas 5.1 and 5.2 assume less than the section's standing assumptions (not the drift condition (2.4)).

Trivializing formalizations are excluded:

  • Lean's value 000 for a non-integrable integral is ruled out by the integrability conclusions.
  • A pointwise generator would be weaker than the paper's notion, so the generator is the uniform limit.
  • An ∃! over transition families would be false at negative times, so uniqueness is stated for t≥0t\ge0t≥0.
  • A martingale problem is not posed for a fixed probability space, and X0=xX_0=xX0​=x is required almost surely.

Needed infrastructure, reusable beyond this mission: matrix calculus on SdS_dSd​ (square roots, spectral derivatives), comparison theorems for quasi-monotone ODEs, analytic dependence of ODE solutions, tightness in Skorokhod space, and martingale problems on locally compact spaces. Contributions are welcome at any of these levels, as are alternative proofs of the milestones.

Selected references

  • C. Cuchiero, D. Filipović, E. Mayerhofer, J. Teichmann, Affine processes on positive semidefinite matrices, Ann. Appl. Probab. 21 (2011) 397–463; cited from arXiv:0910.0137v3. https://arxiv.org/abs/0910.0137v3
  • D. Duffie, D. Filipović, W. Schachermayer, Affine processes and applications in finance, Ann. Appl. Probab. 13 (2003) 984–1053. https://mathscinet.ams.org/mathscinet-getitem?mr=1994043
  • M.-F. Bru, Wishart processes, J. Theoret. Probab. 4 (1991) 725–751. https://mathscinet.ams.org/mathscinet-getitem?mr=1132135
  • S. N. Ethier, T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, New York, 1986. https://mathscinet.ams.org/mathscinet-getitem?mr=0838085
  • P. Volkmann, Über die Invarianz konvexer Mengen und Differentialungleichungen in einem normierten Raume, Math. Ann. 203 (1973) 201–210. https://mathscinet.ams.org/mathscinet-getitem?mr=0322305
19 thms1 active userReviewed
Markov ChainOperations ResearchProbability·Captain: mikedeng1

Validity of Heavy Traffic Steady-State Approximations in Generalized Jackson Networks: Scaled Stationary Queue Lengths Converge to the Stationary Distribution of the Reflected Brownian MotionResearch Paper

Motivation

Open networks of single-server queues with general (non-exponential) interarrival and service times, generalized Jackson networks (GJNs), model manufacturing lines, communication networks and service systems. Their stationary distributions are almost never available in closed form. The standard engineering approximation replaces the scaled queue-length vector by the stationary distribution of a reflected Brownian motion (RBM) in the orthant, which is the diffusion limit of the network in heavy traffic, when every station is close to full utilisation.

The diffusion limit itself (Reiman, 1984) is a statement about the process on finite time intervals. Using the RBM's stationary law as an approximation of the network's stationary law requires interchanging two limits: time to infinity (steady state) and traffic intensity to one (heavy traffic). For a long time this interchange was assumed rather than proved.

Timeline.

  • 1984. Reiman proved the process-level heavy-traffic limit for open queueing networks started empty (doi:10.1287/moor.9.3.441).
  • 1987. Harrison and Williams characterised when an orthant RBM has a stationary distribution and showed it is unique (doi:10.1080/17442508708833469).
  • 1995. Dai related fluid-model stability to positive Harris recurrence of multiclass networks (doi:10.1214/aoap/1177004828).
  • 2006. Gamarnik and Zeevi proved the interchange of limits for GJNs whose primitives have exponential moments (arXiv:math/0410066). This mission formalizes that result.

Setting

There are JJJ stations. Station jjj receives external arrivals with i.i.d. interarrival times of law FA,jF_{A,j}FA,j​ (rate αj\alpha_jαj​, or no arrivals at all) and serves jobs first-in-first-out with i.i.d. service times of law FS,jF_{S,j}FS,j​ (mean mjm_jmj​, rate μj=1/mj\mu_j = 1/m_jμj​=1/mj​). A job finishing at jjj moves to kkk with probability pjkp_{jk}pjk​ or leaves. The routing matrix PPP is substochastic with spectral radius below one. Interarrival and service times have uniformly bounded conditional exponential moments of their residual lives (conditions (1)–(2)). The traffic equation λ=α+P′λ\lambda = \alpha + P'\lambdaλ=α+P′λ gives the effective rates λ=[I−P′]−1α\lambda = [I-P']^{-1}\alphaλ=[I−P′]−1α and the traffic intensities ρj=λjmj\rho_j = \lambda_j m_jρj​=λj​mj​.

The queue lengths Q(t)Q(t)Q(t) are not Markov. The state Qˉ(t)=(Q(t),a^(t),v^(t))\bar Q(t) = (Q(t),\hat a(t),\hat v(t))Qˉ​(t)=(Q(t),a^(t),v^(t)), which adds the elapsed interarrival and service times, is a Markov process on X=Z+J×R+2J\mathcal X = \mathbb Z_+^J\times\mathbb R_+^{2J}X=Z+J​×R+2J​. A law π\piπ on X\mathcal XX is stationary if Qˉ(0)∼π\bar Q(0)\sim\piQˉ​(0)∼π implies Qˉ(t)∼π\bar Q(t)\sim\piQˉ​(t)∼π for all t≥0t\ge0t≥0.

Heavy traffic. Fix a critically loaded network Ξ\XiΞ (ρj=1\rho_j=1ρj​=1 for all jjj) and a vector κ0>0\kappa^0>0κ0>0. The network Ξn\Xi^nΞn slows the arrivals of Ξ\XiΞ at station jjj by the factor 1−κj0/n1-\kappa^0_j/\sqrt n1−κj0​/n​, so that ρjn=1−κj/n<1\rho^n_j = 1-\kappa_j/\sqrt n<1ρjn​=1−κj​/n​<1 for an explicit κ>0\kappa>0κ>0 (display (17)). Let πn\pi^nπn be any stationary distribution of Ξn\Xi^nΞn, and let π^n\hat\pi^nπ^n be the law of Qn(0)/nQ^n(0)/\sqrt nQn(0)/n​ under πn\pi^nπn.

The RBM. For a Brownian motion WWW with drift β\betaβ and covariance Γ\GammaΓ, the RBM ZZZ with parameters (β,Γ,I−P′)(\beta,\Gamma,I-P')(β,Γ,I−P′) solves the Skorohod problem Z=W+[I−P′]Y≥0Z = W + [I-P']Y\ge0Z=W+[I−P′]Y≥0, with YYY nondecreasing and increasing only when ZZZ is on the boundary. Here β=−(I−P′)M−1κ\beta = -(I-P')M^{-1}\kappaβ=−(I−P′)M−1κ and Γ\GammaΓ is the explicit covariance matrix of Reiman's theorem, built from μ\muμ, α\alphaα, PPP and the squared coefficients of variation ca,j2c^2_{a,j}ca,j2​, cs,j2c^2_{s,j}cs,j2​ of Ξ\XiΞ.

Formalization targets

Goal: Theorem 8 (p. 18)

π^n ⇒ πRBM(n→∞),\hat\pi^n\ \Rightarrow\ \pi_{\mathrm{RBM}}\qquad(n\to\infty),π^n ⇒ πRBM​(n→∞),

where πRBM\pi_{\mathrm{RBM}}πRBM​ is the unique stationary distribution of the (β,Γ,I−P′)(\beta,\Gamma,I-P')(β,Γ,I−P′)-RBM. The formal goal asserts three things: a stationary distribution of the RBM exists, it is the only one, and π^n\hat\pi^nπ^n converges weakly to it, for every choice of stationary distributions πn\pi^nπn.

Milestones

  1. Theorems 5 and 6 (pp. 15–16). For a general Markov process, a geometric Lyapunov function Φ\PhiΦ gives EπΦ≤ϕ(t0)K/(1−γ)\mathbb E_\pi\Phi\le\phi(t_0)K/(1-\gamma)Eπ​Φ≤ϕ(t0​)K/(1−γ). A Lyapunov function with control of L2L_2L2​ gives an exponential tail Pπ(Φ>s)≲e−θs\mathbb P_\pi(\Phi>s)\lesssim e^{-\theta s}Pπ​(Φ>s)≲e−θs.
  2. Proposition 1 (p. 11). The fluid model drains in time at most w′z/min⁡jμj(1−ρj)w'z/\min_j\mu_j(1-\rho_j)w′z/minj​μj​(1−ρj​), where w=e′[I−P′]−1w=e'[I-P']^{-1}w=e′[I−P′]−1.
  3. Lemma A.1 and Propositions 2–3 (pp. 17, 25). The net input deviates from its fluid path by O(n)O(\sqrt n)O(n​) uniformly over initial states. As a result, Φ(z,a,v)=w′z\Phi(z,a,v)=w'zΦ(z,a,v)=w′z is a Lyapunov function for Ξn\Xi^nΞn with drift −n-\sqrt n−n​ over time nt0nt_0nt0​.
  4. Theorem 7 and Corollary 1 (pp. 17–18). Pπn(n−1/2w′Qn(0)>s)≤C1e−c1s\mathbb P_{\pi^n}(n^{-1/2}w'Q^n(0)>s)\le C_1e^{-c_1s}Pπn​(n−1/2w′Qn(0)>s)≤C1​e−c1​s uniformly in nnn. Hence {π^n}\{\hat\pi^n\}{π^n} is tight.
  5. Theorems 4, 3 and 2 (cited). Reiman's process limit from a general initial law; Harrison and Williams's existence and uniqueness theorem for the RBM's stationary distribution; existence of πn\pi^nπn.

Significance

The result. Theorem 8 justifies the use of the RBM's stationary distribution, which is computable or at least numerically tractable, as an approximation of steady-state queue lengths of a heavily loaded network. Theorem 7 also shows that each stationary queue is of order (1−ρ∗n)−1(1-\rho^{*n})^{-1}(1−ρ∗n)−1 uniformly in nnn. Together with Theorem 8 this gives convergence of all moments (Corollary 2 of the paper) and, through Theorems 9–12, steady-state approximations of sojourn times and product-form limits.

Formalizing it. No part of this argument is machine-checked. The formalization would add reusable infrastructure for queueing theory in Lean: a Markov-state model of a generalized Jackson network with residual times, Lyapunov bounds on stationary distributions of general Markov processes (Theorems 5–6), and the link between tightness and identification of limit points for stationary laws. Reiman's theorem (Theorem 4) and the Harrison–Williams theorem (Theorem 3) are cited by the paper and are themselves open formalization targets.

Difficulty

Tightness and Reiman's theorem do not combine on their own. Reiman's theorem describes the network on finite time intervals, started empty, while a stationary distribution describes it as time goes to infinity; nothing in the finite-horizon limit forces a limit point of π^n\hat\pi^nπ^n to be stationary for the RBM, or forces different subsequences to have the same limit. The interchange therefore needs the process limit from an arbitrary initial law and the uniqueness of the RBM's stationary law, besides tightness.

The tightness step is the technical core. Moment bounds must be uniform in nnn and in the initial residual times. A Lyapunov argument on the workload w′Qw'Qw′Q over a time horizon of order nnn requires deviation bounds of order n\sqrt nn​ for renewal processes started at arbitrary ages. This is why the residual-life conditions (1)–(2) appear, and why the strong approximation of Lemma A.2 is used. A naive drift argument over a fixed time horizon fails: in heavy traffic the drift of w′Qw'Qw′Q per unit time is only of order n−1/2n^{-1/2}n−1/2.

Formalization scope

  • Stations are Fin J, vectors Fin J → ℝ, P′P'P′ is Pᵀ, and the norm ∥⋅∥\|\cdot\|∥⋅∥ is the ℓ1\ell^1ℓ1 norm, written as an explicit sum. The spectral-radius condition is Pm→0P^m\to0Pm→0.
  • A network is its data (J,FA,FS,P)(\mathcal J, F_A, F_S, P)(J,FA​,FS​,P) plus the predicate IsGJN (positive times, conditions (1)–(2), substochastic PPP). AjA_jAj​ and SjS_jSj​ count renewal epochs in [0,t][0,t][0,t]. The initial times aj(0)a_j(0)aj​(0), vj(0)v_j(0)vj​(0) are residual lives given the elapsed ages a^j(0)\hat a_j(0)a^j​(0), v^j(0)\hat v_j(0)v^j​(0). States carry their elapsed times as reals; the predicate InStateSpace cuts out X=Z+J×R+2J\mathcal X=\mathbb Z_+^J\times\mathbb R_+^{2J}X=Z+J​×R+2J​, and the uniform bounds over initial states (Lemma A.1, Propositions 2–3) and the initial laws of Theorem 4 range over X\mathcal XX only.
  • A realization from an initial law is a probability space carrying the primitives with their joint law and processes Q,BQ, BQ,B satisfying the dynamics (4)–(5) almost surely. E[⋅∣Qˉ(0)=x]\mathbb E[\cdot\mid\bar Q(0)=x]E[⋅∣Qˉ​(0)=x] is the expectation under a realization from δx\delta_xδx​. Stationarity of π\piπ means: a realization from π\piπ exists, and every realization from π\piπ has Qˉ(t)∼π\bar Q(t)\sim\piQˉ​(t)∼π for all t≥0t\ge0t≥0.
  • The heavy-traffic scaling is read as ajn=aj/(1−κj0/n)a^n_j = a_j/(1-\kappa^0_j/\sqrt n)ajn​=aj​/(1−κj0​/n​). The printed aj(1−κj0/n)a_j(1-\kappa^0_j/\sqrt n)aj​(1−κj0​/n​) would overload every Ξn\Xi^nΞn, so no πn\pi^nπn would exist. κ\kappaκ is defined so that (17) holds exactly, and every statement about Ξn\Xi^nΞn is for all large nnn.
  • The RBM is built on the published Reiman84.QueueLength.Paths (Brownian motion with drift and covariance, and the reflection pair). An RBM stationary law must be a probability measure carried by R+J\mathbb R^J_+R+J​. Weak convergence of laws on RJ\mathbb R^JRJ uses Mathlib's topology on ProbabilityMeasure. Theorem 4's process convergence is in coupling form with the uniform topology on [0,T][0,T][0,T].
  • Quantities lim sup⁡n(⋅)<∞\limsup_n(\cdot)<\inftylimsupn​(⋅)<∞ are rendered as one finite bound valid for all large nnn. Expectations of nonnegative quantities are lower Lebesgue integrals in [0,∞][0,\infty][0,∞]. Constants "depending only on Ξ\XiΞ" are quantified before nnn and before the stationary distributions.
  • Disclosed departures from the page:
    • ϕ(t0)<∞\phi(t_0)<\inftyϕ(t0​)<∞ is assumed in Theorem 5.
    • {Φ>K}≠∅\{\Phi>K\}\neq\emptyset{Φ>K}=∅ is assumed in Theorem 6. Its tail constant (29) is stated as (γθ/2)−1(\gamma\theta/2)^{-1}(γθ/2)−1, which is what the paper's proof yields, instead of the printed (1−γθ/2)−1(1-\gamma\theta/2)^{-1}(1−γθ/2)−1.
    • Γ\GammaΓ is positive definite in Theorem 3, the hypothesis of Harrison and Williams.
    • The derivative bound w′q˙(t)≤−min⁡jμj(1−ρj)w'\dot q(t)\le-\min_j\mu_j(1-\rho_j)w′q˙​(t)≤−minj​μj​(1−ρj​) of Proposition 1 is stated for ρj≤1\rho_j\le1ρj​≤1 at every station; the page states it unconditionally, and it fails when two stations are overloaded.
    • Theorems 5 and 6 are stated for the time-t0t_0t0​ transition kernel of the Markov process.
  • A trivializing formalization is ruled out explicitly. The goal keeps the existence and uniqueness of πRBM\pi_{\mathrm{RBM}}πRBM​ as conjuncts, stationarity requires a realization to exist, and the RBM's stationary law must live on the orthant. Hence neither an impossible network nor an empty RBM notion makes the goal vacuous.
  • Contributions are welcome on any milestone. The cited Theorems 2–4 are substantial on their own, and Theorems 5–6 are independent of queueing.

Selected references

  • D. Gamarnik and A. Zeevi, Validity of heavy traffic steady-state approximations in generalized Jackson networks, Ann. Appl. Probab. 16(1), 2006, 56–90. arXiv:math/0410066, doi:10.1214/105051605000000638
  • M. I. Reiman, Open queueing networks in heavy traffic, Math. Oper. Res. 9(3), 1984, 441–458. doi:10.1287/moor.9.3.441
  • J. M. Harrison and R. J. Williams, Brownian models of open queueing networks with homogeneous customer populations, Stochastics 22, 1987, 77–115. doi:10.1080/17442508708833469
  • J. G. Dai, On positive Harris recurrence of multiclass queueing networks: a unified approach via fluid limit models, Ann. Appl. Probab. 5(1), 1995, 49–77. doi:10.1214/aoap/1177004828
  • H. Chen and D. D. Yao, Fundamentals of Queueing Networks: Performance, Asymptotics, and Optimization, Springer, 2001 (reference [11] of the paper; Chapter 7).
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Operations ResearchProbability·Captain: mikedeng1

A Theoretical Framework for the Pricing of Contingent Claims in the Presence of Model Uncertainty: Superreplication Price Equals a Supremum over Martingale Measures with Bracket BoundsResearch Paper

Motivation

Classical arbitrage pricing fixes one probabilistic model of the underlying asset and prices a contingent claim as an expectation under an equivalent martingale measure. When the volatility is not known, a seller who wants to be safe under every plausible model has to superreplicate: hold an initial capital and a trading strategy whose terminal value dominates the claim under all models at once. The uncertain volatility model (UVM) of Avellaneda, Levy and Parás (Appl. Math. Finance 1995) and Lyons (Appl. Math. Finance 1995) is the standard instance: the volatility is only known to lie in an interval [σ‾,σˉ][\underline\sigma,\bar\sigma][σ​,σˉ].

The family of laws describing such uncertainty is not dominated by a single reference probability, so "almost surely" and the usual stochastic integral are not available. Denis and Martini (Ann. Appl. Probab. 2006) replace them by a capacity and a quasi-sure stochastic integral, and show that the superreplication price of a broad class of path-dependent European claims is a supremum of expectations over martingale laws. This framework is a precursor of quasi-sure analysis and GGG-expectations (Denis, Hu and Peng, Potential Anal. 2011; Soner, Touzi and Zhang, Electron. J. Probab. 2011).

Setting

Fix T>0T>0T>0. Ω\OmegaΩ is the space of continuous paths B=(Bt)t∈[0,T]B=(B_t)_{t\in[0,T]}B=(Bt​)t∈[0,T]​ with B0=0B_0=0B0​=0, with the uniform norm, Borel σ\sigmaσ-field B\mathcal BB and canonical filtration Ft=σ(Bs:s≤t)\mathcal F_t=\sigma(B_s:s\le t)Ft​=σ(Bs​:s≤t). A martingale measure is a probability on Ω\OmegaΩ under which BBB is an (Ft)(\mathcal F_t)(Ft​)-martingale; Pm\mathbf P_mPm​ denotes the set of these.

A nonzero measure μˉ\bar\muμˉ​ on [0,T][0,T][0,T] with continuous distribution function μˉt=μˉ([0,t])\bar\mu_t=\bar\mu([0,t])μˉ​t​=μˉ​([0,t]) bounds the bracket. Hypothesis H(μˉ)H(\bar\mu)H(μˉ​) on a set P⊆Pm\mathbf P\subseteq\mathbf P_mP⊆Pm​ says d⟨B⟩tP≤dμˉtd\langle B\rangle^P_t\le d\bar\mu_td⟨B⟩tP​≤dμˉ​t​ for every P∈PP\in\mathbf PP∈P; H(μ‾,μˉ)H(\underline\mu,\bar\mu)H(μ​,μˉ​) adds a lower bound dμ‾t≤d⟨B⟩tPd\underline\mu_t\le d\langle B\rangle^P_tdμ​t​≤d⟨B⟩tP​. In the UVM, dμ‾=σ‾2dtd\underline\mu=\underline\sigma^2dtdμ​=σ​2dt and dμˉ=σˉ2dtd\bar\mu=\bar\sigma^2dtdμˉ​=σˉ2dt.

The capacity of a bounded continuous φ\varphiφ is c(φ)=sup⁡P∈P∥φ∥L2(P)c(\varphi)=\sup_{P\in\mathbf P}\|\varphi\|_{L^2(P)}c(φ)=supP∈P​∥φ∥L2(P)​, extended to all functions through lower semicontinuous majorants. A set is polar if its capacity is 000, and a property holds quasi-surely (q.s.) outside a polar set. L\mathcal LL is the completion of Cb(Ω)C_b(\Omega)Cb​(Ω) under ccc. Elementary integrands h=∑ikti1]ti,ti+1]h=\sum_i k_{t_i}\mathbb 1_{]t_i,t_{i+1}]}h=∑i​kti​​1]ti​,ti+1​]​ have integrals IT(h)=∑ikti(Bti+1−Bti)I_T(h)=\sum_ik_{t_i}(B_{t_{i+1}}-B_{t_i})IT​(h)=∑i​kti​​(Bti+1​​−Bti​​), and H\mathcal HH is their completion for ∥h∥H=sup⁡P(EP∫0Ths2dμˉs)1/2\|h\|_{\mathcal H}=\sup_P(E_P\int_0^Th_s^2d\bar\mu_s)^{1/2}∥h∥H​=supP​(EP​∫0T​hs2​dμˉ​s​)1/2. K={IT(h):h∈H}K=\{I_T(h):h\in\mathcal H\}K={IT​(h):h∈H} is the space of attainable gains. The superreplication price of a claim fff is

Λ(f)=inf⁡{a∈R: ∃g∈K, a+g≥f q.s.}.\Lambda(f)=\inf\{a\in\mathbb R:\ \exists g\in K,\ a+g\ge f\ \text{q.s.}\}.Λ(f)=inf{a∈R: ∃g∈K, a+g≥f q.s.}.

Formalization targets

Goal: Theorem 3.1 for explicit claims

Assume H(μ‾,μˉ)H(\underline\mu,\bar\mu)H(μ​,μˉ​) and that μˉ\bar\muμˉ​ is Hölder continuous. There is a set P′′⊂Pm\mathbf P''\subset\mathbf P_mP′′⊂Pm​ of martingale measures satisfying H(μ‾,μˉ)H(\underline\mu,\bar\mu)H(μ​,μˉ​) such that

Λ(f)=sup⁡{EPf:P∈P′′}\Lambda(f)=\sup\{E_Pf:P\in\mathbf P''\}Λ(f)=sup{EP​f:P∈P′′}

for every bounded continuous fff of the form F(Bt1,…,Btd)F(B_{t_1},\dots,B_{t_d})F(Bt1​​,…,Btd​​), G(∫0TF(Bs)ds)G\big(\int_0^TF(B_s)ds\big)G(∫0T​F(Bs​)ds) or G(sup⁡tBt)G(\sup_tB_t)G(supt​Bt​), with GGG (and the cylindrical FFF) bounded continuous. The goal leaves P′′\mathbf P''P′′ unspecified, as the paper does.

Milestones

In attack order: the transfer of a.s. inequalities to q.s. ones (Lemma A.7); the pathwise moment bound (Bt−Bs)2n≤∫sth dB+Cμˉ(]s,t])n(B_t-B_s)^{2n}\le\int_s^th\,dB+C\bar\mu(]s,t])^n(Bt​−Bs​)2n≤∫st​hdB+Cμˉ​(]s,t])n q.s. (Proposition 2.9) and its price form Λ((Bt−Bs)2n)≤C2nμˉ([s,t])n\Lambda((B_t-B_s)^{2n})\le C_{2n}\bar\mu([s,t])^nΛ((Bt​−Bs​)2n)≤C2n​μˉ​([s,t])n (Proposition 2.13); a universal bracket ⟨B⟩t∈L\langle B\rangle_t\in\mathcal L⟨B⟩t​∈L (Lemma 2.10) approximated by realized variance (Lemma 2.14); weak duality Λ(f)≥sup⁡P′EPf\Lambda(f)\ge\sup_{\mathbf P'}E_PfΛ(f)≥supP′​EP​f (Lemma 2.15); the representation Λ(f)=sup⁡Q∈QEQf~\Lambda(f)=\sup_{Q\in\mathcal Q}E_Q\tilde fΛ(f)=supQ∈Q​EQ​f~​ over probabilities on the Stone–Čech compactification Ω~\tilde\OmegaΩ~ (§5, p. 19) and the Cauchy–Schwarz inequality for Λ\LambdaΛ (Lemma 4.3); the martingale property and continuity of B~\tilde BB~ under each QQQ (Proposition 5.2); the bracket bounds for the induced law Q∗Q^*Q∗ (Lemma 5.3); membership of the three claim families in the class Γ\GammaΓ of fff with EQf~=EQ∗fE_Q\tilde f=E_{Q^*}fEQ​f~​=EQ∗​f (Lemmas 5.4–5.6); and Theorem 3.1 for the literal class Γ\GammaΓ.

Further statements: Theorem 6.1 (all martingale measures with H(μ‾,μˉ)H(\underline\mu,\bar\mu)H(μ​,μˉ​) form a valid P′′\mathbf P''P′′), Proposition 3.2 (the case dom⁡Λ=L\operatorname{dom}\Lambda=\mathcal LdomΛ=L), Proposition 2.12 (measures not charging polar sets inherit the bracket bounds), Theorem A.8 (closedness of KKK under H(aμˉ,μˉ)H(a\bar\mu,\bar\mu)H(aμˉ​,μˉ​)).

Significance

The theorem identifies the cheapest model-free hedge of path-dependent European claims (cylindrical payoffs, Asian-type averages, lookbacks on the maximum) with a worst-case expectation over martingale laws obeying the same bracket bounds. Theorem 6.1 specializes it to the generalized UVM, where the dual set is all martingale measures with dμ‾≤d⟨B⟩≤dμˉd\underline\mu\le d\langle B\rangle\le d\bar\mudμ​≤d⟨B⟩≤dμˉ​; the paper notes this is new even for the Lebesgue case. The result supplies a rigorous non-dominated duality on which robust pricing bounds and GGG-expectation pricing rest.

The theorem is proved in the paper; no part of it is machine-checked. A formalization would produce the first Lean development of a capacity on path space, of a quasi-sure stochastic integral, and of a continuous-time quadratic variation on the canonical space. These objects are absent from Mathlib, which has discrete- and continuous-time martingales, the Stone–Čech compactification and the Riesz–Markov–Kakutani theorem, but no stochastic integral.

Difficulty

The family P\mathbf PP is not dominated, so neither the Itô integral of a single model nor a common null set is available: every inequality obtained under one PPP by the Itô formula must be lifted to a quasi-sure one, and every limit taken in the capacity. The natural dual argument (Hahn–Banach on L\mathcal LL) produces linear forms whose representation as measures on Ω\OmegaΩ is not available because dom⁡Λ\operatorname{dom}\LambdadomΛ need not be all of L\mathcal LL. The paper's route works on bounded continuous claims and compactifies; the price is that the dual measures live on Ω~\tilde\OmegaΩ~, where BtB_tBt​ is unbounded and must be extended by truncation, and the identity EQf~=EQ∗fE_Q\tilde f=E_{Q^*}fEQ​f~​=EQ∗​f linking Ω~\tilde\OmegaΩ~ back to Ω\OmegaΩ holds only for a class of claims that has to be checked family by family.

Formalization scope

Ω\OmegaΩ is a subtype of C(Set.Icc 0 T, ℝ) (paths with B0=0B_0=0B0​=0) with the Borel σ\sigmaσ-field of the sup-norm topology. Distribution functions are continuous StieltjesFunctions vanishing at 000 and positive at TTT. The quadratic variation is a predicate: an adapted process with PPP-a.s. continuous nondecreasing paths from 000 such that B2−AB^2-AB2−A is a martingale. The capacity takes values in [0,∞][0,\infty][0,∞] with the Appendix's Lebesgue extension; q.s. means outside a set of capacity zero. L\mathcal LL, H\mathcal HH and KKK are membership predicates on functions. KKK is the image of the completion H\mathcal HH. Λ\LambdaΛ and every supremum are extended reals. Ω~\tilde\OmegaΩ~ is Mathlib's StoneCech, and Q\mathcal QQ is the set of Borel probabilities on it dominated by Λ\LambdaΛ on Cb(Ω)C_b(\Omega)Cb​(Ω).

Standing assumptions, stated as hypotheses: H(μˉ)H(\bar\mu)H(μˉ​) on P\mathbf PP for all §2 results, H(μ‾,μˉ)H(\underline\mu,\bar\mu)H(μ​,μˉ​) where the page assumes it, and Hölder continuity of μˉ\bar\muμˉ​ for every result of §4–§5 and the goal (p. 12: "From now on, we assume that μˉ\bar\muμˉ​ is Hölder continuous"). The goal replaces the class Γ\GammaΓ, which is defined only inside the proof, by the three families of Lemmas 5.4–5.6. The literal form is a milestone. Lemma 2.14 adds P≠∅\mathbf P\neq\emptysetP=∅. Lemma 5.3 is stated for the law Q∗Q^*Q∗ on Ω\OmegaΩ.

The following trivializing formalizations are ruled out. An empty P\mathbf PP with a real-valued Λ\LambdaΛ would make the goal 0=00=00=0; here both sides are −∞-\infty−∞. Defining q.s. as "a.s. for every PPP" would make Lemma A.7 a tautology. Replacing KKK by the closure of elementary integrals would shrink Λ\LambdaΛ. Dropping the martingale condition from the quadratic-variation predicate would make H(μ‾,μˉ)H(\underline\mu,\bar\mu)H(μ​,μˉ​) satisfiable by any deterministic process.

A complete development needs Itô's formula and the Burkholder–Davis–Gundy inequalities for continuous martingales, Doob–Meyer uniqueness, a Kolmogorov continuity criterion, and the theory of regular Choquet capacities. These are reusable well beyond this mission, and contributions of any of them are welcome.

Selected references

  • L. Denis and C. Martini, A theoretical framework for the pricing of contingent claims in the presence of model uncertainty, Ann. Appl. Probab. 16(2):827–852, 2006. arXiv:math/0607111v1. https://arxiv.org/abs/math/0607111
  • M. Avellaneda, A. Levy and A. Parás, Pricing and hedging derivative securities in markets with uncertain volatilities, Appl. Math. Finance 2(2):73–88, 1995. https://doi.org/10.1080/13504869500000005
  • T. J. Lyons, Uncertain volatility and the risk-free synthesis of derivatives, Appl. Math. Finance 2(2):117–133, 1995. https://doi.org/10.1080/13504869500000007
  • L. Denis, M. Hu and S. Peng, Function spaces and capacity related to a sublinear expectation: application to G-Brownian motion paths, Potential Anal. 34:139–161, 2011. https://doi.org/10.1007/s11118-010-9185-x
  • H. M. Soner, N. Touzi and J. Zhang, Quasi-sure stochastic analysis through aggregation, Electron. J. Probab. 16:1844–1879, 2011. https://doi.org/10.1214/EJP.v16-950
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AnalysisOperations ResearchProbability·Captain: mikedeng1

Law of Large Numbers Limits for Many-Server Queues 2: The Fluid Age Measure Converges to the Equilibrium Measure (1 − G(x))dxResearch Paper

Motivation

Large call centers, cloud server farms and hospital wards are modeled as many-server queues: NNN identical servers, customers arriving according to a counting process, each customer served by one server for a random time drawn from a distribution GGG, and customers who find all servers busy waiting in a first-come first-served queue. When NNN is large, the number of customers is of order NNN and the natural object of study is the fluid limit, obtained by dividing all quantities by NNN and letting N→∞N\to\inftyN→∞. For exponential service times the fluid limit is a finite-dimensional ordinary differential equation. For a general service distribution — and call-center data show service times far from exponential (lognormal, in Brown et al., 2005) — the state must record how long each customer in service has been served, and the fluid limit is a measure-valued process.

Kaspi and Ramanan (Ann. Appl. Probab. 21 (2011) 33–114) characterize this limit by a pair of fluid equations for general GGG with a density, prove that they have at most one solution, show that the scaled NNN-server processes converge to it, and describe its long-time behavior. This mission is the last of these results: in the critically loaded fluid system, every solution converges to equilibrium.

Timeline. Whitt (2006) introduced a fluid model of the many-server queue with general service times and abandonment, and stated the case λˉ<1\bar\lambda<1λˉ<1 of property (1) of the goal theorem without proof (his Theorem 7.3). Kaspi and Ramanan (2011) gave the measure-valued formulation with the age process, uniqueness and existence of fluid solutions, and the convergence to equilibrium formalized here. Reed (2009) treated the related G/GI/NG/GI/NG/GI/N queue in the Halfin–Whitt regime.

Setting

The service distribution GGG has a density ggg, is carried by [0,∞)[0,\infty)[0,∞), and has mean one: ∫0∞x g(x) dx=∫0∞(1−G(x)) dx=1\int_0^\infty x\,g(x)\,dx=\int_0^\infty(1-G(x))\,dx=1∫0∞​xg(x)dx=∫0∞​(1−G(x))dx=1. Let M=sup⁡{x≥0:G(x)<1}∈(0,∞]M=\sup\{x\ge0:G(x)<1\}\in(0,\infty]M=sup{x≥0:G(x)<1}∈(0,∞], and let h=g/(1−G)h=g/(1-G)h=g/(1−G) be the hazard rate on [0,M)[0,M)[0,M).

The fluid state at time ttt is a number Xˉ(t)≥0\bar X(t)\ge0Xˉ(t)≥0, the scaled number of customers in system, and a measure νˉt\bar\nu_tνˉt​ on [0,M)[0,M)[0,M) of total mass at most one: νˉt(A)\bar\nu_t(A)νˉt​(A) is the scaled number of customers in service whose age (time already spent in service) lies in AAA. The input is a nondecreasing càdlàg arrival function Eˉ\bar EEˉ with Eˉ(0)=0\bar E(0)=0Eˉ(0)=0, an initial number Xˉ(0)\bar X(0)Xˉ(0) and an initial age measure νˉ0\bar\nu_0νˉ0​, satisfying 1−⟨1,νˉ0⟩=[1−Xˉ(0)]+1-\langle\mathbf 1,\bar\nu_0\rangle=[1-\bar X(0)]^+1−⟨1,νˉ0​⟩=[1−Xˉ(0)]+ (servers are idle only when nobody waits). The set of such triples is S0\mathcal S_0S0​.

A càdlàg pair (Xˉ,νˉ)(\bar X,\bar\nu)(Xˉ,νˉ) solves the fluid equations if the cumulative departures Dˉ(t)=∫0t⟨h,νˉs⟩ ds\bar D(t)=\int_0^t\langle h,\bar\nu_s\rangle\,dsDˉ(t)=∫0t​⟨h,νˉs​⟩ds are finite, the entries into service Kˉ(t)=⟨1,νˉt⟩−⟨1,νˉ0⟩+Dˉ(t)\bar K(t)=\langle\mathbf 1,\bar\nu_t\rangle-\langle\mathbf 1,\bar\nu_0\rangle+\bar D(t)Kˉ(t)=⟨1,νˉt​⟩−⟨1,νˉ0​⟩+Dˉ(t) satisfy the transport equation

⟨φ(⋅,t),νˉt⟩=⟨φ(⋅,0),νˉ0⟩+∫0t⟨φx+φs,νˉs⟩ ds−∫0t⟨hφ(⋅,s),νˉs⟩ ds+∫[0,t]φ(0,s) dKˉ(s)\langle\varphi(\cdot,t),\bar\nu_t\rangle=\langle\varphi(\cdot,0),\bar\nu_0\rangle+\int_0^t\langle\varphi_x+\varphi_s,\bar\nu_s\rangle\,ds-\int_0^t\langle h\varphi(\cdot,s),\bar\nu_s\rangle\,ds+\int_{[0,t]}\varphi(0,s)\,d\bar K(s)⟨φ(⋅,t),νˉt​⟩=⟨φ(⋅,0),νˉ0​⟩+∫0t​⟨φx​+φs​,νˉs​⟩ds−∫0t​⟨hφ(⋅,s),νˉs​⟩ds+∫[0,t]​φ(0,s)dKˉ(s)

for every compactly supported test function φ\varphiφ on [0,M)×[0,∞)[0,M)\times[0,\infty)[0,M)×[0,∞) (ages grow at unit rate, customers leave at rate hhh, new customers enter at age 000), mass is conserved, Xˉ(t)=Xˉ(0)+Eˉ(t)−Dˉ(t)\bar X(t)=\bar X(0)+\bar E(t)-\bar D(t)Xˉ(t)=Xˉ(0)+Eˉ(t)−Dˉ(t), and the system is non-idling, 1−⟨1,νˉt⟩=[1−Xˉ(t)]+1-\langle\mathbf 1,\bar\nu_t\rangle=[1-\bar X(t)]^+1−⟨1,νˉt​⟩=[1−Xˉ(t)]+.

The equilibrium measure is νˉ∗(dx)=(1−G(x)) dx\bar\nu_*(dx)=(1-G(x))\,dxνˉ∗​(dx)=(1−G(x))dx on [0,M)[0,M)[0,M), a probability measure by the mean-one normalization. With Eˉ=id\bar E=\mathrm{id}Eˉ=id (arrival rate equal to the total service capacity), Xˉ≡c≥1\bar X\equiv c\ge1Xˉ≡c≥1 and νˉ≡νˉ∗\bar\nu\equiv\bar\nu_*νˉ≡νˉ∗​ is a constant solution. Assumption 2 asks that hhh be bounded or lower semicontinuous near MMM. The renewal measure of GGG is U=∑n≥0G∗nU=\sum_{n\ge0}G^{*n}U=∑n≥0​G∗n, the unit mass at 000 included.

Formalization targets

Goal: Theorem 3.9

Under Assumption 2:

  1. if Eˉ=λˉ id\bar E=\bar\lambda\,\mathrm{id}Eˉ=λˉid with λˉ∈[0,1]\bar\lambda\in[0,1]λˉ∈[0,1] and the system starts empty, then Xˉ(t)=⟨1,νˉt⟩\bar X(t)=\langle\mathbf 1,\bar\nu_t\rangleXˉ(t)=⟨1,νˉt​⟩ increases to λˉ\bar\lambdaλˉ and νˉt\bar\nu_tνˉt​ increases weakly to λˉνˉ∗\bar\lambda\bar\nu_*λˉνˉ∗​;
  2. if ∫x2g(x) dx<∞\int x^2g(x)\,dx<\infty∫x2g(x)dx<∞, then for Eˉ=id\bar E=\mathrm{id}Eˉ=id and every initial condition in S0\mathcal S_0S0​,
lim⁡t→∞⟨f,νˉt⟩=∫[0,∞)f(x)(1−G(x)) dxfor every bounded continuous f.\lim_{t\to\infty}\langle f,\bar\nu_t\rangle=\int_{[0,\infty)}f(x)(1-G(x))\,dx\qquad\text{for every bounded continuous }f.t→∞lim​⟨f,νˉt​⟩=∫[0,∞)​f(x)(1−G(x))dxfor every bounded continuous f.

Milestones

  • Lemma 3.4: a solution restarted at time ttt solves the fluid equations for the shifted data.
  • Remark 3.8: the invariant solution (c+Eˉ−id,νˉ∗)(c+\bar E-\mathrm{id},\bar\nu_*)(c+Eˉ−id,νˉ∗​) when λˉ≥1\bar\lambda\ge1λˉ≥1.
  • Corollary 4.4, (4.6): Kˉ\bar KKˉ is the renewal measure UUU convolved with an explicit forcing term.
  • Proposition 6.1(1)–(3): the solution started empty, explicitly up to the first time τ1\tau_1τ1​ it fills, its monotone convergence for constant λˉ≤1\bar\lambda\le1λˉ≤1, and the comparison of an arbitrary solution with it.
  • Lemma 6.2: a reference system built from UUU converges weakly to ⟨1,π0⟩νˉ∗\langle\mathbf 1,\pi_0\rangle\bar\nu_*⟨1,π0​⟩νˉ∗​.
  • Lemma 6.3: a uniform renewal estimate under a finite second moment.

Significance

Theorem 3.9(2) is the stability statement of the fluid model in the critically loaded case: whatever the initial occupancy and the initial ages, the age distribution of customers in service converges to the stationary excess distribution of GGG. It justifies using νˉ∗\bar\nu_*νˉ∗​ as the operating point around which diffusion approximations of many-server queues are built, and it is the fluid counterpart of the classical fact that the age of a stationary renewal process has density 1−G1-G1−G. Part (1) gives the transient behavior of an underloaded or critically loaded system started empty.

The result is proved in the paper; nothing here is open. To our knowledge none of it has been formalized. A formalization adds machine-checked statements of a measure-valued fluid model that the companion mission (uniqueness of fluid solutions, Theorem 3.5) shares, and exercises renewal theory — the renewal measure, a key renewal theorem for laws with a density, Lorden's inequality — in a form usable by other queueing developments.

Difficulty

The naive argument would show that ⟨f,νˉt⟩\langle f,\bar\nu_t\rangle⟨f,νˉt​⟩ is given by an explicit formula and pass to the limit. The explicit age representation of a solution involves Kˉ\bar KKˉ, which is known only through a renewal equation whose forcing term depends on νˉ\bar\nuνˉ itself; there is no closed form unless the system never fills up. For Eˉ=id\bar E=\mathrm{id}Eˉ=id the system can alternate between full and not full, and the convergence must be proved without knowing when. Two ingredients carry the weight: a comparison showing that the occupancy tends to one, and a key renewal theorem for the backward recurrence time of a renewal process with a density, which needs total-variation rather than vague convergence because the test functions are only bounded and continuous. The uniform-in-time control of Lemma 6.3 is where the second moment enters.

Formalization scope

Everything lives in ManyServerFluid.Equilibrium. The service law is a structure holding the density ggg with g≥0g\ge0g≥0, g=0g=0g=0 on (−∞,0)(-\infty,0)(−∞,0), ∫g=1\int g=1∫g=1, and mean one. Time is R\mathbb RR, read on [0,∞)[0,\infty)[0,∞). Age measures are Mathlib FiniteMeasure ℝ carried by [0,M)[0,M)[0,M), with the weak topology, so "càdlàg" is in the paper's topology. The departures ∫0t⟨h,νˉs⟩ds\int_0^t\langle h,\bar\nu_s\rangle ds∫0t​⟨h,νˉs​⟩ds are lower integrals in [0,∞][0,\infty][0,∞]; dKˉd\bar KdKˉ and dZdZdZ are Lebesgue–Stieltjes measures. The convolution powers are the published QueueingFundamentals.MG1.convPow.

Explicit choices, each also stated in the item that uses it:

  • g=0g=0g=0 below 000 and ∫g=1\int g=1∫g=1 are explicit; the paper's "νˉ0\bar\nu_0νˉ0​" is νˉ(0)\bar\nu(0)νˉ(0), stated as an equation.
  • Compact support of test functions is relative to [0,M)×R+[0,M)\times\mathbb R_+[0,M)×R+​, as the paper intends; the directional derivative is supplied as a second function.
  • Weak convergence is tested on bounded continuous functions on R\mathbb RR; for measures carried by [0,M)[0,M)[0,M) this is equivalent to Cb[0,M)\mathcal C_b[0,M)Cb​[0,M) and Cb(R+)\mathcal C_b(\mathbb R_+)Cb​(R+​). "Increases" means nondecreasing.
  • "The unique solution" is the hypothesis "a solution"; uniqueness is the companion mission.
  • In Proposition 6.1(1) the printed limit ∫0τ1f(t−s)⋯\int_0^{\tau_1}f(t-s)\cdots∫0τ1​​f(t−s)⋯ is read with τ1\tau_1τ1​ for ttt, and only for τ1<∞\tau_1<\inftyτ1​<∞.
  • In Lemma 6.3 the free ttt of (6.11) is quantified after ∃Tε\exists T_\varepsilon∃Tε​, uniformly, as the proof establishes and uses.
  • Lemma 6.2 states that Z∈I0Z\in\mathcal I_0Z∈I0​ and that a càdlàg family satisfying (6.6) exists, besides (6.7).
  • Remark 3.8 is stated as membership in the solution set, the conclusion the paper draws.

Weak convergence in Theorem 3.9(2) is against all bounded continuous functions, not compactly supported ones; vague convergence would let mass escape towards MMM and is not the theorem. The monotonicity in part (1) is part of the statement. A formalization in which these were dropped, or in which UUU omitted the unit mass at 000, would state a different result.

Existence. The paper's proof of Theorem 3.9(2) compares an arbitrary solution with the solution started empty, which it obtains from its Theorem 3.7 (existence via the NNN-server limit); that theorem is not part of this series. Here every solution is a hypothesis, so nothing false is stated, but a proof of the goal must construct the empty-start solution for Eˉ=id\bar E=\mathrm{id}Eˉ=id. It is explicit: νˉt\bar\nu_tνˉt​ has density 1−G1-G1−G on [0,t][0,t][0,t] while t<τ1t<\tau_1t<τ1​, and from τ1=M<∞\tau_1=M<\inftyτ1​=M<∞ on it equals νˉ∗\bar\nu_*νˉ∗​ (Proposition 6.1, Remark 3.8, Lemma 3.4).

Contributions welcome: general renewal theory (local finiteness of UUU, Lorden's inequality, the key renewal theorem for spread-out laws in total variation), and lemmas on the fluid equations shared with the uniqueness mission (the monotonicity of Kˉ\bar KKˉ, the renewal equation (4.5), the age representation (3.11)).

Selected references

  • H. Kaspi and K. Ramanan, Law of Large Numbers Limits for Many-Server Queues, Ann. Appl. Probab. 21(1) (2011) 33–114. https://doi.org/10.1214/09-AAP662
  • W. Whitt, Fluid Models for Multiserver Queues with Abandonments, Oper. Res. 54 (2006) 37–54. https://mathscinet.ams.org/mathscinet-getitem?mr=2201245
  • L. Brown, N. Gans, A. Mandelbaum, A. Sakov, H. Shen, S. Zeltyn and L. Zhao, Statistical analysis of a telephone call center: A queueing-science perspective, J. Amer. Statist. Assoc. 100 (2005) 36–50. https://mathscinet.ams.org/mathscinet-getitem?mr=2166068
  • J. Reed, The G/GI/N queue in the Halfin–Whitt regime, Ann. Appl. Probab. 19 (2009) 2211–2269. https://mathscinet.ams.org/mathscinet-getitem?mr=2588244
  • S. Asmussen, Applied Probability and Queues, 2nd ed., Springer, 2003. https://mathscinet.ams.org/mathscinet-getitem?mr=1978607
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Functional AnalysisProbability·Captain: mikedeng1

Affine Processes on Positive Semidefinite Matrices III: For d ≥ 2, a Markov Family Is Infinitely Decomposable Iff It Is Affine with Zero Diffusion Iff It Is Affine and Infinitely DivisibleResearch Paper

Motivation

Affine processes are Markov processes whose Laplace transform depends exponential-affinely on the initial state. On the cone Sd+S_d^+Sd+​ of positive semidefinite matrices they model stochastic covariance matrices in multivariate stochastic volatility, interest-rate and credit models. Examples include the Wishart process of Bru (Bru 1991) and Ornstein–Uhlenbeck processes driven by matrix Lévy subordinators (Barndorff-Nielsen and Stelzer 2007, reference [3] of the paper). Cuchiero, Filipović, Mayerhofer and Teichmann (2011) characterize all affine processes on Sd+S_d^+Sd+​ by admissible parameter sets.

On the canonical state space R+m×Rn\mathbb R_+^m\times\mathbb R^nR+m​×Rn, Duffie, Filipović and Schachermayer (2003) showed that regular affine processes are exactly the infinitely decomposable Markov processes: the law started at x(1)+⋯+x(k)x^{(1)}+\dots+x^{(k)}x(1)+⋯+x(k) is a kkk-fold convolution of laws started at the x(i)x^{(i)}x(i). That property drives their existence proof. On Sd+S_d^+Sd+​ with d≥2d\ge2d≥2 it fails. The Wishart marginals are not infinitely divisible, a classical result of Paul Lévy. This mission formalizes the exact characterization: Theorem 2.9 of Cuchiero et al.

Setting

MdM_dMd​ is the space of real d×dd\times dd×d matrices and SdS_dSd​ the symmetric ones. SdS_dSd​ carries the pairing ⟨x,y⟩=Tr(xy)\langle x,y\rangle=\mathrm{Tr}(xy)⟨x,y⟩=Tr(xy) and the norm ∥x∥=⟨x,x⟩\|x\|=\sqrt{\langle x,x\rangle}∥x∥=⟨x,x⟩​. Sd+S_d^+Sd+​ is the closed convex cone of positive semidefinite matrices, and Sd+∪{Δ}S_d^+\cup\{\Delta\}Sd+​∪{Δ} its one-point compactification. The point Δ\DeltaΔ is the cemetery, where a killed process goes.

A transition family (pt)t≥0(p_t)_{t\ge0}(pt​)t≥0​ consists of sub-stochastic kernels on Sd+S_d^+Sd+​ satisfying p0(x,⋅)=δxp_0(x,\cdot)=\delta_xp0​(x,⋅)=δx​ and the Chapman–Kolmogorov equations. It is stochastically continuous if ps(x,⋅)→pt(x,⋅)p_s(x,\cdot)\to p_t(x,\cdot)ps​(x,⋅)→pt​(x,⋅) weakly as s→ts\to ts→t. The process is affine (Definition 2.1) if there are φ≥0\varphi\ge0φ≥0 and ψ∈Sd+\psi\in S_d^+ψ∈Sd+​ with

∫e−⟨u,ξ⟩pt(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+.\int e^{-\langle u,\xi\rangle}p_t(x,d\xi)=e^{-\varphi(t,u)-\langle\psi(t,u),x\rangle},\qquad t\ge0,\ u,x\in S_d^+.∫e−⟨u,ξ⟩pt​(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+​.

Theorem 2.4 of the paper attaches to every affine process a unique admissible parameter set (α,b,βij,c,γ,m,μ)(\alpha,b,\beta^{ij},c,\gamma,m,\mu)(α,b,βij,c,γ,m,μ). In it, α∈Sd+\alpha\in S_d^+α∈Sd+​ is the diffusion parameter, b⪰(d−1)αb\succeq(d-1)\alphab⪰(d−1)α the constant drift, ccc and γ\gammaγ the killing rates, and mmm and μ\muμ the jump measures. The exponents solve the generalized Riccati equations ∂tφ=F(ψ)\partial_t\varphi=F(\psi)∂t​φ=F(ψ), ∂tψ=R(ψ)\partial_t\psi=R(\psi)∂t​ψ=R(ψ), with F,RF,RF,R given by (2.16)–(2.17).

The canonical space Ω\OmegaΩ consists of paths ω:R+→Sd+∪{Δ}\omega:\mathbb R_+\to S_d^+\cup\{\Delta\}ω:R+​→Sd+​∪{Δ} that stay at Δ\DeltaΔ once they reach it, with coordinate process Xt(ω)=ω(t)X_t(\omega)=\omega(t)Xt​(ω)=ω(t). P\mathcal PP is the set of families (Px)x∈Sd+(P_x)_{x\in S_d^+}(Px​)x∈Sd+​​ of laws on Ω\OmegaΩ under which XXX is a stochastically continuous Markov process with Px[X0=x]=1P_x[X_0=x]=1Px​[X0​=x]=1. The convolution P∗QP*QP∗Q is the image of P×QP\times QP×Q under (ω,ω′)↦ω+ω′(\omega,\omega')\mapsto\omega+\omega'(ω,ω′)↦ω+ω′. A family (Px)∈P(P_x)\in\mathcal P(Px​)∈P is infinitely decomposable (Definition 2.7) if for every k≥1k\ge1k≥1 there is (Px(k))∈P(P^{(k)}_x)\in\mathcal P(Px(k)​)∈P with Px(1)+⋯+x(k)=Px(1)(k)∗⋯∗Px(k)(k)P_{x^{(1)}+\dots+x^{(k)}}=P^{(k)}_{x^{(1)}}*\dots*P^{(k)}_{x^{(k)}}Px(1)+⋯+x(k)​=Px(1)(k)​∗⋯∗Px(k)(k)​. It is infinitely divisible if every marginal Px∘Xt−1P_x\circ X_t^{-1}Px​∘Xt−1​ is.

Formalization targets

Goal: Theorem 2.9 (p. 12)

For d≥2d\ge2d≥2 and (Px)∈P(P_x)\in\mathcal P(Px​)∈P, the following are equivalent:

(i) (Px) is infinitely decomposable  ⟺  (ii) X is affine with α=0  ⟺  (iii) X is affine and infinitely divisible.\text{(i) }(P_x)\text{ is infinitely decomposable}\iff\text{(ii) }X\text{ is affine with }\alpha=0\iff\text{(iii) }X\text{ is affine and infinitely divisible}.(i) (Px​) is infinitely decomposable⟺(ii) X is affine with α=0⟺(iii) X is affine and infinitely divisible.

Milestones

  • Lemma 6.1. An additive g:Sd+→Rg:S_d^+\to\mathbb Rg:Sd+​→R extends to an additive f:Sd→Rf:S_d\to\mathbb Rf:Sd​→R. If ggg is measurable, then f(x)=⟨c,x⟩f(x)=\langle c,x\ranglef(x)=⟨c,x⟩ for some c∈Sdc\in S_dc∈Sd​.
  • Lemma 6.2. A measurable, strictly positive hhh with h(x+y)=h(x)h(y)h(x+y)=h(x)h(y)h(x+y)=h(x)h(y) on Sd+S_d^+Sd+​ has the form h(x)=e−⟨c,x⟩h(x)=e^{-\langle c,x\rangle}h(x)=e−⟨c,x⟩, c∈Sdc\in S_dc∈Sd​. If h≤1h\le1h≤1, then c∈Sd+c\in S_d^+c∈Sd+​.
  • Lemma 6.4. For k≥2k\ge2k≥2, Px(1)(1)∗⋯∗Px(k)(k)=Px(0)P^{(1)}_{x^{(1)}}*\dots*P^{(k)}_{x^{(k)}}=P^{(0)}_{x}Px(1)(1)​∗⋯∗Px(k)(k)​=Px(0)​ holds iff every finite-dimensional Laplace functional has the form Ex(j)[e−∑i⟨u(i),Xti⟩]=ρ(j)e−⟨ψ,x⟩\mathbb E^{(j)}_x[e^{-\sum_i\langle u^{(i)},X_{t_i}\rangle}]=\rho^{(j)}e^{-\langle\psi,x\rangle}Ex(j)​[e−∑i​⟨u(i),Xti​​⟩]=ρ(j)e−⟨ψ,x⟩ with ∏i≥1ρ(i)=ρ(0)\prod_{i\ge1}\rho^{(i)}=\rho^{(0)}∏i≥1​ρ(i)=ρ(0).
  • Lemma 5.10. The cones C\mathcal CC (Lévy–Khintchine exponents plus a constant) and CS\mathcal C^SCS are closed under composition and pointwise limits. For α=0\alpha=0α=0, truncating small jumps of μ\muμ approximates RRR locally uniformly.
  • Proposition 5.11. For an admissible parameter set with α=0\alpha=0α=0, (φ(t,⋅),ψ(t,⋅))∈(C,CS)(\varphi(t,\cdot),\psi(t,\cdot))\in(\mathcal C,\mathcal C^S)(φ(t,⋅),ψ(t,⋅))∈(C,CS) for every t≥0t\ge0t≥0.

Significance

The theorem separates two classes that coincide on R+m×Rn\mathbb R_+^m\times\mathbb R^nR+m​×Rn. On Sd+S_d^+Sd+​ with d≥2d\ge2d≥2, a diffusion component, which must satisfy b⪰(d−1)αb\succeq(d-1)\alphab⪰(d−1)α, is incompatible with taking kkk-th roots, because the root would need drift b/kb/kb/k. So the existence proof of Duffie–Filipović–Schachermayer, which builds a process from infinitely divisible kernels, covers exactly the pure-jump affine processes on Sd+S_d^+Sd+​. Processes with a diffusion part need the martingale-problem approach of the paper's §5. Proposition 5.11 gives the alternative existence proof for α=0\alpha=0α=0 (§5.3).

The theorem is proved in the paper. As far as is known, none of it has been machine-checked: no formal library has affine processes on matrix cones, convolution of path measures, or the Lévy–Khintchine form on Sd+S_d^+Sd+​. Formalization contributes a checked equivalence that rests on the paper's other main theorem (Theorem 2.4), together with reusable statements about Cauchy's equations on cones and Laplace functionals of Markov families. It is the third mission of a series. Missions I and II formalize the two halves of Theorem 2.4.

Difficulty

The equivalence links three layers: path-space laws, one-dimensional kernels, and Riccati exponents. (i) ⇒\Rightarrow⇒ (ii) first needs the multiplicative structure of Laplace functionals in the initial state. That gives affinity of the process and of each kkk-th root, with exponents (φ/k,ψ)(\varphi/k,\psi)(φ/k,ψ). Then it needs the fact that the root's parameter set is (α,b/k,… )(\alpha,b/k,\dots)(α,b/k,…) and is again admissible, so b/k⪰(d−1)αb/k\succeq(d-1)\alphab/k⪰(d−1)α for all kkk. The second step relies on the full necessity theorem, in particular Proposition 4.18. The first fails without strict positivity of the Laplace functional: Cauchy's exponential equation has non-exponential solutions that vanish somewhere (Remark 6.3). (ii) ⇒\Rightarrow⇒ (iii) requires every Riccati solution to stay in the Lévy–Khintchine cone. This is clear for finite-variation jumps via Picard iteration, but the general case needs the approximation Rδ→RR^\delta\to RRδ→R. (iii) ⇒\Rightarrow⇒ (i) must produce a Markov family of kkk-th roots on path space, not merely roots of each marginal. The case d=1d=1d=1 shows that d≥2d\ge2d≥2 cannot be dropped: there the Cox–Ingersoll–Ross process has α≠0\alpha\ne0α=0 and is infinitely decomposable.

Formalization scope

  • Matrices. MdM_dMd​ is Fin d → Fin d → ℝ, with ⟨x,y⟩=∑i,jxijyji\langle x,y\rangle=\sum_{i,j}x_{ij}y_{ji}⟨x,y⟩=∑i,j​xij​yji​ and ∥x∥=⟨x,x⟩\|x\|=\sqrt{\langle x,x\rangle}∥x∥=⟨x,x⟩​. Sd+S_d^+Sd+​ is the subtype of matrices with Mathlib's PosSemidef.
  • Parameters. The matrix measure μ\muμ is encoded as H dνH\,d\nuHdν, with ν\nuν finite and HHH a positive semidefinite density. This is equivalent to the paper's μ\muμ; take ν=∑iμii\nu=\sum_i\mu_{ii}ν=∑i​μii​. Exponents are functions on R×Md\mathbb R\times M_dR×Md​, evaluated at t≥0t\ge0t≥0 and positive semidefinite uuu. Time derivatives at t=0t=0t=0 are one-sided.
  • Path space. Sd+∪{Δ}S_d^+\cup\{\Delta\}Sd+​∪{Δ} is OnePoint of the cone, with its Borel σ-algebra. Addition is extended with Δ\DeltaΔ absorbing. Ω\OmegaΩ is the space of all paths R≥0→Sd+∪{Δ}\mathbb R_{\ge0}\to S_d^+\cup\{\Delta\}R≥0​→Sd+​∪{Δ} with the product σ-algebra; every notion in the theorem depends only on finite-dimensional distributions. Absorption at Δ\DeltaΔ and the Markov property with transition family ppp are imposed through finite-dimensional distributions. The path-sum map is measurable, which is checked in Lean, so the convolution is a genuine push-forward.
  • Marginals. Infinite divisibility of a marginal is that of the sub-probability kernel pt(x,⋅)p_t(x,\cdot)pt​(x,⋅). Killed mass sits at Δ\DeltaΔ, so roots are sub-probabilities.
  • The parameter set. "Affine with α=0\alpha=0α=0" refers to the unique admissible parameter set whose F,RF,RF,R drive the Riccati equations. The truncation function χ\chiχ is arbitrary.
  • Corrections to the page. Lemma 6.4 carries the hypothesis k≥2k\ge2k≥2, from its proof ("Fix k>1k>1k>1"). For k=1k=1k=1 the statement is false. In Proposition 5.11, "the solutions" are the jointly continuous ones.
  • Ruled out. A kernel-level identity in place of infinite decomposability is ruled out: (i) is stated on path space. The goal keeps the hypothesis d≥2d\ge2d≥2.
  • Reusable work. Contributions are welcome on Cauchy's equations on cones (Lemmas 6.1–6.2), on the measure theory of path convolutions, and on Lévy–Khintchine exponents on Sd+S_d^+Sd+​. All three are useful beyond this mission.

Selected references

  • C. Cuchiero, D. Filipović, E. Mayerhofer, J. Teichmann, Affine processes on positive semidefinite matrices, Ann. Appl. Probab. 21 (2011) 397–463; arXiv:0910.0137v3. https://arxiv.org/abs/0910.0137
  • D. Duffie, D. Filipović, W. Schachermayer, Affine processes and applications in finance, Ann. Appl. Probab. 13 (2003) 984–1053. https://doi.org/10.1214/aoap/1060202833
  • M.-F. Bru, Wishart processes, J. Theoret. Probab. 4 (1991) 725–751. https://doi.org/10.1007/BF01259552
  • O. E. Barndorff-Nielsen, R. Stelzer, Positive-definite matrix processes of finite variation, Probab. Math. Statist. 27 (2007) 3–43.
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Probability·Captain: marwahaha

A directional zero–one law under strict ellipticityOpen Problem

Motivation

A random environment can favor different directions at different sites. The source asks whether escape in one prescribed real direction can have an intermediate probability after averaging over the environment. The source is OpenAI's September 2026 manuscript.

Setting

A transition row assigns probabilities to the nearest-neighbor steps of the integer lattice. Rows at different sites are independent and have the same law. Strict ellipticity means every step probability is positive almost surely, without a common positive lower bound.

Formalization targets

P0 ⁣(⟨Xn,ℓ⟩→+∞)∈{0,1}(d≥3, ℓ≠0).\mathbb P_0\!\left(\langle X_n,\ell\rangle\to+\infty\right)\in\{0,1\}\qquad(d\ge3,\ \ell\ne0).P0​(⟨Xn​,ℓ⟩→+∞)∈{0,1}(d≥3, ℓ=0).

For every dimension d ≥ 3, a random walk in an i.i.d. random environment on the lattice ℤ^d obeys a directional zero-one law. Here a row at a site is a probability vector p on the 2d nearest-neighbour steps (coordinate direction i in Fin d, sign + or −), with each p(e) in [0,1] and the entries summing to 1. The environment assigns an independent row to every site, each drawn from a probability measure μ on rows, and the strict ellipticity hypothesis on μ says that μ-almost every row gives every one of the 2d steps strictly positive probability. Given the environment, the walker at site x moves to x plus the unit vector of step e with probability p_x(e); the annealed law of the path started at 0 averages over both the environment and the walk. For any nonzero real vector ℓ in ℝ^d, the escape event is that the path X satisfies Σᵢ Xₙ(i)·ℓᵢ → +∞ as n → ∞, that is, the walk tends to infinity in the direction ℓ. The conclusion is that the annealed probability of this event, starting from 0, is either exactly 0 or exactly 1.

The goal is OAI.DirectionalZeroOne.directional_zero_one.

Significance

The target gives a directional zero–one law under positivity alone. It makes no moment or uniform ellipticity assumption. The manuscript presents a mathematical argument; the attached goal currently has status Open, so the requested contribution is a Lean proof of the displayed formal target.

Difficulty

Revisiting sites reuses the same random transition row, so path increments are not independent under the averaged law. Ordinary zero–one laws for independent increments do not directly apply.

Formalization scope

Lean builds the annealed path measure through a Markov kernel on environment-position pairs. The starting site is the origin, the direction is any nonzero real vector, and escape means the scalar projection tends to positive infinity.

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

Selected references

  • OpenAI, A directional zero–one law under strict ellipticity, preprint, September 2026. Manuscript.
  • OpenAI, accompanying Lean statement. Pinned source.
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Functional AnalysisProbability·Captain: mikedeng1

Affine Processes on Positive Semidefinite Matrices I: Every Affine Process on the PSD Cone Is Regular and Feller, with Generator (2.12) Given by an Admissible Parameter SetResearch Paper

Motivation

Matrix-valued affine processes on the cone of positive semidefinite matrices are used in finance as models of stochastic covariance: multi-asset option pricing with stochastic volatility and correlation, and fixed-income models with stochastically correlated risk factors and default intensities. The best-known example is the Wishart process of Bru (1991). What makes these models tractable is that the Laplace transform of the state is exponential-affine in the initial state, with exponents that solve ordinary differential equations of Riccati type.

Cuchiero, Filipović, Mayerhofer and Teichmann (2011) give the mathematical foundation: a complete characterization of stochastically continuous affine processes on Sd+S_d^+Sd+​ through an admissible parameter set. Their Theorem 2.4 has two halves. This mission formalizes the first, necessity, half: every affine process on Sd+S_d^+Sd+​ is regular and Feller, and its generator and Riccati equations are given by an admissible parameter set.

Timeline. Duffie, Filipović and Schachermayer (2003) characterized regular affine processes on the canonical state space R+m×Rn\mathbb R_+^m \times \mathbb R^nR+m​×Rn, assuming regularity. Keller-Ressel, Schachermayer and Teichmann showed that on that state space stochastic continuity already implies regularity. The 2011 paper carries both the characterization and the regularity result over to Sd+S_d^+Sd+​, a non-polyhedral cone with a curved boundary, on which the drift must satisfy the new condition b⪰(d−1)αb \succeq (d-1)\alphab⪰(d−1)α.

Setting

Let SdS_dSd​ be the space of real symmetric d×dd\times dd×d matrices with scalar product ⟨x,y⟩=Tr(xy)\langle x,y\rangle = \mathrm{Tr}(xy)⟨x,y⟩=Tr(xy) and norm ∥x∥=⟨x,x⟩1/2\|x\| = \langle x,x\rangle^{1/2}∥x∥=⟨x,x⟩1/2. Let Sd+S_d^+Sd+​ be the cone of positive semidefinite matrices and Sd++S_d^{++}Sd++​ its interior, and write x⪯yx \preceq yx⪯y when y−x∈Sd+y - x \in S_d^+y−x∈Sd+​.

A time-homogeneous Markov process XXX on Sd+S_d^+Sd+​ is described by sub-stochastic transition kernels pt(x,dξ)p_t(x,d\xi)pt​(x,dξ), t≥0t\ge 0t≥0. Mass that is lost goes to a cemetery state Δ\DeltaΔ. The kernels satisfy the Chapman–Kolmogorov equations, and the semigroup is Ptf(x)=∫f(ξ) pt(x,dξ)P_tf(x) = \int f(\xi)\,p_t(x,d\xi)Pt​f(x)=∫f(ξ)pt​(x,dξ). The process is affine (Definition 2.1) if it is stochastically continuous, i.e. ps(x,⋅)→pt(x,⋅)p_s(x,\cdot) \to p_t(x,\cdot)ps​(x,⋅)→pt​(x,⋅) weakly as s→ts \to ts→t, and if there are φ:R+×Sd+→R+\varphi : \mathbb R_+ \times S_d^+ \to \mathbb R_+φ:R+​×Sd+​→R+​ and ψ:R+×Sd+→Sd+\psi : \mathbb R_+\times S_d^+ \to S_d^+ψ:R+​×Sd+​→Sd+​ with

∫Sd+e−⟨u,ξ⟩ pt(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+.\int_{S_d^+} e^{-\langle u,\xi\rangle}\,p_t(x,d\xi) = e^{-\varphi(t,u) - \langle\psi(t,u),x\rangle}, \qquad t\ge0,\ u,x\in S_d^+.∫Sd+​​e−⟨u,ξ⟩pt​(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+​.

It is regular (Definition 2.2) if F(u)=∂tφ(t,u)∣t=0+F(u) = \partial_t\varphi(t,u)|_{t=0+}F(u)=∂t​φ(t,u)∣t=0+​ and R(u)=∂tψ(t,u)∣t=0+R(u) = \partial_t\psi(t,u)|_{t=0+}R(u)=∂t​ψ(t,u)∣t=0+​ exist and are continuous at u=0u=0u=0.

An admissible parameter set (α,b,βij,c,γ,m,μ)(\alpha, b, \beta^{ij}, c, \gamma, m, \mu)(α,b,βij,c,γ,m,μ), associated with a bounded continuous truncation function χ\chiχ (equal to the identity near 000), consists of:

  • a diffusion coefficient α∈Sd+\alpha \in S_d^+α∈Sd+​ and a constant drift b⪰(d−1)αb \succeq (d-1)\alphab⪰(d−1)α;
  • killing rates c≥0c \ge 0c≥0 and γ∈Sd+\gamma \in S_d^+γ∈Sd+​;
  • a jump measure mmm with ∫(∥ξ∥∧1) m(dξ)<∞\int(\|\xi\|\wedge1)\,m(d\xi)<\infty∫(∥ξ∥∧1)m(dξ)<∞;
  • a matrix μ\muμ of finite signed measures with μ(E)∈Sd+\mu(E) \in S_d^+μ(E)∈Sd+​, defining M(x,dξ)=⟨x,μ(dξ)⟩/(∥ξ∥2∧1)M(x,d\xi) = \langle x,\mu(d\xi)\rangle/(\|\xi\|^2\wedge1)M(x,dξ)=⟨x,μ(dξ)⟩/(∥ξ∥2∧1);
  • a linear drift B(x)=∑i,jβijxijB(x) = \sum_{i,j}\beta^{ij}x_{ij}B(x)=∑i,j​βijxij​.

These are subject to the boundary conditions (2.9) and (2.11) for x,u∈Sd+x,u \in S_d^+x,u∈Sd+​ with ⟨x,u⟩=0\langle x,u\rangle = 0⟨x,u⟩=0. The space S+\mathcal S_+S+​ consists of restrictions to Sd+S_d^+Sd+​ of rapidly decreasing smooth functions on SdS_dSd​.

Formalization targets

Goal: Theorem 2.4, first part

If XXX is affine on Sd+S_d^+Sd+​, then XXX is regular and Feller, S+\mathcal S_+S+​ lies in the domain of its generator A\mathcal AA on C0(Sd+)C_0(S_d^+)C0​(Sd+​), and there is an admissible parameter set such that for f∈S+f \in \mathcal S_+f∈S+​

Af(x)=12∑Aijkl(x) ∂ij∂klf(x)+∑(bij+Bij(x)) ∂ijf(x)−(c+⟨γ,x⟩)f(x)+∫(f(x+ξ)−f(x)) m(dξ)+∫(f(x+ξ)−f(x)−⟨χ(ξ),∇f(x)⟩) M(x,dξ),\mathcal Af(x) = \tfrac12\sum A_{ijkl}(x)\,\partial_{ij}\partial_{kl}f(x) + \sum (b_{ij}+B_{ij}(x))\,\partial_{ij}f(x) - (c+\langle\gamma,x\rangle)f(x) + \int (f(x+\xi)-f(x))\,m(d\xi) + \int \big(f(x+\xi)-f(x)-\langle\chi(\xi),\nabla f(x)\rangle\big)\,M(x,d\xi),Af(x)=21​∑Aijkl​(x)∂ij​∂kl​f(x)+∑(bij​+Bij​(x))∂ij​f(x)−(c+⟨γ,x⟩)f(x)+∫(f(x+ξ)−f(x))m(dξ)+∫(f(x+ξ)−f(x)−⟨χ(ξ),∇f(x)⟩)M(x,dξ),

with Aijkl(x)=xikαjl+xilαjk+xjkαil+xjlαikA_{ijkl}(x) = x_{ik}\alpha_{jl}+x_{il}\alpha_{jk}+x_{jk}\alpha_{il}+x_{jl}\alpha_{ik}Aijkl​(x)=xik​αjl​+xil​αjk​+xjk​αil​+xjl​αik​. In addition, φ,ψ\varphi,\psiφ,ψ solve ∂tφ=F(ψ)\partial_t\varphi = F(\psi)∂t​φ=F(ψ), φ(0,u)=0\varphi(0,u)=0φ(0,u)=0, ∂tψ=R(ψ)\partial_t\psi = R(\psi)∂t​ψ=R(ψ), ψ(0,u)=u\psi(0,u) = uψ(0,u)=u, with

F(u)=⟨b,u⟩+c−∫(e−⟨u,ξ⟩−1) m(dξ),R(u)=−2uαu+B⊤(u)+γ−∫e−⟨u,ξ⟩−1+⟨χ(ξ),u⟩∥ξ∥2∧1 μ(dξ).F(u) = \langle b,u\rangle + c - \int (e^{-\langle u,\xi\rangle}-1)\,m(d\xi),\qquad R(u) = -2u\alpha u + B^\top(u) + \gamma - \int \frac{e^{-\langle u,\xi\rangle}-1+\langle\chi(\xi),u\rangle}{\|\xi\|^2\wedge1}\,\mu(d\xi).F(u)=⟨b,u⟩+c−∫(e−⟨u,ξ⟩−1)m(dξ),R(u)=−2uαu+B⊤(u)+γ−∫∥ξ∥2∧1e−⟨u,ξ⟩−1+⟨χ(ξ),u⟩​μ(dξ).

Milestones, in attack order

  1. Lemma 3.1 and Lemma 3.3: order-preserving, continuous, analytic semiflows map Sd++S_d^{++}Sd++​ into Sd++S_d^{++}Sd++​.
  2. Lemma 3.2: semiflow identities, monotonicity, continuity and analyticity of φ,ψ\varphi,\psiφ,ψ.
  3. Proposition 3.4: Feller and regular.
  4. Lemmas 4.1 and 4.4: zero divisors in the cone, and linear extension of additive maps.
  5. Proposition 4.9: F,RF,RF,R have the form (2.16)–(2.17) with b∈Sd+b\in S_d^+b∈Sd+​.
  6. Lemma B.2 and Theorem B.3: exponentials lie in S+\mathcal S_+S+​ and span a dense subspace.
  7. Proposition 4.12: the generator formula (2.12) on S+\mathcal S_+S+​.
  8. Lemma 4.17 and Proposition 4.18: derivatives of det⁡\detdet at diagonal matrices, and the drift condition b⪰(d−1)αb\succeq(d-1)\alphab⪰(d−1)α.

Significance

The result. Theorem 2.4 reduces the study of affine processes on Sd+S_d^+Sd+​ to finitely many parameters. Any such process, a priori specified only through its Laplace transform, has the Lévy–Khintchine-type generator (2.12), its Laplace exponents solve the Riccati system, and its parameters obey the admissibility conditions. The drift condition b⪰(d−1)αb\succeq(d-1)\alphab⪰(d−1)α is the matrix analogue of the Feller condition, and for d≥2d\ge2d≥2 it excludes affine diffusions on Sd+S_d^+Sd+​ with zero constant drift. The Feller property yields càdlàg versions, and the generator formula is the starting point for the semimartingale description and for the converse existence result.

Formalizing it. The theorem is proved in the paper, and this mission produces a machine-checked version of the necessity direction. Along the way it builds reusable infrastructure: a Lean model of Markov transition families on a cone, Feller semigroups on C0C_0C0​ of a closed cone, generators on Schwartz-type test spaces with the symmetric-matrix derivative convention, and the positive semidefinite cone's order and boundary facts. No machine-checked proof of this theorem, or of its R+m×Rn\mathbb R_+^m\times\mathbb R^nR+m​×Rn predecessor, is known to exist.

Difficulty

The definition assumes only stochastic continuity and the exponential-affine form of the Laplace transform; differentiability in time is not given. Obtaining regularity, and hence the Riccati equations, needs the positivity statement of Lemma 3.3. Its proof uses analyticity in uuu and the boundary geometry of Sd+S_d^+Sd+​. Identifying FFF and RRR requires Lévy–Khintchine representations on cones and on SdS_dSd​, and a convergence theorem for Laplace transforms. The admissibility conditions on the boundary come from support considerations at each boundary point. The drift condition (2.4) is not captured by the conditions read off from Laplace exponents at boundary points along single directions; it is a genuinely matrix-valued constraint coupling bbb and α\alphaα. Extending the generator formula from exponentials to all of S+\mathcal S_+S+​ needs a density result in a Fréchet topology and the closedness of the generator.

Formalization scope

  • Matrices are Fin d → Fin d → ℝ, with ⟨x,y⟩=∑xijyji\langle x,y\rangle=\sum x_{ij}y_{ji}⟨x,y⟩=∑xij​yji​ and ∥x∥=⟨x,x⟩1/2\|x\|=\langle x,x\rangle^{1/2}∥x∥=⟨x,x⟩1/2. Mathlib's positive semidefiniteness, which includes symmetry over R\mathbb RR, defines Sd+S_d^+Sd+​. The state space is the subtype Sd+S_d^+Sd+​ with its subspace topology and Borel σ\sigmaσ-algebra.
  • Transition families are Mathlib kernels indexed by t∈Rt\in\mathbb Rt∈R and constrained only for t≥0t\ge0t≥0. Sub-stochasticity encodes the cemetery. Stochastic continuity is convergence of integrals of bounded continuous functions as s→ts\to ts→t within [0,∞)[0,\infty)[0,∞).
  • The exponents φ,ψ\varphi,\psiφ,ψ are functions on R×Md\mathbb R\times M_dR×Md​, used at t≥0t\ge0t≥0 and positive semidefinite arguments. Analyticity on Sd++S_d^{++}Sd++​ is analyticity of y↦ψ(t,(y+y⊤)/2)y\mapsto\psi(t,(y+y^\top)/2)y↦ψ(t,(y+y⊤)/2) on an open subset of MdM_dMd​.
  • The matrix measure μ\muμ is encoded as H dνH\,d\nuHdν with ν\nuν finite and HHH positive semidefinite and integrable. This loses nothing, since ν=∑iμii\nu = \sum_i\mu_{ii}ν=∑i​μii​ dominates every μij\mu_{ij}μij​.
  • S+\mathcal S_+S+​ is the set of restrictions of Schwartz functions on MdM_dMd​. Partial derivatives ∂/∂xij\partial/\partial x_{ij}∂/∂xij​ of functions on SdS_dSd​ are taken in the direction 12(Eij+Eji)\tfrac12(E^{ij}+E^{ji})21​(Eij+Eji), per §1.2 of the paper. Lemma 4.17 alone uses raw entry derivatives of det⁡\detdet on MdM_dMd​, as its proof does.
  • The Feller property uses the platform definition EthierKurtz.IsStronglyContinuousContractionSemigroup on C0(Sd+)C_0(S_d^+)C0​(Sd+​). "f∈D(A)f\in D(\mathcal A)f∈D(A) and Af=g\mathcal Af=gAf=g" is uniform convergence of (Ptf−f)/t(P_tf-f)/t(Pt​f−f)/t to ggg on Sd+S_d^+Sd+​.
  • Lean assigns the value 000 to the integral of a non-integrable function. Wherever a statement concludes a formula containing an integral, it therefore also concludes integrability of the integrand, so the formula cannot hold through this default value. Regularity and the Feller property are conclusions, never hypotheses, of the goal. The drift condition (2.4) is part of admissibility in the goal; Propositions 4.9, 4.12 and 4.18 use admissibility without (2.4) and b∈Sd+b\in S_d^+b∈Sd+​, as in the paper.
  • Contributions are welcome on any milestone. The matrix lemmas (3.1, 3.3, 4.1, 4.4, 4.17) are self-contained, and Lemma B.2 and Theorem B.3 concern only Schwartz functions.

Selected references

  • C. Cuchiero, D. Filipović, E. Mayerhofer, J. Teichmann, Affine processes on positive semidefinite matrices, Ann. Appl. Probab. 21 (2011) 397–463; cited as arXiv:0910.0137v3. https://arxiv.org/abs/0910.0137
  • D. Duffie, D. Filipović, W. Schachermayer, Affine processes and applications in finance, Ann. Appl. Probab. 13 (2003) 984–1053. https://doi.org/10.1214/aoap/1060202833
  • M. Keller-Ressel, W. Schachermayer, J. Teichmann, Affine processes are regular, Probab. Theory Related Fields 151 (2011) 591–611. https://arxiv.org/abs/0906.3392
  • M.-F. Bru, Wishart processes, J. Theoret. Probab. 4 (1991) 725–751. https://doi.org/10.1007/BF01259552
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AnalysisOperations ResearchProbability·Captain: mikedeng1

Law of Large Numbers Limits for Many-Server Queues 1: The Fluid Equations Have at Most One Solution, Given Explicitly by the Age Representation (3.11)Research Paper

Motivation

Large service systems such as call centers and hospital wards are modelled as many-server queues: NNN identical servers, customers arriving according to a general process, service requirements drawn independently from a general distribution GGG, and a single first-come-first-served queue. When GGG is not exponential the number of customers in system is not Markov, and a tractable state must keep track of how long each customer in service has been served. Kaspi and Ramanan (Ann. Appl. Probab. 21 (2011)) take as state the number in system together with the age measure, the point measure of the ages of the customers in service, and prove a functional law of large numbers: scaled by NNN, these processes converge to the unique solution of a deterministic system, the fluid equations. Earlier fluid and diffusion analyses of the G/GI/NG/GI/NG/GI/N queue worked with other state descriptors (Reed, Ann. Appl. Probab. 19 (2009); Whitt, Oper. Res. 54 (2006)); the measure-valued description records the elapsed service time of every customer in service, which is the information a non-exponential service distribution requires.

This mission covers the deterministic half of that result: the fluid equations are well posed, and their solution is given in closed form.

Setting

Service requirements have a density ggg that vanishes on (−∞,0)(-\infty,0)(−∞,0), G(x)=∫(−∞,x]gG(x)=\int_{(-\infty,x]}gG(x)=∫(−∞,x]​g, and the mean is normalized to one, ∫x g(x) dx=1\int x\,g(x)\,dx=1∫xg(x)dx=1. Let M=sup⁡{x≥0:G(x)<1}∈(0,∞]M=\sup\{x\ge0: G(x)<1\}\in(0,\infty]M=sup{x≥0:G(x)<1}∈(0,∞] and let h=g/(1−G)h=g/(1-G)h=g/(1−G) be the hazard rate on [0,M)[0,M)[0,M); hhh is locally integrable on [0,M)[0,M)[0,M) but not integrable on it. For a measure μ\muμ and a function fff write ⟨f,μ⟩=∫f dμ\langle f,\mu\rangle=\int f\,d\mu⟨f,μ⟩=∫fdμ, and 1\mathbf 11 for the constant one.

The data are a triple (Eˉ,Xˉ(0),νˉ0)(\bar E,\bar X(0),\bar\nu_0)(Eˉ,Xˉ(0),νˉ0​) in

S0={(f,x,μ):f nondecreasing caˋdlaˋg,f(0)=0; x≥0; μ a measure on [0,M), ⟨1,μ⟩≤1, 1−⟨1,μ⟩=[1−x]+},\mathcal S_0=\{(f,x,\mu): f \text{ nondecreasing càdlàg}, f(0)=0;\ x\ge0;\ \mu \text{ a measure on }[0,M),\ \langle\mathbf 1,\mu\rangle\le1,\ 1-\langle\mathbf 1,\mu\rangle=[1-x]^+\},S0​={(f,x,μ):f nondecreasing caˋdlaˋg,f(0)=0; x≥0; μ a measure on [0,M), ⟨1,μ⟩≤1, 1−⟨1,μ⟩=[1−x]+},

where Eˉ\bar EEˉ is the cumulative arrival process, Xˉ(0)\bar X(0)Xˉ(0) the initial number in system and νˉ0\bar\nu_0νˉ0​ the initial age measure (per server, so the total capacity is one). A càdlàg pair (Xˉ,νˉ)(\bar X,\bar\nu)(Xˉ,νˉ), with νˉt\bar\nu_tνˉt​ a sub-probability measure on [0,M)[0,M)[0,M) in the weak topology, solves the fluid equations if for every t≥0t\ge0t≥0: ∫0t⟨h,νˉs⟩ds<∞\int_0^t\langle h,\bar\nu_s\rangle ds<\infty∫0t​⟨h,νˉs​⟩ds<∞ (3.4); for every test function φ∈Cc1,1([0,M)×R+)\varphi\in\mathcal C_c^{1,1}([0,M)\times\mathbb R_+)φ∈Cc1,1​([0,M)×R+​)

⟨φ(⋅,t),νˉt⟩=⟨φ(⋅,0),νˉ0⟩+∫0t⟨φx+φs,νˉs⟩ds−∫0t⟨hφ(⋅,s),νˉs⟩ds+∫[0,t]φ(0,s) dKˉ(s)(3.5);\langle\varphi(\cdot,t),\bar\nu_t\rangle=\langle\varphi(\cdot,0),\bar\nu_0\rangle+\int_0^t\langle\varphi_x+\varphi_s,\bar\nu_s\rangle ds-\int_0^t\langle h\varphi(\cdot,s),\bar\nu_s\rangle ds+\int_{[0,t]}\varphi(0,s)\,d\bar K(s)\quad(3.5);⟨φ(⋅,t),νˉt​⟩=⟨φ(⋅,0),νˉ0​⟩+∫0t​⟨φx​+φs​,νˉs​⟩ds−∫0t​⟨hφ(⋅,s),νˉs​⟩ds+∫[0,t]​φ(0,s)dKˉ(s)(3.5);

Xˉ(t)=Xˉ(0)+Eˉ(t)−Dˉ(t)\bar X(t)=\bar X(0)+\bar E(t)-\bar D(t)Xˉ(t)=Xˉ(0)+Eˉ(t)−Dˉ(t) (3.6); and the nonidling condition 1−⟨1,νˉt⟩=[1−Xˉ(t)]+1-\langle\mathbf 1,\bar\nu_t\rangle=[1-\bar X(t)]^+1−⟨1,νˉt​⟩=[1−Xˉ(t)]+ (3.7). Here Dˉ(t)=∫0t⟨h,νˉs⟩ds\bar D(t)=\int_0^t\langle h,\bar\nu_s\rangle dsDˉ(t)=∫0t​⟨h,νˉs​⟩ds is the cumulative departure process and Kˉ(t)=⟨1,νˉt⟩−⟨1,νˉ0⟩+Dˉ(t)\bar K(t)=\langle\mathbf 1,\bar\nu_t\rangle-\langle\mathbf 1,\bar\nu_0\rangle+\bar D(t)Kˉ(t)=⟨1,νˉt​⟩−⟨1,νˉ0​⟩+Dˉ(t) the cumulative entry into service. Equation (3.5) is a weak form of a transport equation: mass moves to the right at unit speed, is killed at rate hhh, and enters at age 000 at rate dKˉd\bar KdKˉ.

Formalization targets

Goal: Theorem 3.5

For every (Eˉ,Xˉ(0),νˉ0)∈S0(\bar E,\bar X(0),\bar\nu_0)\in\mathcal S_0(Eˉ,Xˉ(0),νˉ0​)∈S0​:

  1. the fluid equations have at most one solution;
  2. under (3.4) and the path conditions, (Xˉ,νˉ)(\bar X,\bar\nu)(Xˉ,νˉ) is a solution if and only if it satisfies (3.6), (3.7) and, for every bounded continuous fff and t≥0t\ge0t≥0,
⟨f,νˉt⟩=∫[0,M)f(x+t)1−G(x+t)1−G(x) νˉ0(dx)+∫[0,t]f(t−s)(1−G(t−s)) dKˉ(s);(3.11)\langle f,\bar\nu_t\rangle=\int_{[0,M)}f(x+t)\frac{1-G(x+t)}{1-G(x)}\,\bar\nu_0(dx)+\int_{[0,t]}f(t-s)\big(1-G(t-s)\big)\,d\bar K(s);\quad(3.11)⟨f,νˉt​⟩=∫[0,M)​f(x+t)1−G(x)1−G(x+t)​νˉ0​(dx)+∫[0,t]​f(t−s)(1−G(t−s))dKˉ(s);(3.11)
  1. if Eˉ\bar EEˉ has a density λˉ\bar\lambdaλˉ, then Kˉ\bar KKˉ has a density κˉ\bar\kappaκˉ equal a.e. to λˉ\bar\lambdaλˉ where Xˉ<1\bar X<1Xˉ<1, to λˉ∧⟨h,νˉt⟩\bar\lambda\wedge\langle h,\bar\nu_t\rangleλˉ∧⟨h,νˉt​⟩ where Xˉ=1\bar X=1Xˉ=1, and to ⟨h,νˉt⟩\langle h,\bar\nu_t\rangle⟨h,νˉt​⟩ where Xˉ>1\bar X>1Xˉ>1 (3.12);
  2. if moreover νˉ0\bar\nu_0νˉ0​ is absolutely continuous, so is every νˉt\bar\nu_tνˉt​.

Milestones

  • Remark 4.3, (4.4): integration by parts for the entry term of (4.3).
  • (4.55): the integrated hazard in closed form, ψh(x,t)=(1−G(x))/(1−G(x−t))\psi_h(x,t)=(1-G(x))/(1-G(x-t))ψh​(x,t)=(1−G(x))/(1−G(x−t)) or 1−G(x)1-G(x)1−G(x).
  • Theorem 4.1: for a Radon-measure-valued path satisfying the hazard bound (4.1), the age equation (4.2), which is (3.5) with an arbitrary Radon measure υ0\upsilon_0υ0​ and an arbitrary ZZZ of bounded variation in place of νˉ0\bar\nu_0νˉ0​ and Kˉ\bar KKˉ, holds if and only if the representation (4.3) holds.
  • Proof of Corollary 4.4: Kˉ\bar KKˉ is nondecreasing.
  • Corollary 4.4, (4.5): Kˉ(t)=⟨1,νˉt⟩−⟨1,νˉ0⟩+∫G(x+t)−G(x)1−G(x)νˉ0(dx)+∫0tg(t−s)Kˉ(s)ds\bar K(t)=\langle\mathbf 1,\bar\nu_t\rangle-\langle\mathbf 1,\bar\nu_0\rangle+\int\frac{G(x+t)-G(x)}{1-G(x)}\bar\nu_0(dx)+\int_0^tg(t-s)\bar K(s)dsKˉ(t)=⟨1,νˉt​⟩−⟨1,νˉ0​⟩+∫1−G(x)G(x+t)−G(x)​νˉ0​(dx)+∫0t​g(t−s)Kˉ(s)ds.
  • Lemma 4.5: ∥⟨f,νˉs2⟩−⟨f,νˉs1⟩∥T≤∥f∥M∣Δυ0∣TV+(2∥f∥T+∥f′∥T)∥ΔZ∥T\|\langle f,\bar\nu^2_s\rangle-\langle f,\bar\nu^1_s\rangle\|_T\le\|f\|_M|\Delta\upsilon_0|_{TV}+(2\|f\|_T+\|f'\|_T)\|\Delta Z\|_T∥⟨f,νˉs2​⟩−⟨f,νˉs1​⟩∥T​≤∥f∥M​∣Δυ0​∣TV​+(2∥f∥T​+∥f′∥T​)∥ΔZ∥T​.
  • Theorem 4.6: with equal initial measures, ∥ΔKˉ∥T∨∥ΔDˉ∥T≤∣ΔXˉ(0)∣+∥ΔEˉ∥T\|\Delta\bar K\|_T\vee\|\Delta\bar D\|_T\le|\Delta\bar X(0)|+\|\Delta\bar E\|_T∥ΔKˉ∥T​∨∥ΔDˉ∥T​≤∣ΔXˉ(0)∣+∥ΔEˉ∥T​, together with (4.8) and (4.10).

Significance

Uniqueness of the fluid solution is what turns tightness of the scaled NNN-server processes into convergence: every subsequential limit solves the fluid equations, so all coincide (the paper's Theorem 3.7). The representation (3.11) reduces the measure-valued equation to the scalar process Kˉ\bar KKˉ, and the continuity estimate of Theorem 4.6 says the fluid solution is a Lipschitz function of the arrival process. Both are used in the paper's study of long-time behaviour, where νˉt\bar\nu_tνˉt​ converges to the measure with density 1−G1-G1−G, and (3.12) is the form of the entry rate used there.

The results are proved in the paper. None of them, and no part of the measure-valued fluid model, has a machine-checked proof. Formalizing them produces a checked weak-solution theory for a transport equation with an unbounded killing rate and a measure-valued boundary input, which is a reusable piece of infrastructure for other age- and residual-time-based queueing models.

Difficulty

The central step is Theorem 4.1. The naive approach treats (4.2) as a first-order PDE and integrates along characteristics, but the solution is only a càdlàg path of measures, hhh is merely locally integrable and blows up near MMM, and ZZZ may jump, so classical characteristics are not available; the test functions must not vanish on the boundary x=0x=0x=0, since that is where the entry term lives. The second difficulty is in Theorem 4.6: the entry process Kˉ\bar KKˉ is defined implicitly through the nonidling condition, and comparing two solutions requires a first-crossing argument that distinguishes whether the system is below, at or above capacity at that time.

Formalization scope

The service law is its density ggg (ServiceLaw), with g=0g=0g=0 below 000, ∫g=1\int g=1∫g=1 and mean one. Time is R\mathbb RR read on [0,∞)[0,\infty)[0,∞); every condition is stated for t≥0t\ge0t≥0. Measures of the fluid model are FiniteMeasure ℝ carried by [0,M)[0,M)[0,M), whose topology is weak convergence, so càdlàg paths are càdlàg in MF[0,M)\mathcal M_F[0,M)MF​[0,M) with the weak topology. The paths of Theorem 4.1 and Lemma 4.5 are ℝ → Measure ℝ with values Radon on [0,M)[0,M)[0,M) (possibly infinite) and càdlàg in the vague topology. M∈[0,∞]M\in[0,\infty]M∈[0,∞] is an extended number. The integral in (3.4) is a lower integral in [0,∞][0,\infty][0,∞], and Dˉ\bar DDˉ, Kˉ\bar KKˉ are its real value. dKˉd\bar KdKˉ is the Lebesgue–Stieltjes measure of Kˉ\bar KKˉ, with no atom at 000. A function ZZZ of bounded variation is a difference Z1−Z2Z_1-Z_2Z1​−Z2​ of nondecreasing càdlàg functions vanishing at 000.

Explicit choices: compact support of test functions is relative to [0,M)×R+[0,M)\times\mathbb R_+[0,M)×R+​, so φ(0,s)\varphi(0,s)φ(0,s) need not vanish (with supports taken in R2\mathbb R^2R2 the entry term of (3.5) would vanish identically); νˉ(0)=νˉ0\bar\nu(0)=\bar\nu_0νˉ(0)=νˉ0​ and Xˉ(0)\bar X(0)Xˉ(0) equal to the datum are clauses of the fluid equations, but not of the age equation, where υ0\upsilon_0υ0​ is arbitrary; functions in Cb(R+)\mathcal C_b(\mathbb R_+)Cb​(R+​), Cc(R+)\mathcal C_c(\mathbb R_+)Cc​(R+​) and Cb1(R+)\mathcal C^1_b(\mathbb R_+)Cb1​(R+​) are represented by functions on R\mathbb RR of the same class, of which only values on [0,∞)[0,\infty)[0,∞) are read; norms in Lemma 4.5 are computed in [0,∞][0,\infty][0,∞], since ∣Δυ0∣TV|\Delta\upsilon_0|_{TV}∣Δυ0​∣TV​ may be infinite. Two printed statements are corrected: in Theorem 3.5 the paper's right-hand side of the equivalence lists (3.6) and (3.11); the nonidling condition (3.7), part of the fluid equations on the left, is kept on the right, as the proof requires. In (4.10), ΔXˉ(0)\Delta\bar X(0)ΔXˉ(0) is replaced by ∣ΔXˉ(0)∣|\Delta\bar X(0)|∣ΔXˉ(0)∣, which is what Lemma 4.5 and (4.9) give.

A fluid solution is defined by the weak transport equation (3.5), never by the representation (3.11) or by a formula for νˉ\bar\nuνˉ in terms of Kˉ\bar KKˉ; with such a definition the equivalence of the goal would be an unfolding of definitions.

A complete development needs Lebesgue–Stieltjes integration by parts for càdlàg functions of bounded variation, the Riesz description of the vague topology, and uniqueness for weak solutions of transport equations; these are reusable beyond this mission. Proofs of any milestone, and of the parts of Theorem 3.5 separately, are welcome. The paper's Section 4.3 machinery (the abstract and simplified age equations, Lemmas 4.12–4.13, Propositions 4.15–4.16) is not posed here and may be formalized as supporting lemmas.

Selected references

  • H. Kaspi and K. Ramanan, Law of large numbers limits for many-server queues, Ann. Appl. Probab. 21(1) (2011), 33–114. https://doi.org/10.1214/09-AAP662
  • J. Reed, The G/GI/N queue in the Halfin–Whitt regime, Ann. Appl. Probab. 19(6) (2009), 2211–2269. https://doi.org/10.1214/09-AAP609
  • W. Whitt, Fluid models for multiserver queues with abandonments, Oper. Res. 54(1) (2006), 37–54. https://doi.org/10.1287/opre.1050.0227
  • S. Asmussen, Applied Probability and Queues, 2nd ed., Springer, 2003. https://doi.org/10.1007/b97236
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Numerical AnalysisProbability·Captain: mikedeng1

A Regression-Based Monte Carlo Method to Solve Backward Stochastic Differential Equations I: Projection Errors of the Picard–Regression Scheme Accumulate AdditivelyResearch Paper

Motivation

A backward stochastic differential equation (BSDE) prescribes the value of a process at a terminal time and asks for an adapted process that reaches it while following a given drift. In mathematical finance the price of a contingent claim, and its hedging strategy, solve such an equation; when the market has frictions (different borrowing and lending rates, for example) the drift, called the driver, is nonlinear and no closed form exists. Numerical methods for BSDEs are therefore methods for pricing and hedging under nonlinear models, and also for semilinear parabolic PDEs, which BSDEs represent probabilistically.

Gobet, Lemor and Warin (Ann. Appl. Probab. 15 (2005), arXiv:math/0508491) proposed and analysed a simulation scheme in which every conditional expectation of a backward time-stepping recursion is replaced by a least-squares regression on finitely many functions, as in the Longstaff–Schwartz method for American options. Their analysis splits the total error into three parts: time discretization (Theorem 1, from Zhang's results), replacing conditional expectations by L2\mathbf L_2L2​ projections on function bases (Theorem 2), and replacing those projections by empirical regressions on MMM simulated paths (Theorem 3). This mission formalizes the second part.

Timeline. Zhang (Ann. Appl. Probab. 14 (2004)) and Bouchard and Touzi (Stoch. Proc. Appl. 111 (2004)) established the h\sqrt hh​ rate of the time discretization. Bouchard and Touzi's regression error (their reference [6] in the paper, Theorem 4.1 there) was expressed through the residuals of the scheme's own iterates. Gobet, Lemor and Warin (2005) gave the bound in terms of the residuals of the discrete BSDE, together with estimates on ZZZ.

Setting

Fix a horizon T>0T>0T>0, dimensions d,q≥1d,q\ge1d,q≥1, a drift b(t,x)∈Rdb(t,x)\in\mathbb R^db(t,x)∈Rd and a diffusion matrix σ(t,x)∈Rd×q\sigma(t,x)\in\mathbb R^{d\times q}σ(t,x)∈Rd×q, both Lipschitz in (t,x)(t,x)(t,x) ((H1)), and a driver f(t,x,y,z)∈Rf(t,x,y,z)\in\mathbb Rf(t,x,y,z)∈R with

∣f(t2,x2,y2,z2)−f(t1,x1,y1,z1)∣≤Cf(∣t2−t1∣1/2+∣x2−x1∣+∣y2−y1∣+∣z2−z1∣)(H2).|f(t_2,x_2,y_2,z_2)-f(t_1,x_1,y_1,z_1)|\le C_f\big(|t_2-t_1|^{1/2}+|x_2-x_1|+|y_2-y_1|+|z_2-z_1|\big)\qquad\textbf{(H2)}.∣f(t2​,x2​,y2​,z2​)−f(t1​,x1​,y1​,z1​)∣≤Cf​(∣t2​−t1​∣1/2+∣x2​−x1​∣+∣y2​−y1​∣+∣z2​−z1​∣)(H2).

For N≥1N\ge1N≥1 put h=T/Nh=T/Nh=T/N and tk=kht_k=khtk​=kh. On a probability space with a filtration (Fk)(\mathcal F_k)(Fk​), the increments ΔWk∈Rq\Delta W_k\in\mathbb R^qΔWk​∈Rq are Fk+1\mathcal F_{k+1}Fk+1​-measurable, independent of Fk\mathcal F_kFk​ and Gaussian N(0,hIq)\mathcal N(0,hI_q)N(0,hIq​); ΔWl,k\Delta W_{l,k}ΔWl,k​ is the lll-th component. The Euler scheme is St0N=S0S^N_{t_0}=S_0St0​N​=S0​, Stk+1N=StkN+b(tk,StkN)h+σ(tk,StkN)ΔWkS^N_{t_{k+1}}=S^N_{t_k}+b(t_k,S^N_{t_k})h+\sigma(t_k,S^N_{t_k})\Delta W_kStk+1​N​=Stk​N​+b(tk​,Stk​N​)h+σ(tk​,Stk​N​)ΔWk​. An Fk\mathcal F_kFk​-adapted process PtkN∈Rd′P^N_{t_k}\in\mathbb R^{d'}Ptk​N​∈Rd′ extends StkNS^N_{t_k}Stk​N​ by extra state variables, and the terminal value is ΦN(PtNN)\Phi^N(P^N_{t_N})ΦN(PtN​N​), square integrable.

Write Ek=E(⋅∣Fk)\mathbb E_k=\mathbb E(\cdot\mid\mathcal F_k)Ek​=E(⋅∣Fk​). The discrete BSDE is YtNN=ΦN(PtNN)Y^N_{t_N}=\Phi^N(P^N_{t_N})YtN​N​=ΦN(PtN​N​) and, for k<Nk<Nk<N,

Zl,tkN=1hEk(Ytk+1NΔWl,k),YtkN=Ek(Ytk+1N)+hf(tk,StkN,YtkN,ZtkN).Z^N_{l,t_k}=\tfrac1h\mathbb E_k(Y^N_{t_{k+1}}\Delta W_{l,k}),\qquad Y^N_{t_k}=\mathbb E_k(Y^N_{t_{k+1}})+hf(t_k,S^N_{t_k},Y^N_{t_k},Z^N_{t_k}).Zl,tk​N​=h1​Ek​(Ytk+1​N​ΔWl,k​),Ytk​N​=Ek​(Ytk+1​N​)+hf(tk​,Stk​N​,Ytk​N​,Ztk​N​).

A function basis pl,k(PtkN)∈Rnl,kp_{l,k}(P^N_{t_k})\in\mathbb R^{n_{l,k}}pl,k​(Ptk​N​)∈Rnl,k​ (0≤l≤q0\le l\le q0≤l≤q) is square integrable with invertible Gram matrix E(pl,kpl,k∗)\mathbb E(p_{l,k}p_{l,k}^*)E(pl,k​pl,k∗​). Pp(U)\mathcal P_{p}(U)Pp​(U) is the L2(Ω,P)\mathbf L_2(\Omega,\mathbb P)L2​(Ω,P) orthogonal projection of UUU onto the span of the basis, and Rp(U)=U−Pp(U)\mathcal R_p(U)=U-\mathcal P_p(U)Rp​(U)=U−Pp​(U).

The projection–Picard scheme with III iterations (Definition 1) produces YtkN,i,I=α0,ki,I⋅p0,kY^{N,i,I}_{t_k}=\alpha^{i,I}_{0,k}\cdot p_{0,k}Ytk​N,i,I​=α0,ki,I​⋅p0,k​ and Zl,tkN,i,I=αl,ki,I⋅pl,kZ^{N,i,I}_{l,t_k}=\alpha^{i,I}_{l,k}\cdot p_{l,k}Zl,tk​N,i,I​=αl,ki,I​⋅pl,k​, starting from α0,I=0\alpha^{0,I}=0α0,I=0, where αki,I\alpha^{i,I}_kαki,I​ minimizes

E(Ytk+1N,I,I−α0⋅p0,k+hf(tk,StkN,YtkN,i−1,I,ZtkN,i−1,I)−∑l=1qαl⋅pl,kΔWl,k)2.(9)\mathbb E\Big(Y^{N,I,I}_{t_{k+1}}-\alpha_0\cdot p_{0,k}+hf(t_k,S^N_{t_k},Y^{N,i-1,I}_{t_k},Z^{N,i-1,I}_{t_k})-\sum_{l=1}^q\alpha_l\cdot p_{l,k}\Delta W_{l,k}\Big)^2.\qquad(9)E(Ytk+1​N,I,I​−α0​⋅p0,k​+hf(tk​,Stk​N​,Ytk​N,i−1,I​,Ztk​N,i−1,I​)−l=1∑q​αl​⋅pl,k​ΔWl,k​)2.(9)

Finally AN(S0)=1+∣S0∣2+E∣ΦN(PtNN)∣2\mathcal A^N(S_0)=1+|S_0|^2+\mathbb E|\Phi^N(P^N_{t_N})|^2AN(S0​)=1+∣S0​∣2+E∣ΦN(PtN​N​)∣2.

Formalization targets

Goal: Theorem 2 (p. 11)

For hhh small enough,

max⁡0≤k≤NE∣YtkN,I,I−YtkN∣2+h∑k=0N−1E∣ZtkN,I,I−ZtkN∣2≤Ch2I−2AN(S0)+C∑k=0N−1E∣Rp0,k(YtkN)∣2+Ch∑k=0N−1∑l=1qE∣Rpl,k(Zl,tkN)∣2.\max_{0\le k\le N}\mathbb E|Y^{N,I,I}_{t_k}-Y^N_{t_k}|^2+h\sum_{k=0}^{N-1}\mathbb E|Z^{N,I,I}_{t_k}-Z^N_{t_k}|^2\le Ch^{2I-2}\mathcal A^N(S_0)+C\sum_{k=0}^{N-1}\mathbb E|\mathcal R_{p_{0,k}}(Y^N_{t_k})|^2+Ch\sum_{k=0}^{N-1}\sum_{l=1}^q\mathbb E|\mathcal R_{p_{l,k}}(Z^N_{l,t_k})|^2 .0≤k≤Nmax​E∣Ytk​N,I,I​−Ytk​N​∣2+hk=0∑N−1​E∣Ztk​N,I,I​−Ztk​N​∣2≤Ch2I−2AN(S0​)+Ck=0∑N−1​E∣Rp0,k​​(Ytk​N​)∣2+Chk=0∑N−1​l=1∑q​E∣Rpl,k​​(Zl,tk​N​)∣2.

Milestones

  1. (10)–(11): the minimizer of (9) is given by projections, Zl,tkN,i,I=1hPpl,k(Ytk+1N,I,IΔWl,k)Z^{N,i,I}_{l,t_k}=\frac1h\mathcal P_{p_{l,k}}(Y^{N,I,I}_{t_{k+1}}\Delta W_{l,k})Zl,tk​N,i,I​=h1​Ppl,k​​(Ytk+1​N,I,I​ΔWl,k​) and YtkN,i,I=Pp0,k(Ytk+1N,I,I+hf(…,YtkN,i−1,I,ZtkN,i−1,I))Y^{N,i,I}_{t_k}=\mathcal P_{p_{0,k}}(Y^{N,I,I}_{t_{k+1}}+hf(\dots,Y^{N,i-1,I}_{t_k},Z^{N,i-1,I}_{t_k}))Ytk​N,i,I​=Pp0,k​​(Ytk+1​N,I,I​+hf(…,Ytk​N,i−1,I​,Ztk​N,i−1,I​)).
  2. (12): h E∣Zl,tkN,i,I∣2≤E∣Ytk+1N,I,I∣2−E∣Ek(Ytk+1N,I,I)∣2h\,\mathbb E|Z^{N,i,I}_{l,t_k}|^2\le\mathbb E|Y^{N,I,I}_{t_{k+1}}|^2-\mathbb E|\mathbb E_k(Y^{N,I,I}_{t_{k+1}})|^2hE∣Zl,tk​N,i,I​∣2≤E∣Ytk+1​N,I,I​∣2−E∣Ek​(Ytk+1​N,I,I​)∣2.
  3. (13): the map Y↦Pp0,k(Ytk+1N,I,I+hf(tk,StkN,Y,ZtkN,I,I))Y\mapsto\mathcal P_{p_{0,k}}(Y^{N,I,I}_{t_{k+1}}+hf(t_k,S^N_{t_k},Y,Z^{N,I,I}_{t_k}))Y↦Pp0,k​​(Ytk+1​N,I,I​+hf(tk​,Stk​N​,Y,Ztk​N,I,I​)) is a (Cfh)(C_fh)(Cf​h)-contraction on L2(Fk)\mathbf L_2(\mathcal F_k)L2​(Fk​) with a unique fixed point.
  4. The discrete Gronwall lemma with ccc-terms (p. 11, item 3).
  5. (19): E∣YtkN,i,I∣2+h E∣Zl,tkN,i,I∣2≤CAN(S0)\mathbb E|Y^{N,i,I}_{t_k}|^2+h\,\mathbb E|Z^{N,i,I}_{l,t_k}|^2\le C\mathcal A^N(S_0)E∣Ytk​N,i,I​∣2+hE∣Zl,tk​N,i,I​∣2≤CAN(S0​), uniformly in III, iii, kkk.

Significance

Theorem 2 shows that the projection errors of a backward regression scheme only add up over the NNN time steps, with a constant that does not grow with NNN, and that they are measured by the residuals of the discrete BSDE itself. That makes the influence of the basis directly computable (the paper's §6 does so for Voronoi-cell indicators), and shows that I=2I=2I=2 Picard iterations already give an error of the order of the time discretization. Combined with Theorem 3 it gives the complete error budget of the algorithm.

The result is proved in the paper; to our knowledge none of it is machine-checked. A complete development provides a formal L2\mathbf L_2L2​-regression calculus for discrete BSDEs (projections on random bases, conditional expectations against Gaussian increments, contraction of Picard maps in L2(Fk)\mathbf L_2(\mathcal F_k)L2​(Fk​)) and a backward discrete Gronwall lemma, all reusable for other regression schemes. One printed step, (14), fails at i=1i=1i=1 (see below), so a formal proof also certifies that the theorem survives the repair.

Difficulty

The obvious argument compares the scheme with the discrete BSDE one step at a time and applies Gronwall. It fails for ZZZ: ZtkN,i,IZ^{N,i,I}_{t_k}Ztk​N,i,I​ carries a factor 1/h1/h1/h, and a naive bound E∣Z∣2≤h−1E∣Y∣2\mathbb E|Z|^2\le h^{-1}\mathbb E|Y|^2E∣Z∣2≤h−1E∣Y∣2 summed over N=T/hN=T/hN=T/h steps explodes. A usable bound has to account for the conditional variance of Ytk+1N,I,IY^{N,I,I}_{t_{k+1}}Ytk+1​N,I,I​ given Fk\mathcal F_kFk​, not only its second moment. The second difficulty is that the projection does not commute with the driver: projection errors enter at every step through the nonlinear fff, and must be bounded by residuals of YNY^NYN and ZNZ^NZN, not of the scheme's iterates. A third is the Picard step: at i=1i=1i=1 the iterate is computed with ZN,0,I=0Z^{N,0,I}=0ZN,0,I=0, so it is not an iterate of the contraction of milestone 3, and the printed inequality (14) E∣YtkN,∞,I−YtkN,i,I∣2≤(Cfh)2iE∣YtkN,∞,I∣2\mathbb E|Y^{N,\infty,I}_{t_k}-Y^{N,i,I}_{t_k}|^2\le(C_fh)^{2i}\mathbb E|Y^{N,\infty,I}_{t_k}|^2E∣Ytk​N,∞,I​−Ytk​N,i,I​∣2≤(Cf​h)2iE∣Ytk​N,∞,I​∣2 fails there; an extra term in E∣ZtkN,I,I∣2\mathbb E|Z^{N,I,I}_{t_k}|^2E∣Ztk​N,I,I​∣2 is needed.

Formalization scope

The Lean development lives in the namespace RegMCBSDE.Projection. Points are in EuclideanSpace ℝ (Fin d), the matrix norm in (H1) is the Frobenius norm, and all expectations of squares are lower Lebesgue integrals in [0,∞][0,\infty][0,∞], so no junk value of a Bochner integral can make an inequality vacuous. Component mmm (from 000) of ΔWk\Delta W_kΔWk​ is the paper's ΔWm+1,k\Delta W_{m+1,k}ΔWm+1,k​, and the bases are indexed by Fin (q+1) with l=0l=0l=0 for YYY.

Committed readings:

  • (H3) is dropped. It constrains the continuous terminal functional, which no statement involves.
  • The filtration is abstract. Any filtration with Fk+1\mathcal F_{k+1}Fk+1​-measurable increments independent of Fk\mathcal F_kFk​ and of law N(0,hIq)\mathcal N(0,hI_q)N(0,hIq​); the Brownian filtration is one. The Markov representation of PNP^NPN is not used and is dropped.
  • Schemes are relations. (YN,ZN)(Y^N,Z^N)(YN,ZN) is any solution of (5)–(6), and α\alphaα is any family satisfying the arg-min rule (9) for every i≥1i\ge1i≥1 (the paper runs i≤Ii\le Ii≤I; (19) refers to all i≥0i\ge0i≥0). (10)–(11) are a milestone, not the definition.
  • The projection is Mathlib's orthogonal projection in L2(Ω,P)\mathbf L_2(\Omega,\mathbb P)L2​(Ω,P) onto the span of the basis coordinates. It is not defined by the normal equations.
  • Constants. In Theorem 2 and (19), CCC and the threshold h0h_0h0​ of "hhh small enough" are chosen after (T,d,q,b,σ,f,Cf,L)(T,d,q,b,\sigma,f,C_f,L)(T,d,q,b,σ,f,Cf​,L) and before NNN, III, S0S_0S0​, d′d'd′, the probability space, PNP^NPN, ΦN\Phi^NΦN and the bases. A constant chosen after the scheme data would make the theorem trivially true and is ruled out by this quantifier order.
  • Pinned readings. max⁡k\max_kmaxk​ is "for every k≤Nk\le Nk≤N". In (13) the argument ZN,i−1,IZ^{N,i-1,I}ZN,i−1,I is read as ZN,I,IZ^{N,I,I}ZN,I,I, as the displayed (13) shows, and "hhh small enough" is Cfh<1C_fh<1Cf​h<1. (12) is multiplied by hhh to avoid subtraction. (19) is stated for k≤N−1k\le N-1k≤N−1 and every 1≤l≤q1\le l\le q1≤l≤q. (10) is stated where Ytk+1N,I,IΔWl,kY^{N,I,I}_{t_{k+1}}\Delta W_{l,k}Ytk+1​N,I,I​ΔWl,k​ is square integrable, since P\mathcal PP acts on L2\mathbf L_2L2​.
  • Not stated. (14), which is false at i=1i=1i=1, and the steps whose printed derivation passes through it ((15)–(18), (20)–(26)); Theorem 1 and Propositions 1 and 3.

Contributions welcome: proofs of the milestones, and the Mathlib-level lemmas they need (conditional expectation of a product with an independent centered Gaussian, L2\mathbf L_2L2​ moments of the Euler scheme, the projection identity Pp(U)=Pp(EkU)\mathcal P_p(U)=\mathcal P_p(\mathbb E_kU)Pp​(U)=Pp​(Ek​U) for Fk\mathcal F_kFk​-measurable bases).

Selected references

  • E. Gobet, J.-P. Lemor, X. Warin, A regression-based Monte Carlo method to solve backward stochastic differential equations, Ann. Appl. Probab. 15(3), 2172–2202, 2005. arXiv:math/0508491, doi:10.1214/105051605000000412
  • J. Zhang, A numerical scheme for BSDEs, Ann. Appl. Probab. 14(1), 459–488, 2004. doi:10.1214/aoap/1075828058
  • B. Bouchard, N. Touzi, Discrete-time approximation and Monte-Carlo simulation of backward stochastic differential equations, Stoch. Proc. Appl. 111(2), 175–206, 2004. doi:10.1016/j.spa.2004.01.001
  • F. A. Longstaff, E. S. Schwartz, Valuing American options by simulation: a simple least-squares approach, Rev. Financ. Stud. 14(1), 113–147, 2001. doi:10.1093/rfs/14.1.113
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A Regression-Based Monte Carlo Method to Solve Backward Stochastic Differential Equations II: Simulation Error of the Empirical Regression Scheme in the Number of PathsResearch Paper

Motivation

Backward stochastic differential equations (BSDEs) describe the price and the hedge of a contingent claim in models with nonlinear pricing rules (differential interest rates, funding costs, reflected or constrained claims), and give probabilistic representations of semilinear parabolic PDEs (El Karoui, Peng and Quenez, 1997). Their numerical solution in moderate dimension is done by simulation: a backward recursion over a time grid in which each conditional expectation is replaced by a least-squares regression on simulated paths, the same device as the regression method for Bermudan options of Longstaff and Schwartz (2001).

Gobet, Lemor and Warin (2005) split the error of such a scheme into three parts: time discretization (Theorem 1), projection on finite function bases (Theorem 2), and the replacement of L2\mathbf L_2L2​ projections by empirical regressions on MMM simulated paths (Theorem 3). This mission formalizes the third part, which the authors describe as the major contribution of the paper. Its point is that the error from the simulations is controlled nonasymptotically, step by step, without blowing up as the time step hhh shrinks, even though every regression of the backward recursion reuses the same simulated paths.

Setting

A model consists of a horizon T>0T>0T>0, a drift bbb, a diffusion σ\sigmaσ satisfying the Lipschitz condition (H1), and a driver f(t,x,y,z)f(t,x,y,z)f(t,x,y,z) satisfying (H2): ∣f(t2,x2,y2,z2)−f(t1,x1,y1,z1)∣≤Cf(∣t2−t1∣1/2+∣x2−x1∣+∣y2−y1∣+∣z2−z1∣)|f(t_2,x_2,y_2,z_2)-f(t_1,x_1,y_1,z_1)|\le C_f(|t_2-t_1|^{1/2}+|x_2-x_1|+|y_2-y_1|+|z_2-z_1|)∣f(t2​,x2​,y2​,z2​)−f(t1​,x1​,y1​,z1​)∣≤Cf​(∣t2​−t1​∣1/2+∣x2​−x1​∣+∣y2​−y1​∣+∣z2​−z1​∣). For N≥1N\ge1N≥1, h=T/Nh=T/Nh=T/N, tk=kht_k=khtk​=kh, the Euler scheme is Stk+1N=StkN+b(tk,StkN)h+σ(tk,StkN)ΔWkS^N_{t_{k+1}}=S^N_{t_k}+b(t_k,S^N_{t_k})h+\sigma(t_k,S^N_{t_k})\Delta W_kStk+1​N​=Stk​N​+b(tk​,Stk​N​)h+σ(tk​,Stk​N​)ΔWk​, where the increments ΔWk∼N(0,hIq)\Delta W_k\sim\mathcal N(0,hI_q)ΔWk​∼N(0,hIq​) are independent of the past. A chain PtkN∈Rd′P^N_{t_k}\in\mathbb R^{d'}Ptk​N​∈Rd′ extends StkNS^N_{t_k}Stk​N​, and ΦN(PtNN)\Phi^N(P^N_{t_N})ΦN(PtN​N​) is the terminal value.

At each time tkt_ktk​, function bases p0,kp_{0,k}p0,k​ (for YYY) and pl,kp_{l,k}pl,k​, 1≤l≤q1\le l\le q1≤l≤q (for the components of ZZZ) are fixed, orthonormal in the sense E[pl,k(PtkN)pl,k(PtkN)∗]=Id\mathbb E[p_{l,k}(P^N_{t_k})p_{l,k}(P^N_{t_k})^*]=\mathrm{Id}E[pl,k​(Ptk​N​)pl,k​(Ptk​N​)∗]=Id. The projection–Picard scheme (Definition 1) computes coefficients αki,I\alpha^{i,I}_kαki,I​ by III Picard iterations of an L2\mathbf L_2L2​ least-squares problem, and sets YtkN,I,I=α0,kI,I⋅p0,kY^{N,I,I}_{t_k}=\alpha^{I,I}_{0,k}\cdot p_{0,k}Ytk​N,I,I​=α0,kI,I​⋅p0,k​, Zl,tkN,I,I=αl,kI,I⋅pl,kZ^{N,I,I}_{l,t_k}=\alpha^{I,I}_{l,k}\cdot p_{l,k}Zl,tk​N,I,I​=αl,kI,I​⋅pl,k​.

The empirical scheme (4) replaces the expectation by an average over MMM independent simulations (PN,m,ΔWm)(P^{N,m},\Delta W^m)(PN,m,ΔWm) of the path: αki,I,M\alpha^{i,I,M}_kαki,I,M​ minimizes

1M∑m=1M(Ytk+1N,I,I,M,m−α0⋅p0,km+hfkm(αki−1,I,M)−∑l=1qαl⋅pl,kmΔWl,km)2.\frac1M\sum_{m=1}^M\Big(Y^{N,I,I,M,m}_{t_{k+1}}-\alpha_0\cdot p^m_{0,k}+hf^m_k(\alpha^{i-1,I,M}_k)-\sum_{l=1}^q\alpha_l\cdot p^m_{l,k}\Delta W^m_{l,k}\Big)^2 .M1​m=1∑M​(Ytk+1​N,I,I,M,m​−α0​⋅p0,km​+hfkm​(αki−1,I,M​)−l=1∑q​αl​⋅pl,km​ΔWl,km​)2.

The outputs are truncated: with ρl,kN(x)=max⁡(1,C0∣pl,k(x)∣)\rho^N_{l,k}(x)=\max(1,C_0|p_{l,k}(x)|)ρl,kN​(x)=max(1,C0​∣pl,k​(x)∣) and a smooth profile ξ\xiξ equal to the identity on [−3/2,3/2][-3/2,3/2][−3/2,3/2], YtkN,I,I,M=ρ^0,kN(α0,kI,I,M⋅p0,k)Y^{N,I,I,M}_{t_k}=\hat\rho^N_{0,k}(\alpha^{I,I,M}_{0,k}\cdot p_{0,k})Ytk​N,I,I,M​=ρ^​0,kN​(α0,kI,I,M​⋅p0,k​) with ρ^l,kN(x)=ρl,kN(PtkN)ξ(x/ρl,kN(PtkN))\hat\rho^N_{l,k}(x)=\rho^N_{l,k}(P^N_{t_k})\xi(x/\rho^N_{l,k}(P^N_{t_k}))ρ^​l,kN​(x)=ρl,kN​(Ptk​N​)ξ(x/ρl,kN​(Ptk​N​)). The regression vector is [vk]∗=(p0,k∗,p1,k∗ΔW1,k/h,…,pq,k∗ΔWq,k/h)[v_k]^*=(p_{0,k}^*,p_{1,k}^*\Delta W_{1,k}/\sqrt h,\dots,p_{q,k}^*\Delta W_{q,k}/\sqrt h)[vk​]∗=(p0,k∗​,p1,k∗​ΔW1,k​/h​,…,pq,k∗​ΔWq,k​/h​), and the good event AkM\mathbf A^M_kAkM​ (27) asks that the empirical matrices VjM=1M∑mvjm[vjm]∗V^M_j=\frac1M\sum_mv^m_j[v^m_j]^*VjM​=M1​∑m​vjm​[vjm​]∗ and Pl,jM=1M∑mpl,jm[pl,jm]∗P^M_{l,j}=\frac1M\sum_m p^m_{l,j}[p^m_{l,j}]^*Pl,jM​=M1​∑m​pl,jm​[pl,jm​]∗ be close to the identity for all j≥kj\ge kj≥k.

Formalization targets

Goal: Theorem 3

For I≥3I\ge3I≥3, orthonormal bases with E∣pl,k∣4<∞\mathbb E|p_{l,k}|^4<\inftyE∣pl,k​∣4<∞, C0C_0C0​ such that the bounds of Proposition 2 hold, and hhh small enough, for 0≤k≤N−10\le k\le N-10≤k≤N−1,

E∣YtkN,I,I−YtkN,I,I,M∣2+h∑j=kN−1E∣ZtjN,I,I−ZtjN,I,I,M∣2≤9∑j=kN−1E(∣ρjN∣21[AkM]c)+ChI−1∑j=kN−1[1+∣S0∣2+E∣ρjN∣2]+ChM∑j=kN−1ϵj,\mathbb E|Y^{N,I,I}_{t_k}-Y^{N,I,I,M}_{t_k}|^2+h\sum_{j=k}^{N-1}\mathbb E|Z^{N,I,I}_{t_j}-Z^{N,I,I,M}_{t_j}|^2\le 9\sum_{j=k}^{N-1}\mathbb E(|\rho^N_j|^2\mathbf 1_{[\mathbf A^M_k]^c})+Ch^{I-1}\sum_{j=k}^{N-1}[1+|S_0|^2+\mathbb E|\rho^N_j|^2]+\frac{C}{hM}\sum_{j=k}^{N-1}\epsilon_j,E∣Ytk​N,I,I​−Ytk​N,I,I,M​∣2+hj=k∑N−1​E∣Ztj​N,I,I​−Ztj​N,I,I,M​∣2≤9j=k∑N−1​E(∣ρjN​∣21[AkM​]c​)+ChI−1j=k∑N−1​[1+∣S0​∣2+E∣ρjN​∣2]+hMC​j=k∑N−1​ϵj​,

where ϵj\epsilon_jϵj​ collects second moments of vjvj∗−Idv_jv_j^*-\mathrm{Id}vj​vj∗​−Id, ∣vj∣2∣p0,j+1∣2|v_j|^2|p_{0,j+1}|^2∣vj​∣2∣p0,j+1​∣2 and ∣vj∣2(1+∣StjN∣2+… )|v_j|^2(1+|S^N_{t_j}|^2+\dots)∣vj​∣2(1+∣Stj​N​∣2+…), written out in full in the goal statement. The constant CCC and the threshold on hhh depend only on the model and on ξ\xiξ.

Milestones

  1. Proposition 2: the a priori bounds ∣YtkN,i,I∣≤ρ0,kN|Y^{N,i,I}_{t_k}|\le\rho^N_{0,k}∣Ytk​N,i,I​∣≤ρ0,kN​, h∣Zl,tkN,i,I∣≤ρl,kN\sqrt h|Z^{N,i,I}_{l,t_k}|\le\rho^N_{l,k}h​∣Zl,tk​N,i,I​∣≤ρl,kN​ that fix the truncation levels.
  2. (28)–(29): the empirical least-squares solution and its contraction inequality λmin⁡(VM)∣θx∣2≤∣θx⋅v∣M2≤∣x∣M2\lambda_{\min}(V^M)|\theta_x|^2\le|\theta_x\cdot v|^2_M\le|x|^2_Mλmin​(VM)∣θx​∣2≤∣θx​⋅v∣M2​≤∣x∣M2​.
  3. Lemma 1: on AkM\mathbf A^M_kAkM​ the empirical Picard iterations contract at rate ChChCh to a unique fixed point, with error [Ch]I[Ch]^I[Ch]I after III steps.
  4. (32): the pathwise bound ∣θki,I,M∣2≤C(Ak+1N,M+hBkN,M)|\theta^{i,I,M}_k|^2\le C(\mathcal A^{N,M}_{k+1}+h\mathcal B^{N,M}_k)∣θki,I,M​∣2≤C(Ak+1N,M​+hBkN,M​) on AkM\mathbf A^M_kAkM​.
  5. (34): the expectation formula θk∞,I=E(vk[Ytk+1N,I,I+hfk(αk∞,I)])\theta^{\infty,I}_k=\mathbb E(v_k[Y^{N,I,I}_{t_{k+1}}+hf_k(\alpha^{\infty,I}_k)])θk∞,I​=E(vk​[Ytk+1​N,I,I​+hfk​(αk∞,I​)]).

Significance

Theorem 3 is nonasymptotic: together with Theorems 1 and 2 it lets one compare the three error sources and choose hhh, the bases and MMM jointly for a target accuracy. The 1/(hM)1/(hM)1/(hM) rate shows how many paths a finer time grid requires, and the hI−1h^{I-1}hI−1 term shows that I=3I=3I=3 Picard iterations suffice. The term involving [AkM]c[\mathbf A^M_k]^c[AkM​]c isolates the event on which the empirical regression matrices are badly conditioned, which the truncation keeps under control.

The result is proved in the paper; nothing in this mission is open mathematically. No machine-checked proof of any part of it is known. A formal proof would check a long chain of estimates whose constants the paper tracks only as a generic CCC, and would settle the two misprints in the printed statement (see below). The definitions layer (Euler scheme, regression schemes, empirical regression matrices) is reusable for other regression Monte Carlo schemes for BSDEs and for optimal stopping.

Difficulty

The obvious approach is to treat each regression as an independent statistical estimation problem and apply a variance bound per time step. This fails because all regressions of the backward recursion use the same MMM paths: the response at time tk+1t_{k+1}tk+1​ is itself a function of the simulations, so the regression at tkt_ktk​ is not a regression of a fixed variable on independent samples. Moreover, the empirical matrix VkMV^M_kVkM​ may be singular, and on that event the empirical coefficients are unbounded unless truncated. A naive per-step bound also produces a factor 1/h1/h1/h at each of the N=T/hN=T/hN=T/h steps, which explodes; the proof must keep the accumulated constants of order one.

Formalization scope

  • All objects are defined in the namespace RegMCBSDE.Simulation. Continuous time is not used: the increments ΔWk\Delta W_kΔWk​ are any family that is Fk+1\mathcal F_{k+1}Fk+1​-measurable, independent of Fk\mathcal F_kFk​ and N(0,hIq)\mathcal N(0,hI_q)N(0,hIq​)-distributed for some filtration. That covers the Brownian case. (H3), a condition on the terminal functional of the continuous path, is dropped. So is the Markov representation of PNP^NPN, which no statement uses.
  • Expectations of squared quantities are taken in [0,∞][0,\infty][0,∞], on both sides of every inequality.
  • Euclidean norms are written as sums of squares. ∥A∥≤c\|A\|\le c∥A∥≤c for symmetric AAA is written as ∣x∗Ax∣≤c∣x∣2|x^*Ax|\le c|x|^2∣x∗Ax∣≤c∣x∣2 for all xxx.
  • The schemes are defined as predicates (any minimizer of each least-squares problem), never through a matrix inverse. The empirical coefficients are required to be measurable functions of the simulations, and any such minimizer is allowed, as the paper says the choice is arbitrary.
  • The reference path at which the fitted coefficients are evaluated is assumed independent of the MMM simulations.
  • Picard iterations are imposed for every i≥1i\ge1i≥1.
  • "For hhh small enough" is formalized as T/N<h0T/N<h_0T/N<h0​. Every constant CCC and every h0h_0h0​ is chosen before NNN, III, MMM, kkk, C0C_0C0​, the bases, S0S_0S0​ and the probability space. A formalization in which CCC is chosen after the scheme data would make every inequality with a positive right-hand side trivially true, and is ruled out.
  • "C0C_0C0​ large enough" in Theorem 3 is the hypothesis that the bounds of Proposition 2 hold for C0C_0C0​.
  • Proposition 2 is stated for hhh small enough. The printed statement omits this condition, which its proof needs through the uniform bound (19).
  • In (32) and Lemma 1, ρ0,NN\rho^N_{0,N}ρ0,NN​, which the paper leaves undefined, is read through the terminal response ΦN(PtNN,m)\Phi^N(P^{N,m}_{t_N})ΦN(PtN​N,m​).
  • Corrections to Theorem 3 (both from the paper's proof, p. 21):
    1. The printed j=N−1j=N-1j=N−1 summand contains the undefined p0,Np_{0,N}p0,N​. It is replaced by E(∣vN−1∣2∣ΦN(PtNN)∣2)\mathbb E(|v_{N-1}|^2|\Phi^N(P^N_{t_N})|^2)E(∣vN−1​∣2∣ΦN(PtN​N​)∣2).
    2. The printed factor E∣ρ0,jN(PtjN)∣2\mathbb E|\rho^N_{0,j}(P^N_{t_j})|^2E∣ρ0,jN​(Ptj​N​)∣2 next to E(∣vj∣2∣p0,j+1∣2)\mathbb E(|v_j|^2|p_{0,j+1}|^2)E(∣vj​∣2∣p0,j+1​∣2) becomes E∣ρ0,j+1N(Ptj+1N)∣2\mathbb E|\rho^N_{0,j+1}(P^N_{t_{j+1}})|^2E∣ρ0,j+1N​(Ptj+1​N​)∣2.

Contributions welcome: proofs of the milestones, in particular (28)–(29) (finite-dimensional linear algebra) and (34) (independence and orthonormality), and a construction showing that measurable minimizers of (4) exist.

Selected references

  • E. Gobet, J.-P. Lemor, X. Warin, A regression-based Monte Carlo method to solve backward stochastic differential equations, Ann. Appl. Probab. 15(3), 2172–2202, 2005. https://doi.org/10.1214/105051605000000412, preprint https://arxiv.org/abs/math/0508491v1
  • N. El Karoui, S. Peng, M. C. Quenez, Backward stochastic differential equations in finance, Math. Finance 7(1), 1–71, 1997. https://doi.org/10.1111/1467-9965.00022
  • F. A. Longstaff, E. S. Schwartz, Valuing American options by simulation: a simple least-squares approach, Rev. Financ. Stud. 14(1), 113–147, 2001. https://doi.org/10.1093/rfs/14.1.113
  • J. Zhang, A numerical scheme for BSDEs, Ann. Appl. Probab. 14(1), 459–488, 2004. https://doi.org/10.1214/aoap/1075828058
  • B. Bouchard, N. Touzi, Discrete-time approximation and Monte-Carlo simulation of backward stochastic differential equations, Stochastic Process. Appl. 111(2), 175–206, 2004. https://doi.org/10.1016/j.spa.2004.01.001
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A Numerical Scheme for BSDEs: The Step-Process Scheme Converges in L² at Rate |π| log(1/|π|), and at Rate |π| for L¹-Lipschitz or Markovian Terminal Values (Theorem 6.1)Research Paper

Why discretize a backward SDE

A backward stochastic differential equation (BSDE) prescribes the terminal value of a process instead of its initial value. Pardoux and Peng (1990) proved that a BSDE with Lipschitz driver has a unique adapted solution. Coupled with a forward diffusion it gives a forward–backward SDE (FBSDE), which represents the solution of a semilinear parabolic PDE (nonlinear Feynman–Kac formula) and, in mathematical finance, the price and hedging strategy of a contingent claim, including path-dependent ones such as lookback and Asian options (El Karoui, Peng and Quenez, 1997). In high dimension or with path-dependent payoffs the PDE route is impractical, so one wants a time-discretization of the FBSDE itself, with a proven rate of convergence.

Zhang (2004) gave such a scheme for terminal values that are Lipschitz functionals of the whole path of the forward diffusion, and proved that it converges in mean square at rate ∣π∣log⁡(1/∣π∣)|\pi|\log(1/|\pi|)∣π∣log(1/∣π∣), and at rate ∣π∣|\pi|∣π∣ for L1L^1L1-Lipschitz or Markovian terminal values. The key input is a new L2L^2L2-regularity estimate for the martingale integrand ZZZ. The same regularity estimate underlies the analysis of the Bouchard–Touzi scheme (2004) and of regression-based Monte Carlo methods (Gobet, Lemor and Warin, 2005).

Setting

Fix T>0T>0T>0, a probability space carrying a one-dimensional standard Brownian motion WWW, and its natural filtration F={Ft}\mathbb F=\{\mathcal F_t\}F={Ft​} augmented by the null sets. For x∈Rdx\in\mathbb R^dx∈Rd the FBSDE is

Xt=x+∫0tb(s,Xs) ds+∫0tσ(s,Xs) dWs,Yt=Φ(X)+∫tTf(s,Xs,Ys,Zs) ds−∫tTZs dWs,(2.1)X_t=x+\int_0^t b(s,X_s)\,ds+\int_0^t\sigma(s,X_s)\,dW_s,\qquad Y_t=\Phi(X)+\int_t^T f(s,X_s,Y_s,Z_s)\,ds-\int_t^T Z_s\,dW_s ,\tag{2.1}Xt​=x+∫0t​b(s,Xs​)ds+∫0t​σ(s,Xs​)dWs​,Yt​=Φ(X)+∫tT​f(s,Xs​,Ys​,Zs​)ds−∫tT​Zs​dWs​,(2.1)

where Xt∈RdX_t\in\mathbb R^dXt​∈Rd, Yt,Zt∈RY_t,Z_t\in\mathbb RYt​,Zt​∈R, b,σ,fb,\sigma,fb,σ,f are deterministic functions and Φ\PhiΦ is a deterministic functional of the path X=(Xt)0≤t≤TX=(X_t)_{0\le t\le T}X=(Xt​)0≤t≤T​.

Assumption 2.3 asks that b,σ,fb,\sigma,fb,σ,f be continuous, 12\tfrac1221​-Hölder in time and Lipschitz in the space variables, that Φ\PhiΦ be L∞L^\inftyL∞-Lipschitz,

∣Φ(x1)−Φ(x2)∣≤Ksup⁡0≤t≤T∣x1(t)−x2(t)∣|\Phi(x_1)-\Phi(x_2)|\le K\sup_{0\le t\le T}|x_1(t)-x_2(t)|∣Φ(x1​)−Φ(x2​)∣≤K0≤t≤Tsup​∣x1​(t)−x2​(t)∣

for càdlàg paths x1,x2x_1,x_2x1​,x2​, all with one constant K>0K>0K>0, and that sup⁡t{∣b(t,0)∣+∣σ(t,0)∣+∣f(t,0,0,0)∣}+∣Φ(0)∣≤K\sup_t\{|b(t,0)|+|\sigma(t,0)|+|f(t,0,0,0)|\}+|\Phi(0)|\le Ksupt​{∣b(t,0)∣+∣σ(t,0)∣+∣f(t,0,0,0)∣}+∣Φ(0)∣≤K. Φ\PhiΦ is L1L^1L1-Lipschitz if the supremum can be replaced by ∫0T∣x1(t)−x2(t)∣ dt\int_0^T|x_1(t)-x_2(t)|\,dt∫0T​∣x1​(t)−x2​(t)∣dt.

A partition is π:0=t0<⋯<tn=T\pi:0=t_0<\dots<t_n=Tπ:0=t0​<⋯<tn​=T, with Δti=ti−ti−1\Delta t_i=t_i-t_{i-1}Δti​=ti​−ti−1​ and ∣π∣=max⁡iΔti|\pi|=\max_i\Delta t_i∣π∣=maxi​Δti​; it is κ\kappaκ-uniform if Δti≥∣π∣/κ\Delta t_i\ge|\pi|/\kappaΔti​≥∣π∣/κ for all iii. The Euler scheme is Xt0π=xX^\pi_{t_0}=xXt0​π​=x, Xtiπ=Xti−1π+b(ti−1,Xti−1π)Δti+σ(ti−1,Xti−1π)(Wti−Wti−1)X^\pi_{t_{i}}=X^\pi_{t_{i-1}}+b(t_{i-1},X^\pi_{t_{i-1}})\Delta t_i+\sigma(t_{i-1},X^\pi_{t_{i-1}})(W_{t_i}-W_{t_{i-1}})Xti​π​=Xti−1​π​+b(ti−1​,Xti−1​π​)Δti​+σ(ti−1​,Xti−1​π​)(Wti​​−Wti−1​​), and its step process is X^tπ=Xti−1π\hat X^\pi_t=X^\pi_{t_{i-1}}X^tπ​=Xti−1​π​ on [ti−1,ti)[t_{i-1},t_i)[ti−1​,ti​). With ξπ=Φ(X^π)\xi^\pi=\Phi(\hat X^\pi)ξπ=Φ(X^π) the backward scheme is Ytnπ=ξπY^\pi_{t_n}=\xi^\piYtn​π​=ξπ and, for t∈[ti−1,ti)t\in[t_{i-1},t_i)t∈[ti−1​,ti​),

Ytπ=Ytiπ+f(ti,Xtiπ,Ytiπ,Ztiπ,1)Δti−∫ttiZrπ dWr,Ztiπ,1=1Δti+1E{∫titi+1Zrπ dr ∣ Fti},Y^\pi_t=Y^\pi_{t_i}+f\big(t_i,X^\pi_{t_i},Y^\pi_{t_i},Z^{\pi,1}_{t_i}\big)\Delta t_i-\int_t^{t_i}Z^\pi_r\,dW_r,\qquad Z^{\pi,1}_{t_i}=\frac1{\Delta t_{i+1}}E\Big\{\int_{t_i}^{t_{i+1}}Z^\pi_r\,dr\,\Big|\,\mathcal F_{t_i}\Big\},Ytπ​=Yti​π​+f(ti​,Xti​π​,Yti​π​,Zti​π,1​)Δti​−∫tti​​Zrπ​dWr​,Zti​π,1​=Δti+1​1​E{∫ti​ti+1​​Zrπ​dr​Fti​​},

with Ztnπ,1=0Z^{\pi,1}_{t_n}=0Ztn​π,1​=0. The numerical approximations are the step processes Y^tπ=Yti−1π\hat Y^\pi_t=Y^\pi_{t_{i-1}}Y^tπ​=Yti−1​π​ and Z^tπ=Zti−1π,1\hat Z^\pi_t=Z^{\pi,1}_{t_{i-1}}Z^tπ​=Zti−1​π,1​ on [ti−1,ti)[t_{i-1},t_i)[ti−1​,ti​).

Formalization targets

Goal: Theorem 6.1, (6.5)–(6.6)

Assume Assumption 2.3 and that ZZZ is càdlàg. If fff does not depend on zzz, or π\piπ is κ\kappaκ-uniform, then

sup⁡0≤t≤TE{∣Yt−Y^tπ∣2}+E{∫0T∣Zt−Z^tπ∣2dt}≤C(1+∣x∣2) ∣π∣log⁡1∣π∣(6.5)\sup_{0\le t\le T}E\{|Y_t-\hat Y^\pi_t|^2\}+E\Big\{\int_0^T|Z_t-\hat Z^\pi_t|^2dt\Big\}\le C(1+|x|^2)\,|\pi|\log\frac1{|\pi|}\tag{6.5}0≤t≤Tsup​E{∣Yt​−Y^tπ​∣2}+E{∫0T​∣Zt​−Z^tπ​∣2dt}≤C(1+∣x∣2)∣π∣log∣π∣1​(6.5)

for ∣π∣≤e−1/2|\pi|\le e^{-1/2}∣π∣≤e−1/2, and, if moreover Φ\PhiΦ is L1L^1L1-Lipschitz or Φ(X)=g(XT)\Phi(X)=g(X_T)Φ(X)=g(XT​), the same left-hand side is at most C(1+∣x∣2)∣π∣C(1+|x|^2)|\pi|C(1+∣x∣2)∣π∣ (6.6). The constant CCC depends only on TTT, KKK, κ\kappaκ and ddd. The goal fixes the rates and leaves CCC unspecified.

Milestones

  1. Lemma 3.2: ∥Zt∥p≤Cp(1+∣x∣)\|Z_t\|_p\le C_p(1+|x|)∥Zt​∥p​≤Cp​(1+∣x∣), and the time-regularity E{∣Xt−Xti−1∣2+∣Yt−Yti−1∣2}≤C(1+∣x∣2)∣π∣E\{|X_t-X_{t_{i-1}}|^2+|Y_t-Y_{t_{i-1}}|^2\}\le C(1+|x|^2)|\pi|E{∣Xt​−Xti−1​​∣2+∣Yt​−Yti−1​​∣2}≤C(1+∣x∣2)∣π∣.
  2. Lemma 3.3 and Corollary 3.4, a weighted martingale inequality over a partition.
  3. Theorem 3.1, the L2L^2L2-regularity of ZZZ: ∑iE∫ti−1ti[∣Zt−Zti−1∣2+∣Zt−Zti∣2] dt≤C(1+∣x∣2)∣π∣\sum_i E\int_{t_{i-1}}^{t_i}[|Z_t-Z_{t_{i-1}}|^2+|Z_t-Z_{t_i}|^2]\,dt\le C(1+|x|^2)|\pi|∑i​E∫ti−1​ti​​[∣Zt​−Zti−1​​∣2+∣Zt​−Zti​​∣2]dt≤C(1+∣x∣2)∣π∣.
  4. Lemma 4.1, Theorem 4.2 and Corollary 4.4: errors of the Euler scheme, its step process, and Φ(X^π)\Phi(\hat X^\pi)Φ(X^π).
  5. Lemma 5.4 (a backward discrete Gronwall inequality), Theorem 5.3 and Remark 5.5 (the scheme at the grid points), and Theorem 5.6 (the step processes).

Significance

Theorem 6.1 gives an explicit, implementable scheme for FBSDEs with path-dependent terminal values and a mean-square rate that is sharp up to the logarithm: by Remark 4.3 the factor log⁡(1/∣π∣)\log(1/|\pi|)log(1/∣π∣) cannot be removed for L∞L^\inftyL∞-Lipschitz functionals, since it is already present in the uniform error of the Euler step process. Theorem 3.1 is reusable on its own: any time-discretization of a BSDE whose error is measured against Zti−1Z_{t_{i-1}}Zti−1​​ needs it.

All results are proved in the paper. As far as is known, none has a machine-checked proof; the platform has no prior BSDE discretization result. The work is formalizing the known proofs, which needs the L2L^2L2 Itô integral, Itô's isometry and martingale representation, the standard a priori estimates for SDEs and BSDEs, and Doob's maximal inequality in continuous time.

Difficulty

The obvious argument compares the BSDE and the scheme step by step and closes with a discrete Gronwall inequality (Lemma 5.4). Its error terms include E∫ti−1ti∣Zr−Zti−1∣2drE\int_{t_{i-1}}^{t_i}|Z_r-Z_{t_{i-1}}|^2drE∫ti−1​ti​​∣Zr​−Zti−1​​∣2dr, and no pointwise estimate E∣Zt−Zs∣2≤C∣t−s∣E|Z_t-Z_s|^2\le C|t-s|E∣Zt​−Zs​∣2≤C∣t−s∣ is available: ZZZ is only square integrable in time, with no continuity modulus in general. The proof therefore needs the summed L2L^2L2-regularity of Theorem 3.1, whose proof goes through smooth approximations of the coefficients and of Φ\PhiΦ, the representation of ZZZ by the variational process ∇X\nabla X∇X, and the martingale inequality of Lemma 3.3. The log⁡(1/∣π∣)\log(1/|\pi|)log(1/∣π∣) rate comes from the maximum of nnn Gaussian increments, which an estimate of sup⁡tE\sup_tEsupt​E cannot see.

Formalization scope

Time is ℝ≥0; the state space is EuclideanSpace ℝ (Fin d); the Brownian motion is the coordinate 000 of a Fin 1-indexed standard Brownian motion; F\mathbb FF is the augmented filtration. These, the L2L^2L2 Itô integral and the class L2(F)L^2(\mathbb F)L2(F) are reused from the published modules Peng1990_SMP_Stochastic and ReflectedBSDE_Existence_Setting. Every expectation and time integral of a square is a lower Lebesgue integral in [0,∞][0,\infty][0,∞], so a non-integrable error cannot make a bound vacuous; this rules out the trivializing formalization in which a Bochner integral of a non-integrable error is 000.

The solutions (X,Y,Z)(X,Y,Z)(X,Y,Z) and (Yπ,Zπ)(Y^\pi,Z^\pi)(Yπ,Zπ) are quantified as solutions of their equations; the Euler scheme, X^π\hat X^\piX^π, Zπ,1Z^{\pi,1}Zπ,1, Y^π\hat Y^\piY^π, Z^π\hat Z^\piZ^π are constructed. Each constant CCC is chosen before the probability space, the data, the solution and the partition. Disclosed readings: (i) the log-rate statements assume ∣π∣≤e−1/2|\pi|\le e^{-1/2}∣π∣≤e−1/2, the paper's "π\piπ fine enough" (p. 478); (ii) "ZZZ is càdlàg" includes ZT=ZT−Z_T=Z_{T-}ZT​=ZT−​; (iii) the uniformity constant of Definition 5.2 is κ\kappaκ, not KKK, and CCC may depend on it; (iv) the Hölder constant in time is KKK; (v) X^Tπ=XTπ\hat X^\pi_T=X^\pi_TX^Tπ​=XTπ​, Y^Tπ=YTπ\hat Y^\pi_T=Y^\pi_TY^Tπ​=YTπ​, Z^Tπ=0\hat Z^\pi_T=0Z^Tπ​=0; (vi) Lemma 3.3 uses ∣Λti−1∣|\Lambda_{t_{i-1}}|∣Λti−1​​∣ in place of Λti−1\Lambda_{t_{i-1}}Λti−1​​, which strengthens it; (vii) Lemma 5.4 assumes C≥0C\ge0C≥0. Completeness of the probability space is not used.

Not formalized here: Lemma 2.2 (smooth approximation of Φ\PhiΦ, cited from Ma–Zhang), the background Lemmas 2.4–2.7, and the representation (6.3)–(6.4) of the scheme by functions of the Euler grid values. Welcome contributions: the SDE and BSDE a priori estimates under Lipschitz coefficients, Itô's isometry and martingale representation for the reused Itô integral, and Doob's L2L^2L2 inequality in continuous time; all are reusable well beyond this mission.

Selected references

  • J. Zhang, A numerical scheme for BSDEs, Ann. Appl. Probab. 14(1), 459–488, 2004. https://doi.org/10.1214/aoap/1075828058
  • E. Pardoux and S. Peng, Adapted solution of a backward stochastic differential equation, Systems Control Lett. 14, 55–61, 1990. https://doi.org/10.1016/0167-6911(90)90082-6
  • N. El Karoui, S. Peng and M. C. Quenez, Backward stochastic differential equations in finance, Math. Finance 7(1), 1–71, 1997. https://doi.org/10.1111/1467-9965.00022
  • J. Ma and J. Zhang, Representation theorems for backward stochastic differential equations, Ann. Appl. Probab. 12(4), 1390–1418, 2002. https://doi.org/10.1214/aoap/1037125868
  • B. Bouchard and N. Touzi, Discrete-time approximation and Monte-Carlo simulation of backward stochastic differential equations, Stochastic Process. Appl. 111(2), 175–206, 2004. https://doi.org/10.1016/j.spa.2004.01.001
  • E. Gobet, J.-P. Lemor and X. Warin, A regression-based Monte Carlo method to solve backward stochastic differential equations, Ann. Appl. Probab. 15(3), 2172–2202, 2005. https://doi.org/10.1214/105051605000000412
19 thms1 active userReviewed
Markov ChainProbabilityReinforcement Learning·Captain: mikedeng1

On Actor-Critic Algorithms: Convergence of Actor-Critic Algorithms with TD(1) and TD(λ) Critics on Finite MDPsResearch Paper

Motivation

Reinforcement-learning methods for Markov decision processes split into critic-only methods, which learn an approximate value function and act greedily with respect to it, and actor-only methods, which adjust a parameterized policy along a simulated estimate of the gradient of its performance. Critic-only methods with function approximation can fail to converge; actor-only gradient estimates have high variance. Actor–critic methods combine the two: a critic learns, by temporal-difference (TD) learning, just enough about the value function to give the actor a low-variance gradient direction.

Konda and Tsitsiklis (SIAM J. Control Optim. 42 (2003)) gave the first convergence proof for actor–critic algorithms whose critic uses linear function approximation. Their key observation, found independently by Sutton, McAllester, Singh and Mansour (NIPS 1999), is that the critic need not approximate the value function: it suffices to compute its projection onto a low-dimensional subspace spanned by features determined by the policy parameterization. Earlier convergence results (Konda and Borkar, 1999) covered lookup-table representations only. Actor–critic algorithms, in many later variants, are now a standard tool of reinforcement learning, and this paper is the reference for their asymptotic analysis in the average-cost setting.

Setting

A finite cost MDP consists of finite sets X\mathbb XX (states) and U\mathbb UU (actions), transition probabilities p(y∣x,u)p(y\mid x,u)p(y∣x,u) and a one-stage cost c(x,u)∈Rc(x,u)\in\mathbb Rc(x,u)∈R. A randomized stationary policy with parameter θ∈Rn\theta\in\mathbb R^nθ∈Rn chooses action uuu in state xxx with probability μθ(u∣x)\mu_\theta(u\mid x)μθ​(u∣x). Under the policy θ\thetaθ, the states {Xk}\{X_k\}{Xk​} form a Markov chain with transition matrix P(θ)xy=∑uμθ(u∣x)p(y∣x,u)P(\theta)_{xy}=\sum_u\mu_\theta(u\mid x)p(y\mid x,u)P(θ)xy​=∑u​μθ​(u∣x)p(y∣x,u), and the pairs {Xk,Uk}\{X_k,U_k\}{Xk​,Uk​} a chain with matrix PθP_\thetaPθ​. When these chains are irreducible and aperiodic, πθ\pi_\thetaπθ​ denotes the stationary law of {Xk}\{X_k\}{Xk​}, ηθ(x,u)=πθ(x)μθ(u∣x)\eta_\theta(x,u)=\pi_\theta(x)\mu_\theta(u\mid x)ηθ​(x,u)=πθ​(x)μθ​(u∣x), and the average cost is

αˉ(θ)=∑x,uc(x,u) ηθ(x,u).\bar\alpha(\theta)=\sum_{x,u}c(x,u)\,\eta_\theta(x,u).αˉ(θ)=x,u∑​c(x,u)ηθ​(x,u).

The score is ψθ(x,u)=∇ln⁡μθ(u∣x)∈Rn\psi_\theta(x,u)=\nabla\ln\mu_\theta(u\mid x)\in\mathbb R^nψθ​(x,u)=∇lnμθ​(u∣x)∈Rn, and ⟨f,g⟩θ=∑x,uηθ(x,u)f(x,u)g(x,u)\langle f,g\rangle_\theta=\sum_{x,u}\eta_\theta(x,u)f(x,u)g(x,u)⟨f,g⟩θ​=∑x,u​ηθ​(x,u)f(x,u)g(x,u).

The critic approximates Q-values by r′ϕθ(x,u)r'\phi_\theta(x,u)r′ϕθ​(x,u) with features ϕθ(x,u)∈Rm\phi_\theta(x,u)\in\mathbb R^mϕθ​(x,u)∈Rm whose span contains the components of ψθ\psi_\thetaψθ​. Along one simulated trajectory (X^k,U^k)(\hat X_k,\hat U_k)(X^k​,U^k​), where U^k+1\hat U_{k+1}U^k+1​ is drawn from μθk(⋅∣X^k+1)\mu_{\theta_k}(\cdot\mid\hat X_{k+1})μθk​​(⋅∣X^k+1​), the algorithm updates an average-cost estimate αk\alpha_kαk​, the critic parameter rkr_krk​ and an eligibility trace Z^k\hat Z_kZ^k​ at step size γk\gamma_kγk​ (equation (3.1)), and the actor parameter by

θk+1=θk−βkΓ(rk) rk′ϕθk(X^k+1,U^k+1) ψθk(X^k+1,U^k+1)(3.2)\theta_{k+1}=\theta_k-\beta_k\Gamma(r_k)\,r_k'\phi_{\theta_k}(\hat X_{k+1},\hat U_{k+1})\,\psi_{\theta_k}(\hat X_{k+1},\hat U_{k+1})\qquad(3.2)θk+1​=θk​−βk​Γ(rk​)rk′​ϕθk​​(X^k+1​,U^k+1​)ψθk​​(X^k+1​,U^k+1​)(3.2)

at a slower step size βk\beta_kβk​. The TD(1) critic resets its trace when the state x∗x^*x∗ is entered; the TD(λ\lambdaλ) critic discounts it by λ∈(0,1)\lambda\in(0,1)λ∈(0,1).

Formalization targets

Goal: Theorem 3.4

Under Assumptions 2.1 (positive, smooth policies; irreducible aperiodic chains; uniform reachability of x∗x^*x∗), 3.1–3.2 (bounded smooth features spanning the scores, uniformly nondegenerate) and 3.3 (two-time-scale step sizes and the scaling Γ\GammaΓ),

(a) TD(1):  lim inf⁡k∣∇αˉ(θk)∣=0  w.p.1;(b) ∀ϵ>0 ∃λˉ<1 ∀λ∈[λˉ,1): lim inf⁡k∣∇αˉ(θk)∣<ϵ  w.p.1.\text{(a) TD(1): }\ \liminf_k|\nabla\bar\alpha(\theta_k)|=0\ \text{ w.p.1};\qquad \text{(b) }\forall\epsilon>0\ \exists\bar\lambda<1\ \forall\lambda\in[\bar\lambda,1):\ \liminf_k|\nabla\bar\alpha(\theta_k)|<\epsilon\ \text{ w.p.1}.(a) TD(1):  kliminf​∣∇αˉ(θk​)∣=0  w.p.1;(b) ∀ϵ>0 ∃λˉ<1 ∀λ∈[λˉ,1): kliminf​∣∇αˉ(θk​)∣<ϵ  w.p.1.

The statement leaves the initial parameters and the initial state–action law arbitrary.

Milestones

In attack order: the gradient formula ∇αˉ(θ)=⟨ψθ,Qθ⟩θ\nabla\bar\alpha(\theta)=\langle\psi_\theta,Q_\theta\rangle_\theta∇αˉ(θ)=⟨ψθ​,Qθ​⟩θ​ for every Poisson solution, with bounded Hessian (Theorem 4.6); boundedness of the regenerative quantities (Lemma 5.1) and of the trace moments (Lemma 5.2); uniform positive definiteness of the critic's mean matrix Gˉ(θ)\bar G(\theta)Gˉ(θ) for TD(1) and TD(λ\lambdaλ) (Lemmas 5.3, 5.6); critic tracking, ∣Gˉ(θk)Rk−hˉ(θk)∣→0|\bar G(\theta_k)R_k-\bar h(\theta_k)|\to0∣Gˉ(θk​)Rk​−hˉ(θk​)∣→0 (Theorem 5.7); the bias of the actor direction, sup⁡θ∣f(θ)−∇αˉ(θ)∣≤C(1−λ)\sup_\theta|f(\theta)-\nabla\bar\alpha(\theta)|\le C(1-\lambda)supθ​∣f(θ)−∇αˉ(θ)∣≤C(1−λ) (Lemma 6.1); the descent inequality (6.1); and the convergence of the noise terms (Lemma 6.2).

Significance

The theorem says that a policy-gradient method whose gradient is estimated by a linearly parameterized TD critic, rather than by Monte Carlo returns, still converges to a stationary point of the average cost (exactly for TD(1), approximately for TD(λ\lambdaλ)). It justifies the compatible features principle (the critic's features must span the score functions), the two-time-scale step-size design, and the trade-off in λ\lambdaλ between variance and bias of the actor direction. The intermediate results are of independent use: Theorem 4.6 is the average-cost policy-gradient theorem for arbitrary Poisson solutions, and Theorem 5.7 is a tracking result for linear stochastic approximation driven by a Markov chain whose kernel changes slowly.

The result is proved in the paper, but the proofs of Theorem 4.6, of parts of the verification of the stochastic-approximation hypotheses and of Theorem 6.3 are given as outlines, with details deferred to a separate appendix and to Theorem A.7, recalled from another paper. No machine-checked proof of the theorem, or of the convergence of any actor–critic method, is known. The mission asks for a formal proof of the finite-case theorem and its milestones, which fills in the outlined steps. The finite-case gradient formula of §2 (Theorem 2.2, recalled from Marbach and Tsitsiklis) is posed, unproved, elsewhere on the platform in a reward-MDP form; it is a special case of milestone Theorem 4.6.

Difficulty

The obvious argument treats the actor as a stochastic gradient method with a noisy gradient estimate. It fails at the first step: the critic's estimate rk′ϕθkr_k'\phi_{\theta_k}rk′​ϕθk​​ is biased at every finite time, and the bias does not vanish unless the critic converges, while the critic's target rˉ(θk)\bar r(\theta_k)rˉ(θk​) moves with the actor. The noise is Markovian, generated by a chain whose transition kernel depends on the current parameter, not a martingale difference sequence. Making the two time scales interact correctly requires a Poisson-equation decomposition of the Markov noise that is uniform in θ\thetaθ, together with moment bounds for the eligibility trace, which for TD(1) is an unbounded sum over a regeneration cycle. Uniformity in θ\thetaθ is essential, because the actor iterates θk\theta_kθk​ are not assumed to stay in a bounded set.

Formalization scope

State and action sets are finite types; parameters live in EuclideanSpace ℝ (Fin n) and EuclideanSpace ℝ (Fin m), so ∣⋅∣|\cdot|∣⋅∣ is the Euclidean norm and Mathlib's gradient is ∇\nabla∇. The transition probability p(y∣x,u)p(y\mid x,u)p(y∣x,u) is stored as p x u y. πθ\pi_\thetaπθ​ is a stationary probability vector of P(θ)P(\theta)P(θ), unique under Assumption 2.1(c). The law of the simulated path is built on (X×U)N(\mathbb X\times\mathbb U)^{\mathbb N}(X×U)N by the Ionescu-Tulcea construction (Kernel.trajMeasure), with the next action drawn under the actor parameter that the recursion computes from the history; nothing about the critic or the actor's behaviour is assumed.

Readings and corrections, each also recorded in the affected items:

  • Assumption 3.3(b) is corrected. The printed ∣r∣Γ(r)∈[C1,C2]|r|\Gamma(r)\in[C_1,C_2]∣r∣Γ(r)∈[C1​,C2​] for all rrr is unsatisfiable at r=0r=0r=0 and would make the theorem vacuous; it is formalized as (1+∣r∣)Γ(r)∈[C1,C2](1+|r|)\Gamma(r)\in[C_1,C_2](1+∣r∣)Γ(r)∈[C1​,C2​], which Γ(r)=1/(1+∣r∣)\Gamma(r)=1/(1+|r|)Γ(r)=1/(1+∣r∣) satisfies. The second inequality of (3.3) is quantified over Rm\mathbb R^mRm, the domain of Γ\GammaΓ, not the printed Rn\mathbb R^nRn.
  • Assumption 4.9 (the features have zero mean under μθ(⋅∣x∗)\mu_\theta(\cdot\mid x^*)μθ​(⋅∣x∗)) is added to part (a), and to the TD(1) cases of Theorem 5.7 and Lemma 6.2: the TD(1) analysis uses it and Theorem 6.3 assumes it, though Theorem 3.4 does not list it.
  • "λ\lambdaλ sufficiently close to 1" means: some λˉ<1\bar\lambda<1λˉ<1 such that all λ∈[λˉ,1)\lambda\in[\bar\lambda,1)λ∈[λˉ,1) work.
  • The α\alphaα-update of (3.1) uses c(X^k+1,U^k+1)c(\hat X_{k+1},\hat U_{k+1})c(X^k+1​,U^k+1​) as printed.
  • In (6.1), Γ(rˉ(θ))\Gamma(\bar r(\theta))Γ(rˉ(θ)) is read as Γ(rˉ(θk))\Gamma(\bar r(\theta_k))Γ(rˉ(θk​)).
  • The matrix ⟨Pθk+1ϕθ,ϕθ′⟩θ\langle P_\theta^{k+1}\phi_\theta,\phi_\theta'\rangle_\theta⟨Pθk+1​ϕθ​,ϕθ′​⟩θ​ in the TD(λ\lambdaλ) Gˉ1\bar G_1Gˉ1​ is oriented so that Gˉ1\bar G_1Gˉ1​ is the steady-state mean of the critic's update matrix.
  • Results stated in the paper for Polish spaces (Theorems 4.6, 5.7) are stated under the finite assumptions that the paper says imply them; "w.p.1" in Theorem 5.7 is made explicit.

The lim inf⁡\liminfliminf is taken in [0,∞][0,\infty][0,∞], so a sequence with ∣∇αˉ(θk)∣→∞|\nabla\bar\alpha(\theta_k)|\to\infty∣∇αˉ(θk​)∣→∞ cannot satisfy the conclusion through a junk value, and differentiability of αˉ\bar\alphaαˉ is part of the conclusion, so the statement cannot hold because Lean's gradient returns 000 at non-differentiable points. Series (tsum) and matrix inverses in the milestone objects converge, respectively are invertible, under the assumptions. The hypotheses are satisfiable: Γ(r)=1/(1+∣r∣)\Gamma(r)=1/(1+|r|)Γ(r)=1/(1+∣r∣), βk=(k+1)−1\beta_k=(k+1)^{-1}βk​=(k+1)−1, γk=(k+1)−2/3\gamma_k=(k+1)^{-2/3}γk​=(k+1)−2/3 and the features ϕθ=ψθ\phi_\theta=\psi_\thetaϕθ​=ψθ​ (which satisfy Assumption 4.9 at every state) meet the parts that could be in doubt.

A complete development needs finite Markov-chain theory uniform in a parameter (existence, uniqueness and smooth dependence of stationary laws; geometric ergodicity; Poisson equations; regeneration), differentiation of θ↦πθ\theta\mapsto\pi_\thetaθ↦πθ​, almost-sure convergence of linear stochastic approximation with Markov noise, and martingale convergence. The Markov-chain and stochastic-approximation parts are reusable well beyond this mission. Contributions of proofs of any milestone, of auxiliary lemmas on parameterized finite Markov chains, and of the general two-time-scale tracking theorem (the paper's Theorem A.7) are welcome.

Selected references

  • V. R. Konda and J. N. Tsitsiklis, On Actor-Critic Algorithms, SIAM J. Control Optim. 42(4), 1143–1166, 2003. https://doi.org/10.1137/S0363012901385691
  • R. S. Sutton, D. McAllester, S. Singh and Y. Mansour, Policy Gradient Methods for Reinforcement Learning with Function Approximation, NIPS 12, 2000. https://papers.nips.cc/paper/1713-policy-gradient-methods-for-reinforcement-learning-with-function-approximation
  • V. R. Konda and V. S. Borkar, Actor-Critic–Type Learning Algorithms for Markov Decision Processes, SIAM J. Control Optim. 38(1), 94–123, 1999. https://doi.org/10.1137/S036301299731669X
  • J. N. Tsitsiklis and B. Van Roy, Average Cost Temporal-Difference Learning, Automatica 35(11), 1799–1808, 1999. https://doi.org/10.1016/S0005-1098(99)00099-0
  • P. Marbach and J. N. Tsitsiklis, Simulation-Based Optimization of Markov Reward Processes, IEEE Trans. Automat. Control 46(2), 191–209, 2001. https://doi.org/10.1109/9.905687
14 thms1 active userReviewed
Operations ResearchProbability·Captain: mikedeng1

Is Network Traffic Approximated by Stable Lévy Motion or Fractional Brownian Motion? 2: Superposed ON/OFF Input Under Slow Growth Converges (fidi) to α-Stable Lévy MotionResearch Paper

Motivation

Measurements of Ethernet and Web traffic in the 1990s showed burstiness at every time scale, long-range dependence, and file sizes and transmission times with tails like x−αx^{-\alpha}x−α, 1<α<21<\alpha<21<α<2 (Leland, Taqqu, Willinger and Wilson, 1994; Crovella and Bestavros, 1997). The standard explanation models each user as an ON/OFF source that alternates between transmitting at unit rate and staying silent, with heavy-tailed period lengths. Many such sources are superposed and time is rescaled. Taqqu, Willinger and Sherman (1997) showed that the limit is fractional Brownian motion when the number of sources is sent to infinity first. That limit is the basis of Gaussian queueing models of network buffers.

Mikosch, Resnick, Rootzén and Stegeman (2002) asked what happens when the number of sources MMM and the time scale TTT grow together. The answer depends on how fast M=M(T)M=M(T)M=M(T) grows. Under fast growth the limit is fractional Brownian motion; this is Theorem 4 of the paper and a separate mission. Under slow growth the limit is an α-stable Lévy motion: it has independent increments and infinite variance, and its sample paths jump. This mission formalizes the slow growth result, Theorem 2. The two answers lead to different buffer and dimensioning models, so the dichotomy matters for traffic engineering.

Setting

Period laws. ON-periods have law FonF_{\mathrm{on}}Fon​ and OFF-periods have law FoffF_{\mathrm{off}}Foff​; both are laws of non-negative random variables. Their means are μon\mu_{\mathrm{on}}μon​ and μoff\mu_{\mathrm{off}}μoff​, and μ=μon+μoff\mu=\mu_{\mathrm{on}}+\mu_{\mathrm{off}}μ=μon​+μoff​. Their right tails Fˉ=1−F\bar F=1-FFˉ=1−F satisfy (2.1)–(2.2):

Fˉon(x)=x−αLon(x),Fˉoff(x)=x−αoffLoff(x),1<α<αoff<2,\bar F_{\mathrm{on}}(x)=x^{-\alpha}L_{\mathrm{on}}(x),\qquad \bar F_{\mathrm{off}}(x)=x^{-\alpha_{\mathrm{off}}}L_{\mathrm{off}}(x),\qquad 1<\alpha<\alpha_{\mathrm{off}}<2,Fˉon​(x)=x−αLon​(x),Fˉoff​(x)=x−αoff​Loff​(x),1<α<αoff​<2,

where LonL_{\mathrm{on}}Lon​ and LoffL_{\mathrm{off}}Loff​ are slowly varying: L(cx)/L(x)→1L(cx)/L(x)\to1L(cx)/L(x)→1 for every c>0c>0c>0. The ON-periods therefore have the heavier tail.

One source. Let X1,X2,…X_1,X_2,\dotsX1​,X2​,… be iid FonF_{\mathrm{on}}Fon​ and Yoff,Y1,Y2,…Y_{\mathrm{off}},Y_1,Y_2,\dotsYoff​,Y1​,Y2​,… iid FoffF_{\mathrm{off}}Foff​. Let BBB be Bernoulli with P(B=1)=μon/μP(B=1)=\mu_{\mathrm{on}}/\muP(B=1)=μon​/μ. Let Xon(0)X^{(0)}_{\mathrm{on}}Xon(0)​ and Yoff(0)Y^{(0)}_{\mathrm{off}}Yoff(0)​ have the integrated-tail laws F(0)(x)=μF−1∫0xFˉ(s) dsF^{(0)}(x)=\mu_F^{-1}\int_0^x\bar F(s)\,dsF(0)(x)=μF−1​∫0x​Fˉ(s)ds. All of these variables are independent. Put Zi=Xi+YiZ_i=X_i+Y_iZi​=Xi​+Yi​. The delay is T0=B(Xon(0)+Yoff)+(1−B)Yoff(0)T_0=B(X^{(0)}_{\mathrm{on}}+Y_{\mathrm{off}})+(1-B)Y^{(0)}_{\mathrm{off}}T0​=B(Xon(0)​+Yoff​)+(1−B)Yoff(0)​, and the renewal epochs are Tn=T0+∑i=1nZiT_n=T_0+\sum_{i=1}^nZ_iTn​=T0​+∑i=1n​Zi​. The source is ON at time ttt when

Wt=B 1[0,Xon(0))(t)+∑n≥01[Tn,Tn+Xn+1)(t)=1.W_t=B\,\mathbf 1_{[0,X^{(0)}_{\mathrm{on}})}(t)+\sum_{n\ge0}\mathbf 1_{[T_n,T_n+X_{n+1})}(t)=1 .Wt​=B1[0,Xon(0)​)​(t)+n≥0∑​1[Tn​,Tn​+Xn+1​)​(t)=1.

This construction makes WWW stationary.

Superposition. MMM iid sources W(1),…,W(M)W^{(1)},\dots,W^{(M)}W(1),…,W(M) feed a server. N(t)=∑mWt(m)N(t)=\sum_mW^{(m)}_tN(t)=∑m​Wt(m)​ is the number of active sources, and A(t)=∫0tN(s) dsA(t)=\int_0^tN(s)\,dsA(t)=∫0t​N(s)ds is the cumulative input; its mean is EA(t)=Mμ−1μontEA(t)=M\mu^{-1}\mu_{\mathrm{on}}tEA(t)=Mμ−1μon​t.

Growth. b(t)=(1/Fˉon)←(t)b(t)=(1/\bar F_{\mathrm{on}})^{\leftarrow}(t)b(t)=(1/Fˉon​)←(t) is the quantile function (2.9). M=M(T)M=M(T)M=M(T) is integer valued, non-decreasing and tends to infinity. Slow Growth Condition 1 is b(MT)/T→0b(MT)/T\to0b(MT)/T→0.

Stable laws. Sα(σ,β,μ)S_\alpha(\sigma,\beta,\mu)Sα​(σ,β,μ) is the law with characteristic function exp⁡{−σα∣θ∣α(1−iβ sign(θ)tan⁡πα2)+iμθ}\exp\{-\sigma^\alpha|\theta|^\alpha(1-i\beta\,\mathrm{sign}(\theta)\tan\frac{\pi\alpha}2)+i\mu\theta\}exp{−σα∣θ∣α(1−iβsign(θ)tan2πα​)+iμθ} for α≠1\alpha\neq1α=1. The α-stable Lévy motion Xα,σ,βX_{\alpha,\sigma,\beta}Xα,σ,β​ has independent stationary increments, and X(t)∼Sα(σt1/α,β,0)X(t)\sim S_\alpha(\sigma t^{1/\alpha},\beta,0)X(t)∼Sα​(σt1/α,β,0).

Formalization targets

Goal: Theorem 2 (p. 40)

With Cα=1−αΓ(2−α)cos⁡(πα/2)C_\alpha=\dfrac{1-\alpha}{\Gamma(2-\alpha)\cos(\pi\alpha/2)}Cα​=Γ(2−α)cos(πα/2)1−α​, σ=Cα−1/α\sigma=C_\alpha^{-1/\alpha}σ=Cα−1/α​ and c=μoff/μ1+1/αc=\mu_{\mathrm{off}}/\mu^{1+1/\alpha}c=μoff​/μ1+1/α, under Condition 1

A(T⋅)−TMμ−1μon(⋅)b(MT)→ fidi c Xα,σ,1(⋅).\frac{A(T\cdot)-TM\mu^{-1}\mu_{\mathrm{on}}(\cdot)}{b(MT)}\xrightarrow{\ fidi\ }c\,X_{\alpha,\sigma,1}(\cdot).b(MT)A(T⋅)−TMμ−1μon​(⋅)​ fidi ​cXα,σ,1​(⋅).

Every constant is stated as printed. The normalisation is the paper's b(MT)b(MT)b(MT) and the limit is the totally skewed (β=1\beta=1β=1) Lévy motion.

Milestones (§5, in the order of the proof)

  • Lemmas 3 and 6: the initial ON-periods (A1A_1A1​) and the overshoots beyond TTT (A3A_3A3​) are negligible at scale b(MT)b(MT)b(MT).
  • Lemmas 4 and 5: the per-source renewal count ξT\xi_TξT​ concentrates around μT=T/μ\mu_T=T/\muμT​=T/μ with probability 1−o(1/M)1-o(1/M)1−o(1/M), plus a truncated-overshoot bound.
  • Lemmas 7, 8 and 9: the left tails of the centred sums Sn=∑k≤nJkS_n=\sum_{k\le n}J_kSn​=∑k≤n​Jk​ are negligible, and replacing ξT\xi_TξT​ by [μT][\mu_T][μT​] is harmless. Here Jk=ron(Xk−μon)−roff(Yk−μoff)J_k=r_{\mathrm{on}}(X_k-\mu_{\mathrm{on}})-r_{\mathrm{off}}(Y_k-\mu_{\mathrm{off}})Jk​=ron​(Xk​−μon​)−roff​(Yk​−μoff​).
  • Lemma 10: [b(MT)]−1A21→cXα,σ,1(1)[b(MT)]^{-1}A_{21}\to cX_{\alpha,\sigma,1}(1)[b(MT)]−1A21​→cXα,σ,1​(1) in distribution.
  • Lemmas 11 and 12: tails of linear combinations of increments, and the two-dimensional limit.

Significance

Theorem 2 identifies the limit regime where the Gaussian heavy-traffic picture fails for ON/OFF traffic. When few sources are observed over long horizons, the aggregate input has infinite-variance, independent-increment fluctuations of size b(MT)≈(MT)1/αb(MT)\approx(MT)^{1/\alpha}b(MT)≈(MT)1/α. Read together with Theorem 4, the result says the growth rate of MMM relative to TTT decides between the two classical models of network input. The proof turns the ON/OFF superposition into row-wise iid random sums and uses a heavy-tailed large-deviation estimate for random walks (Cline and Hsing). That technique carries over to other renewal-reward processes with regularly varying rewards.

The result is proved in the paper. No machine-checked version exists, either of the theorem or of the probabilistic substrate it rests on. Formalization would produce:

  • a stationary alternating renewal process in Lean;
  • a usable notion of regular variation with the quantile function bbb;
  • stable laws given by characteristic functions;
  • the infinitely divisible convergence criterion (Petrov's conditions (A)–(C)) that the proof cites for row-wise iid sums.

Correction. Lemma 12 as printed omits the normalisation [b(MT)]−1[b(MT)]^{-1}[b(MT)]−1 on its left-hand side. Its proof and its use in Theorem 2 both have it, and without it the claim fails because the left-hand side grows. The mission states Lemma 12 with the normalisation. Lemma 11's upper summation limits μTt\mu_{Tt}μTt​ are read as integer parts, as elsewhere in §5.

Difficulty

The natural first idea is to treat A(T)A(T)A(T) as a sum of MMM iid terms and apply the stable central limit theorem for triangular arrays. This fails as stated: each source's contribution A(m)(T)A^{(m)}(T)A(m)(T) is itself a random sum ∑k≤ξTXk\sum_{k\le\xi_T}X_k∑k≤ξT​​Xk​, and its count ξT\xi_TξT​ depends strongly on the XkX_kXk​. Moreover, MMM grows too slowly for a law-of-large-numbers smoothing across sources. The count must be replaced by its mean simultaneously for all MMM sources, with an error probability o(1/M)o(1/M)o(1/M), uniformly as T→∞T\to\inftyT→∞. This requires the two-sided large-deviation estimate of Lemma 4. Its lower tail rests on the Cline–Hsing asymptotics P(Sn>x)∼nFˉ(x)P(S_n>x)\sim n\bar F(x)P(Sn​>x)∼nFˉ(x) for heavy-tailed random walks; its upper tail rests on a Cramér bound. Then Petrov's conditions must be checked at the exact scale b(MT)b(MT)b(MT). That needs Potter bounds for the slowly varying factors and a non-uniform Berry–Esseen estimate for the truncated sums. None of these tools is in Mathlib.

Formalization scope

All declarations are in the namespace NetTraffic.OnOffStable, in one definitions file.

Conventions.

  • Each time scale TTT has its own probability space (ΩT,PT)(\Omega_T,P_T)(ΩT​,PT​), which carries M(T)M(T)M(T) independent sources indexed 0,…,M(T)−10,\dots,M(T)-10,…,M(T)−1. Only laws matter, and the statements quantify over every such family.
  • Lean's X n and Y n are the paper's Xn+1X_{n+1}Xn+1​ and Yn+1Y_{n+1}Yn+1​.
  • ξT\xi_TξT​ is a Set.ncard (junk 000 on a null event). WWW is a tsum of indicators, and AAA is an interval integral.
  • b(t)=inf⁡{x>0:tFˉon(x)≤1}b(t)=\inf\{x>0:t\bar F_{\mathrm{on}}(x)\le1\}b(t)=inf{x>0:tFˉon​(x)≤1}. This set is non-empty for t>0t>0t>0, so bbb is never the junk value 000, and b(MT)/T→0b(MT)/T\to0b(MT)/T→0 is a real condition.
  • Lon(x)=xαFˉon(x)L_{\mathrm{on}}(x)=x^\alpha\bar F_{\mathrm{on}}(x)Lon​(x)=xαFˉon​(x) is assumed slowly varying, which is equivalent to (2.1).
  • Fidi convergence is stated with sorted times: for each kkk there is a probability measure on EuclideanSpace ℝ (Fin k) whose characteristic function is that of c(X(t1),…,X(tk))c(X(t_1),\dots,X(t_k))c(X(t1​),…,X(tk​)), and the laws of the normalised input vectors converge weakly to it. The characteristic function pins the limit down. Its existence is part of the claim, because Mathlib has no stable laws.
  • Convergence in probability means PT(∣YT∣>η)→0P_T(|Y_T|>\eta)\to0PT​(∣YT​∣>η)→0 for every η>0\eta>0η>0.
  • The lemmas that use EA3EA_3EA3​ and EXξT1[⋅]E X_{\xi_T}\mathbf 1[\cdot]EXξT​​1[⋅] also assert integrability, so Bochner junk values cannot trivialise them.

Ruled out. None of the following is acceptable: an encoding in which bbb, NNN or AAA collapses to a junk value; a model hypothesis that no family satisfies (the period laws must be genuine probability laws with finite means, which holds because α>1\alpha>1α>1); a limit "law" not pinned by its characteristic function; or convergence of one-dimensional laws only.

Needed infrastructure.

  • Regular variation: Karamata's theorem and Potter bounds (Proposition 2, App. B).
  • Large deviations for heavy-tailed random walks (Corollary 1, App. A).
  • Renewal theory for delayed alternating renewal processes.
  • Stable laws and the convergence criterion for row-wise iid sums.

The regular-variation and stable-law layers are reusable well beyond this mission. Formalizations of any milestone, of those general tools, or of alternative proofs of the one-dimensional limit are welcome.

Selected references

  • T. Mikosch, S. Resnick, H. Rootzén and A. Stegeman, Is network traffic approximated by stable Lévy motion or fractional Brownian motion?, Ann. Appl. Probab. 12(1):23–68, 2002. https://doi.org/10.1214/aoap/1015961155
  • M. S. Taqqu, W. Willinger and R. Sherman, Proof of a fundamental result in self-similar traffic modeling, Computer Communication Review 27:5–23, 1997. https://doi.org/10.1145/251007.251012
  • W. E. Leland, M. S. Taqqu, W. Willinger and D. V. Wilson, On the self-similar nature of Ethernet traffic (extended version), IEEE/ACM Trans. Networking 2(1):1–15, 1994. https://doi.org/10.1109/90.282603
  • M. E. Crovella and A. Bestavros, Self-similarity in World Wide Web traffic: evidence and possible causes, IEEE/ACM Trans. Networking 5(6):835–846, 1997. https://doi.org/10.1109/90.650143
  • D. B. H. Cline and T. Hsing, Large deviation probabilities for sums of random variables with heavy or subexponential tails, Technical report, Texas A&M University, 1991.
  • G. Samorodnitsky and M. S. Taqqu, Stable Non-Gaussian Random Processes, Chapman and Hall, 1994. https://doi.org/10.1201/9780203738818
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Operations ResearchProbability·Captain: mikedeng1

Is Network Traffic Approximated by Stable Lévy Motion or Fractional Brownian Motion? 3: Infinite Source Poisson Input Under Fast Growth Converges in (D[0,∞), J₁) to Fractional Brownian MotionResearch Paper

Why heavy-tailed input matters

Measurements of Ethernet and Internet traffic in the 1990s showed that cumulative traffic is self-similar and long-range dependent: correlations of the input rate decay so slowly that they are not summable, and fluctuations at large time scales do not average out the way Poisson-type models predict. A widely accepted explanation is that the lengths of individual transmissions (file sizes, session durations) are heavy tailed, with infinite variance. Queueing and capacity-planning calculations then depend on which stochastic process approximates the cumulative input over long horizons.

Two candidate approximations had been proposed: fractional Brownian motion, a Gaussian self-similar process with dependent increments (Taqqu, Willinger and Sherman, 1997; Leland, Taqqu, Willinger and Wilson, 1994), and α-stable Lévy motion, a heavy-tailed process with independent increments. Mikosch, Resnick, Rootzén and Stegeman (Ann. Appl. Probab. 12 (2002) 23–68) showed that both arise from the same model, and that the answer depends on how fast the connection rate grows relative to the time scale. This mission formalizes their Gaussian answer for the infinite source Poisson model: Theorem 3.

  • 1994–1997: Leland et al. measure self-similarity in Ethernet traffic; Willinger, Taqqu, Sherman and Wilson derive fractional Brownian motion from ON/OFF sources with heavy-tailed periods, in an iterated limit (first the number of sources, then time).
  • 2002: Mikosch, Resnick, Rootzén and Stegeman take both limits simultaneously and identify a slow-growth regime (stable Lévy limit) and a fast-growth regime (fractional Brownian limit), for both the ON/OFF and the infinite source Poisson model.

The infinite source Poisson model

Connections start at the points (Γk)k∈Z(\Gamma_k)_{k\in\mathbb Z}(Γk​)k∈Z​ of a homogeneous Poisson process on R\mathbb RR with rate λ\lambdaλ, labelled so that Γ0<0<Γ1\Gamma_0<0<\Gamma_1Γ0​<0<Γ1​; equivalently, −Γ0-\Gamma_0−Γ0​, Γ1\Gamma_1Γ1​ and Γk+1−Γk\Gamma_{k+1}-\Gamma_kΓk+1​−Γk​ (k≠0k\neq0k=0) are iid exponential with parameter λ\lambdaλ. Connection kkk transmits at unit rate for a length XkX_kXk​; the XkX_kXk​ are iid with law FonF_{\mathrm{on}}Fon​ on [0,∞)[0,\infty)[0,∞) and independent of (Γk)(\Gamma_k)(Γk​). The tail Fˉon(x)=P(Xk>x)\bar F_{\mathrm{on}}(x)=P(X_k>x)Fˉon​(x)=P(Xk​>x) is regularly varying:

Fˉon(x)=x−αL(x),x>0,1<α<2,(2.8)\bar F_{\mathrm{on}}(x)=x^{-\alpha}L(x),\qquad x>0,\quad 1<\alpha<2,\tag{2.8}Fˉon​(x)=x−αL(x),x>0,1<α<2,(2.8)

with LLL slowly varying (L(cx)/L(x)→1L(cx)/L(x)\to1L(cx)/L(x)→1 for every c>0c>0c>0). The mean μon\mu_{\mathrm{on}}μon​ is finite and the variance infinite. The number of active connections and the cumulative input are

N(t)=∑k1[Γk≤t<Γk+Xk],A(t)=∫0tN(s) ds.N(t)=\sum_k\mathbf 1[\Gamma_k\le t<\Gamma_k+X_k],\qquad A(t)=\int_0^tN(s)\,ds .N(t)=k∑​1[Γk​≤t<Γk​+Xk​],A(t)=∫0t​N(s)ds.

The model is indexed by a time scale T→∞T\to\inftyT→∞, with a connection rate λ=λ(T)\lambda=\lambda(T)λ=λ(T) that is non-decreasing in TTT. With the quantile function b(t)=(1/Fˉon)←(t)=inf⁡{x>0:1/Fˉon(x)≥t}b(t)=(1/\bar F_{\mathrm{on}})^{\leftarrow}(t)=\inf\{x>0:1/\bar F_{\mathrm{on}}(x)\ge t\}b(t)=(1/Fˉon​)←(t)=inf{x>0:1/Fˉon​(x)≥t}, the fast growth Condition 2 is

lim⁡T→∞b(λT)T=∞,\lim_{T\to\infty}\frac{b(\lambda T)}{T}=\infty ,T→∞lim​Tb(λT)​=∞,

equivalently λTFˉon(T)→∞\lambda T\bar F_{\mathrm{on}}(T)\to\inftyλTFˉon​(T)→∞: many transmissions longer than the observation window start in it. With σT2(1)=λT3Fˉon(T)\sigma_T^2(1)=\lambda T^3\bar F_{\mathrm{on}}(T)σT2​(1)=λT3Fˉon​(T) the normalised input is

GT(t)=A(Tt)−λμonTt[σT2(1) σ2]1/2,t≥0.G_T(t)=\frac{A(Tt)-\lambda\mu_{\mathrm{on}}Tt}{[\sigma_T^2(1)\,\sigma^2]^{1/2}},\qquad t\ge0 .GT​(t)=[σT2​(1)σ2]1/2A(Tt)−λμon​Tt​,t≥0.

Standard fractional Brownian motion BHB_HBH​ with Hurst index H∈(0,1)H\in(0,1)H∈(0,1) is a mean-zero Gaussian process on [0,∞)[0,\infty)[0,∞) with a.s. continuous paths and Cov(BH(t),BH(s))=12(t2H+s2H−∣t−s∣2H)\mathrm{Cov}(B_H(t),B_H(s))=\tfrac12\big(t^{2H}+s^{2H}-|t-s|^{2H}\big)Cov(BH​(t),BH​(s))=21​(t2H+s2H−∣t−s∣2H).

Formalization targets

Goal: Theorem 3 (corrected)

Under (2.8), λ\lambdaλ non-decreasing and Condition 2,

GT(⋅)→dBH(⋅)in (D[0,∞),J1),H=3−α2,σ2=2(α−1)(2−α)(3−α).G_T(\cdot)\xrightarrow{d}B_H(\cdot)\quad\text{in }(\mathbb D[0,\infty),J_1),\qquad H=\frac{3-\alpha}2,\qquad \sigma^2=\frac{2}{(\alpha-1)(2-\alpha)(3-\alpha)} .GT​(⋅)d​BH​(⋅)in (D[0,∞),J1​),H=23−α​,σ2=(α−1)(2−α)(3−α)2​.

On the constant. The paper takes σ2\sigma^2σ2 from its display (6.6), σ2=13−α[α2−α+2μon]\sigma^2=\frac1{3-\alpha}\big[\frac{\alpha}{2-\alpha}+\frac2{\mu_{\mathrm{on}}}\big]σ2=3−α1​[2−αα​+μon​2​]. With that value the theorem is false. Two terms are lost in the variance bookkeeping of the proof: (6.4) omits the factor λm2∼λm3∼λμon\lambda m_2\sim\lambda m_3\sim\lambda\mu_{\mathrm{on}}λm2​∼λm3​∼λμon​ in the variances of the second and third regional sums, each of which contributes 1/(3−α)1/(3-\alpha)1/(3−α), and (6.2) discards (P4−EP4)T(P_4-EP_4)T(P4​−EP4​)T by an argument valid only under slow growth; under Condition 2 its variance is ∼λT3Fˉon(T)/(α−1)\sim\lambda T^3\bar F_{\mathrm{on}}(T)/(\alpha-1)∼λT3Fˉon​(T)/(α−1). The sum α(2−α)(3−α)+23−α+1α−1\frac{\alpha}{(2-\alpha)(3-\alpha)}+\frac2{3-\alpha}+\frac1{\alpha-1}(2−α)(3−α)α​+3−α2​+α−11​ equals 2(α−1)(2−α)(3−α)\frac2{(\alpha-1)(2-\alpha)(3-\alpha)}(α−1)(2−α)(3−α)2​, which is also what VarA(T)=2∫0T(T−h) λ∫h∞Fˉon(v) dv dh\mathrm{Var}A(T)=2\int_0^T(T-h)\,\lambda\int_h^\infty\bar F_{\mathrm{on}}(v)\,dv\,dhVarA(T)=2∫0T​(T−h)λ∫h∞​Fˉon​(v)dvdh and Karamata's theorem give. Since VarBH(1)=1\mathrm{Var}B_H(1)=1VarBH​(1)=1, only this value makes the limit standard. All other constants are those of the paper.

Intermediate targets

The milestones follow the proof: Lemma 1 (Condition 2 ⇔ λTFˉon(T)→∞\lambda T\bar F_{\mathrm{on}}(T)\to\inftyλTFˉon​(T)→∞ ⇔ Cov(NT(0),NT(T))→∞\mathrm{Cov}(N_T(0),N_T(T))\to\inftyCov(NT​(0),NT​(T))→∞), Lemma 2 (fast part), the covariance identity (2.14), the moment asymptotics (4.9) and (4.14), the central limit theorem (6.3) for the first regional sum, the one-dimensional limit (6.5) with the corrected variance, stationarity of the increments of GTG_TGT​, and the fourth-moment bounds (6.8) and E(GT(t+u)−GT(t))4≤cu2E(G_T(t+u)-G_T(t))^4\le cu^2E(GT​(t+u)−GT​(t))4≤cu2 that give tightness.

Significance

The theorem identifies the fast-growth regime of the infinite source Poisson model (the M/G/∞ input model) with fractional Brownian motion, so that Gaussian long-range-dependent models of network traffic are limits of a mechanistic model, not postulates; together with Theorem 1 it shows that the choice between Gaussian and stable approximations is decided by a single growth condition, b(λT)/T→0b(\lambda T)/T\to0b(λT)/T→0 or →∞\to\infty→∞. Queueing analyses of fluid queues fed by fractional Brownian motion inherit their justification from limits of this kind.

The result is proved in the paper, apart from the constant discussed above; it is not formalized anywhere. A formalization adds a machine-checked statement with the correct normalisation and a reusable development of regularly varying tails, Poisson marked point processes on R×[0,∞)\mathbb R\times[0,\infty)R×[0,∞), fractional Brownian motion, and Skorokhod's J1J_1J1​ topology on D[0,∞)\mathbb D[0,\infty)D[0,∞).

Difficulty

The obvious argument is a central limit theorem for A(T)A(T)A(T), but A(T)A(T)A(T) is not a sum of independent terms of bounded variance: transmissions that straddle the window are long and heavy tailed, and their contribution is of the same order as the bulk. The proof splits the points into four regions according to where a transmission starts and ends, and each region needs its own moment asymptotics through Karamata's theorem; the bookkeeping is exactly where the printed constant goes wrong. The functional statement then needs tightness in D[0,∞)\mathbb D[0,\infty)D[0,∞): a fourth-moment bound on increments that is uniform in TTT and in the position of the increment, which requires Potter-type bounds on Fˉon(uT)/Fˉon(T)\bar F_{\mathrm{on}}(uT)/\bar F_{\mathrm{on}}(T)Fˉon​(uT)/Fˉon​(T) for small uuu. Convergence of finite-dimensional distributions alone does not give the theorem.

Formalization scope

  • Time and models. T→∞T\to\inftyT→∞ along atTop on R\mathbb RR. Each model TTT has its own probability space; the theorems hold for every family of models with the stated rate and length law. Time in GTG_TGT​ runs over R≥0\mathbb R_{\ge0}R≥0​.
  • Standing hypotheses. FonF_{\mathrm{on}}Fon​ is a probability measure with Fon((−∞,0))=0F_{\mathrm{on}}((-\infty,0))=0Fon​((−∞,0))=0 (lengths are non-negative, implicit on the page); (2.8) is stated as "x↦xαFˉon(x)x\mapsto x^\alpha\bar F_{\mathrm{on}}(x)x↦xαFˉon​(x) is slowly varying", 1<α<21<\alpha<21<α<2; λ(T)>0\lambda(T)>0λ(T)>0 and λ\lambdaλ is non-decreasing (§3.1); Condition 2. No other hypothesis is added.
  • Junk values ruled out. bbb is an infimum over {x>0:tFˉon(x)≤1}\{x>0:t\bar F_{\mathrm{on}}(x)\le1\}{x>0:tFˉon​(x)≤1}, never a division by zero; NNN is a cardinality and A1A_1A1​ a sum of non-negative terms, whose junk values (000 on an infinite set) occur only on null events; fourth moments are asserted together with integrability; equalities of laws are asserted together with measurability. The limit is pinned completely: Gaussian, mean zero, the covariance above with σH=1\sigma_H=1σH​=1, H=(3−α)/2H=(3-\alpha)/2H=(3−α)/2, continuous paths. Fidi convergence in place of the functional limit, a free scale in the limit, or a limit identified only by its marginals would each be a different, weaker theorem.
  • Weak convergence is stated in coupling form: for every sequence Tn→∞T_n\to\inftyTn​→∞ there is one probability space with copies YnY_nYn​ of the laws of GTnG_{T_n}GTn​​ (all finite-dimensional distributions) and a standard fractional Brownian motion Y′Y'Y′ such that Yn→Y′Y_n\to Y'Yn​→Y′ in J1J_1J1​ almost surely, càdlàg paths included. On the Polish space D[0,∞)\mathbb D[0,\infty)D[0,∞) this is equivalent to weak convergence. Because A(T⋅)A(T\cdot)A(T⋅) and BHB_HBH​ have continuous paths, J1J_1J1​ convergence here coincides with locally uniform convergence.
  • Infrastructure needed: Karamata's theorem and Potter bounds for regularly varying functions; the Poisson random measure of the marked points and its restriction to disjoint regions; a Lyapunov central limit theorem for Poisson sums; fractional Brownian motion and its existence; Billingsley's moment criterion for tightness in D[0,K]\mathbb D[0,K]D[0,K]. The regular-variation and Skorokhod-space material is reusable well beyond this mission; contributions of any of these pieces, and of any milestone, are welcome.

Selected references

  • T. Mikosch, S. Resnick, H. Rootzén and A. Stegeman, Is network traffic approximated by stable Lévy motion or fractional Brownian motion?, Ann. Appl. Probab. 12(1) (2002), 23–68. https://doi.org/10.1214/aoap/1015961155
  • W. E. Leland, M. S. Taqqu, W. Willinger and D. V. Wilson, On the self-similar nature of Ethernet traffic (extended version), IEEE/ACM Trans. Networking 2 (1994), 1–15. https://doi.org/10.1109/90.282603
  • W. Willinger, M. S. Taqqu, R. Sherman and D. V. Wilson, Self-similarity through high-variability: statistical analysis of Ethernet LAN traffic at the source level, IEEE/ACM Trans. Networking 5 (1997), 71–86. https://doi.org/10.1109/90.554723
  • N. H. Bingham, C. M. Goldie and J. L. Teugels, Regular Variation, Cambridge University Press, 1987. https://doi.org/10.1017/CBO9780511721434
  • P. Billingsley, Convergence of Probability Measures, Wiley, 1968 (Theorem 12.3, moment criterion for tightness).
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ProbabilityStatistics·Captain: mikedeng1

Do Price and Volatility Jump Together?: The Observable Jump–Volatility Statistics U(F, kₙ) Converge in Probability to U(F) in the Skorokhod TopologyResearch Paper

Motivation

Asset prices observed at high frequency show two kinds of discontinuity: jumps in the price itself and abrupt changes in its volatility. Whether the two occur at the same times matters for modelling. Many stochastic volatility models used in option pricing let the price and the volatility jump together (for example the affine jump-diffusion models of Duffie, Pan and Singleton, Econometrica 2000), while others make them jump independently or not at all, and the choice affects pricing, hedging and risk management. Jean Jacod and Viktor Todorov (Do price and volatility jump together?, Ann. Appl. Probab. 20 (2010)) built statistical tests of this question that use only discretely observed prices. The tests rest on a law of large numbers, Theorem 3.1 of the paper, and this mission formalizes it.

Setting

The price is an Itô semimartingale XXX on a filtered probability space (Ω,F,(Ft)t≥0,P)(\Omega,\mathcal F,(\mathcal F_t)_{t\ge0},\mathbb P)(Ω,F,(Ft​)t≥0​,P):

Xt=X0+∫0tbs ds+∫0tσs dWs+∫0t ⁣ ⁣∫Eδ(s,z)1{∣δ(s,z)∣≤1}(μ−ν)(ds,dz)+∫0t ⁣ ⁣∫Eδ(s,z)1{∣δ(s,z)∣>1}μ(ds,dz),X_t=X_0+\int_0^t b_s\,ds+\int_0^t\sigma_s\,dW_s+\int_0^t\!\!\int_E\delta(s,z)1_{\{|\delta(s,z)|\le1\}}(\mu-\nu)(ds,dz)+\int_0^t\!\!\int_E\delta(s,z)1_{\{|\delta(s,z)|>1\}}\mu(ds,dz),Xt​=X0​+∫0t​bs​ds+∫0t​σs​dWs​+∫0t​∫E​δ(s,z)1{∣δ(s,z)∣≤1}​(μ−ν)(ds,dz)+∫0t​∫E​δ(s,z)1{∣δ(s,z)∣>1}​μ(ds,dz),

where WWW is a Brownian motion, μ\muμ is a Poisson random measure on R+×E\mathbb R_+\times ER+​×E with compensator ν(ds,dz)=ds⊗λ(dz)\nu(ds,dz)=ds\otimes\lambda(dz)ν(ds,dz)=ds⊗λ(dz), and δ(ω,s,z)\delta(\omega,s,z)δ(ω,s,z) is the jump size produced by an atom (s,z)(s,z)(s,z) of μ\muμ. The volatility is ct=σt2c_t=\sigma_t^2ct​=σt2​, and ΔXs=Xs−Xs−\Delta X_s=X_s-X_{s-}ΔXs​=Xs​−Xs−​ is the jump of XXX at time sss.

Two assumptions are imposed. (H-rrr), 0≤r<20\le r<20≤r<2: the drift bbb is locally bounded, σ\sigmaσ is càdlàg with σt≠0\sigma_t\ne0σt​=0 and σt−≠0\sigma_{t-}\ne0σt−​=0, and ∣δ(ω,t,z)∣≤Γt(ω)γ(z)|\delta(\omega,t,z)|\le\Gamma_t(\omega)\gamma(z)∣δ(ω,t,z)∣≤Γt​(ω)γ(z) with Γ\GammaΓ locally bounded and ∫E(γr∧1) dλ<∞\int_E(\gamma^r\wedge1)\,d\lambda<\infty∫E​(γr∧1)dλ<∞; smaller rrr means fewer small jumps, and r=0r=0r=0 means finitely many jumps on bounded intervals. (K-vvv), 0<v≤10<v\le10<v≤1: σt=Σ(Zt,Z‾t)\sigma_t=\Sigma(Z_t,\overline Z_t)σt​=Σ(Zt​,Zt​) for a C1C^1C1 function Σ\SigmaΣ, where ZZZ is itself an Itô semimartingale with controlled jumps and Z‾\overline ZZ is Hölder of order vvv in the sense ∣Z‾t+s−Z‾t∣≤Γt+s′sv|\overline Z_{t+s}-\overline Z_t|\le\Gamma'_{t+s}s^v∣Zt+s​−Zt​∣≤Γt+s′​sv for 0<s≤10<s\le10<s≤1.

For a test function F(x,y,z)F(x,y,z)F(x,y,z), the unobservable target is the jump functional

U(F)t=∑s≤tF(ΔXs,cs−,cs) 1{ΔXs≠0},U(F)_t=\sum_{s\le t}F(\Delta X_s,c_{s-},c_s)\,1_{\{\Delta X_s\ne0\}},U(F)t​=s≤t∑​F(ΔXs​,cs−​,cs​)1{ΔXs​=0}​,

which compares, at each price jump, the volatility just before and just after it. The data are the values XiΔnX_{i\Delta_n}XiΔn​​ on a grid of mesh Δn→0\Delta_n\to0Δn​→0, with increments ΔinX=XiΔn−X(i−1)Δn\Delta^n_iX=X_{i\Delta_n}-X_{(i-1)\Delta_n}Δin​X=XiΔn​​−X(i−1)Δn​​. With a truncation level unu_nun​ and a window size knk_nkn​, the local volatility estimator is

c^(kn)i=1knΔn∑j=1kn∣Δi+jnX∣2 1{∣Δi+jnX∣≤un},\widehat c(k_n)_i=\frac1{k_n\Delta_n}\sum_{j=1}^{k_n}|\Delta^n_{i+j}X|^2\,1_{\{|\Delta^n_{i+j}X|\le u_n\}},c(kn​)i​=kn​Δn​1​j=1∑kn​​∣Δi+jn​X∣21{∣Δi+jn​X∣≤un​}​,

and the observable statistic is

U(F,kn)t=∑i=kn+1[t/Δn]−knF(ΔinX,c^(kn)i−kn−1,c^(kn)i) 1{∣ΔinX∣>un}.U(F,k_n)_t=\sum_{i=k_n+1}^{[t/\Delta_n]-k_n}F\big(\Delta^n_iX,\widehat c(k_n)_{i-k_n-1},\widehat c(k_n)_i\big)\,1_{\{|\Delta^n_iX|>u_n\}}.U(F,kn​)t​=i=kn​+1∑[t/Δn​]−kn​​F(Δin​X,c(kn​)i−kn​−1​,c(kn​)i​)1{∣Δin​X∣>un​}​.

The tuning (3.3) is un≍Δnϖu_n\asymp\Delta_n^{\varpi}un​≍Δnϖ​ and kn≍Δn−ρk_n\asymp\Delta_n^{-\rho}kn​≍Δn−ρ​ with 0<ϖ<120<\varpi<\tfrac120<ϖ<21​ and 0<ρ<10<\rho<10<ρ<1. Finally, R\mathcal RR is the family of open sets R⊆RR\subseteq\mathbb RR⊆R with finite complement that contain every value xxx with P(∃s>0:ΔXs=x)>0\mathbb P(\exists s>0:\Delta X_s=x)>0P(∃s>0:ΔXs​=x)>0.

Formalization targets

Goal: Theorem 3.1

Let FFF be Borel, continuous at each point of R×(0,∞)2R\times(0,\infty)^2R×(0,∞)2 for some R∈RR\in\mathcal RR∈R, and assume one of (a) F(x,y,z)=0F(x,y,z)=0F(x,y,z)=0 for ∣x∣≤ε|x|\le\varepsilon∣x∣≤ε; (b) r=0r=0r=0; (c) ∣F(x,y,z)∣≤K∣x∣r(1+y+z)|F(x,y,z)|\le K|x|^r(1+y+z)∣F(x,y,z)∣≤K∣x∣r(1+y+z) for ∣x∣≤ε|x|\le\varepsilon∣x∣≤ε. Then U(F)U(F)U(F) is a.s. well defined and

U(F,kn)→ P U(F)for the Skorokhod topology.U(F,k_n)\xrightarrow{\ \mathbb P\ }U(F)\qquad\text{for the Skorokhod topology}.U(F,kn​) P ​U(F)for the Skorokhod topology.

Milestones

They follow the proof of §8, in which the coefficients are bounded by a constant (the localized bound (8.3)):

  • (8.4): with probability tending to one, the big jumps up to time ttt lie in distinct sampling windows;
  • (8.11) and (8.14): E(∣ΔinX∣2∣F(i−1)Δn)≤KΔn\mathbb E(|\Delta^n_iX|^2\mid\mathcal F_{(i-1)\Delta_n})\le K\Delta_nE(∣Δin​X∣2∣F(i−1)Δn​​)≤KΔn​ and E(c^(kn)i∣FiΔn)≤K\mathbb E(\widehat c(k_n)_i\mid\mathcal F_{i\Delta_n})\le KE(c(kn​)i​∣FiΔn​​)≤K, with KKK uniform;
  • Lemma 8.1, (8.18): c^(kn)i→cS\widehat c(k_n)_i\to c_Sc(kn​)i​→cS​ and c^(kn)i−kn−1→cS−\widehat c(k_n)_{i-k_n-1}\to c_{S-}c(kn​)i−kn​−1​→cS−​ in probability on the events where no big jump falls in the corresponding window;
  • (8.27): the part of U(F,kn)U(F,k_n)U(F,kn​) carried by the big jumps converges to the corresponding part of U(F)U(F)U(F);
  • (8.29): the remainder driven by the small jumps vanishes in mean, uniformly in nnn, as the jump threshold goes to zero;
  • Theorem 3.1 under the localized bound (8.3), which §8.4 proves directly.

Significance

Theorem 3.1 makes U(F,kn)TU(F,k_n)_TU(F,kn​)T​ a consistent estimator of U(F)TU(F)_TU(F)T​. Choosing FFF nonnegative with F(x,y,y)=0F(x,y,y)=0F(x,y,y)=0 makes U(F)T>0U(F)_T>0U(F)T​>0 exactly when XXX and ccc jump together on [0,T][0,T][0,T], and the tests of §4 of the paper (Theorems 4.1–4.5), together with the central limit theorems 3.2 and 3.3, are built on this. The same truncated local volatility estimators appear throughout high-frequency econometrics, so their consistency (Lemma 8.1) is reusable on its own.

The result is proved in the paper. No machine-checked proof of it, or of any of its steps, is known to exist. A formal development would also produce a reusable layer for Itô semimartingales with Poisson jumps: the representation (2.1), compensated jump integrals, and convergence in probability in the Skorokhod space. None of these is currently available in Mathlib.

Difficulty

The obvious argument treats each increment ΔinX\Delta^n_iXΔin​X and replaces the estimators c^(kn)i\widehat c(k_n)_ic(kn​)i​ by c(i−1)Δnc_{(i-1)\Delta_n}c(i−1)Δn​​. This fails in two places. First, U(F,kn)U(F,k_n)U(F,kn​) has about t/Δnt/\Delta_nt/Δn​ summands, so errors of each summand that vanish in probability need not sum to something small. The infinitely many small jumps must be controlled in mean, through the moment bounds of §8.2 and the growth condition of case (c), and the cutoff unu_nun​ must separate jumps from Brownian increments. Second, the estimators look at windows of knk_nkn​ increments that may contain a jump of XXX or of ccc. Consistency holds only away from the big jumps, and the jump times are random, so conditioning has to be done with respect to the enlarged filtrations Ft(m)\mathcal F^{(m)}_tFt(m)​ that know the big jumps in advance. Finally, the limit is in the Skorokhod topology: the jumps of U(F,kn)U(F,k_n)U(F,kn​) occur at grid times close to, but not equal to, those of U(F)U(F)U(F), so uniform convergence fails.

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​ and processes are functions ℝ≥0 → Ω → ℝ. The Poisson random measure is given by its atoms N(ω)⊆R+×EN(\omega)\subseteq\mathbb R_+\times EN(ω)⊆R+​×E, with at most one atom at each time. The Brownian integrals use the published EthierKurtz.HasBrownianItoIntegral. The compensated jump integral is characterized by the Lévy–Itô limit of compensated truncated sums. Càdlàg paths and Skorokhod convergence are the published KurtzProtter91.Integrals definitions. Convergence in probability for the Skorokhod topology is the subsequence criterion: every subsequence has a further subsequence converging almost surely. The identity (2.1) and the path properties hold almost surely, for each ttt.

The conventions are the following.

  • Following §8.1, ZZZ is written with the same Poisson measure as XXX and a second Brownian motion W′W'W′ independent of WWW.
  • Clause (b) of (H-·) is not imposed on ZZZ.
  • γ0\gamma^0γ0 means 1{γ>0}1_{\{\gamma>0\}}1{γ>0}​.
  • Increments have integer indices, with ΔinX=0\Delta^n_iX=0Δin​X=0 for i≤0i\le0i≤0.
  • A0=EA_0=EA0​=E.
  • Δn→0\Delta_n\to0Δn​→0 is added to (3.3), as the paper's standing regime.
  • The localized bound (8.3) omits the term ∣Xt∣|X_t|∣Xt​∣: together with the other bounds it cannot hold for all ttt, and keeping it would make the §8 statements vacuous.

The conclusion of Theorem 3.1 includes the a.s. summability of U(F)tU(F)_tU(F)t​. A formalization in which the infinite sum takes a default value, the expectations are junk values of non-integrable variables, or the hypotheses cannot be met is ruled out: X=WX=WX=W with σ≡1\sigma\equiv1σ≡1 and no jumps satisfies every hypothesis with r=0r=0r=0 and v=1v=1v=1.

A complete development needs stochastic integration against Brownian motion and compensated Poisson measures, Burkholder-type moment bounds, and the Skorokhod topology on D[0,∞)D[0,\infty)D[0,∞). These are reusable well beyond this mission. Contributions to any of them, and proofs of individual milestones, are welcome.

Selected references

  • J. Jacod, V. Todorov, Do price and volatility jump together?, Ann. Appl. Probab. 20(4) (2010) 1425–1469. arXiv:1010.4990, doi:10.1214/09-AAP654
  • J. Jacod, A. N. Shiryaev, Limit Theorems for Stochastic Processes, 2nd ed., Springer, 2003. doi:10.1007/978-3-662-05265-5
  • D. Duffie, J. Pan, K. Singleton, Transform analysis and asset pricing for affine jump-diffusions, Econometrica 68 (2000) 1343–1376. doi:10.1111/1468-0262.00164
  • T. G. Kurtz, P. Protter, Weak limit theorems for stochastic integrals and stochastic differential equations, Ann. Probab. 19 (1991) 1035–1070. doi:10.1214/aop/1176990334
14 thms1 active userReviewed
Control TheoryOperations ResearchProbability·Captain: mikedeng1

On Minimizing the Ruin Probability by Investment and Reinsurance I: An Increasing Solution f of the HJB Equation Is Bounded, δ(u) = f(u)/f(∞), and the Feedback Strategy A*, b* Is OptimalResearch Paper

Motivation

An insurance company that collects premiums and pays random claims is ruined when its surplus becomes negative. The probability of ultimate ruin is the classical solvency criterion of risk theory, going back to Lundberg and Cramér. Real insurers have two levers on this probability: they can invest part of the surplus in a risky asset, and they can cede part of every claim to a reinsurer, at a price. The question of how to use both levers dynamically, as a function of the current surplus, so as to make the probability of ruin as small as possible, is a stochastic control problem for a jump-diffusion.

H. Schmidli, On minimizing the ruin probability by investment and reinsurance, Ann. Appl. Probab. 12 (2002), solves this problem for the Cramér–Lundberg model with proportional reinsurance and investment in a Black–Scholes asset. The main results are a verification theorem (Theorem 1, the subject of this mission) and an existence theorem for the associated integral equation (Theorem 2, the companion mission).

Timeline. Hipp and Plum (2000) treated investment in the Cramér–Lundberg model through the Hamilton–Jacobi–Bellman equation, assuming a bounded solution. Schmidli (2001) treated optimal proportional reinsurance alone. The 2002 paper combines investment and reinsurance, and proves the verification theorem without assuming the solution to be bounded.

Setting

Claims arrive at the jumps T1<T2<…T_1<T_2<\dotsT1​<T2​<… of a Poisson process NNN with rate λ>0\lambda>0λ>0; the claim sizes Y1,Y2,…Y_1,Y_2,\dotsY1​,Y2​,… are i.i.d. with continuous distribution function GGG, G(0)=0G(0)=0G(0)=0, independent of NNN. The insurer receives premiums at rate c>0c>0c>0. A risky asset Zt=exp⁡{σWt+(μ−12σ2)t}Z_t=\exp\{\sigma W_t+(\mu-\frac12\sigma^2)t\}Zt​=exp{σWt​+(μ−21​σ2)t}, with μ,σ>0\mu,\sigma>0μ,σ>0 and WWW a standard Brownian motion independent of the claims, is available.

A strategy is a pair of processes (At,bt)(A_t,b_t)(At​,bt​), predictable for the smallest right-continuous filtration generated by the claims and WWW: At∈RA_t\in\mathbb RAt​∈R is the amount invested in the risky asset (locally bounded), and bt∈[0,1]b_t\in[0,1]bt​∈[0,1] is the retention level, meaning the insurer pays btYb_tYbt​Y of a claim YYY occurring at time ttt, at a reinsurance premium rate c(bt)c(b_t)c(bt​). The surplus X=XAbX=X^{Ab}X=XAb starting from u≥0u\ge0u≥0 solves

dXt=(c−c(bt)+μAt) dt+σAt dWt−bt dSt,X0=u,dX_t=\big(c-c(b_t)+\mu A_t\big)\,dt+\sigma A_t\,dW_t-b_t\,dS_t,\qquad X_0=u,dXt​=(c−c(bt​)+μAt​)dt+σAt​dWt​−bt​dSt​,X0​=u,

where St=∑i≤NtYiS_t=\sum_{i\le N_t}Y_iSt​=∑i≤Nt​​Yi​ is the aggregate claims process. The ruin time is τ=inf⁡{t≥0:Xt<0}\tau=\inf\{t\ge0:X_t<0\}τ=inf{t≥0:Xt​<0}, the survival probability is δAb(u)=P[τ=∞]\delta^{Ab}(u)=\mathbb P[\tau=\infty]δAb(u)=P[τ=∞], and the value function is δ(u)=sup⁡A,bδAb(u)\delta(u)=\sup_{A,b}\delta^{Ab}(u)δ(u)=supA,b​δAb(u).

The premium function c(b)c(b)c(b) is decreasing and continuous on [0,1][0,1][0,1], c(1)=0c(1)=0c(1)=0, lim inf⁡b↑1c(b)/(1−b)>0\liminf_{b\uparrow1}c(b)/(1-b)>0liminfb↑1​c(b)/(1−b)>0, and there is b‾>0\underline b>0b​>0 with c(b)>cc(b)>cc(b)>c for b<b‾b<\underline bb<b​ and c(b)≤cc(b)\le cc(b)≤c for b≥b‾b\ge\underline bb≥b​ (full reinsurance is too expensive).

The Hamilton–Jacobi–Bellman equation for δ\deltaδ is, with the convention f(u)=0f(u)=0f(u)=0 for u<0u<0u<0,

sup⁡b∈[0,1]sup⁡A≥0[12σ2A2f′′(u)+(c−c(b)+μA)f′(u)+λ(E[f(u−bY)]−f(u))]=0.(1)\sup_{b\in[0,1]}\sup_{A\ge0}\Big[\tfrac12\sigma^2A^2f''(u)+\big(c-c(b)+\mu A\big)f'(u)+\lambda\big(\mathbb E[f(u-bY)]-f(u)\big)\Big]=0.\tag{1}b∈[0,1]sup​A≥0sup​[21​σ2A2f′′(u)+(c−c(b)+μA)f′(u)+λ(E[f(u−bY)]−f(u))]=0.(1)

For strictly concave fff the maximum over AAA is attained at A∗(u)=−μf′(u)/(σ2f′′(u))A^*(u)=-\mu f'(u)/(\sigma^2f''(u))A∗(u)=−μf′(u)/(σ2f′′(u)) (equation (2)); b∗(u)b^*(u)b∗(u) denotes a measurable maximiser in bbb.

Formalization targets

Goal: Theorem 1 (p. 896)

Let fff be strictly increasing and nonnegative on [0,∞)[0,\infty)[0,∞), continuous there, twice continuously differentiable on (0,∞)(0,\infty)(0,∞), zero on (−∞,0)(-\infty,0)(−∞,0), and a solution of (1) at every u>0u>0u>0. Then fff is bounded, f(∞)=lim⁡x→∞f(x)∈(0,∞)f(\infty)=\lim_{x\to\infty}f(x)\in(0,\infty)f(∞)=limx→∞​f(x)∈(0,∞),

δ(u)=f(u)f(∞)(u≥0),\delta(u)=\frac{f(u)}{f(\infty)}\qquad(u\ge0),δ(u)=f(∞)f(u)​(u≥0),

and every surplus process from u>0u>0u>0 following At=A∗(Xt−)A_t=A^*(X_{t-})At​=A∗(Xt−​), bt=b∗(Xt−)b_t=b^*(X_{t-})bt​=b∗(Xt−​) has survival probability δ(u)\delta(u)δ(u).

Milestones

The proof of Theorem 1 runs through: Lemma 3 (for small surplus the optimal retention is b∗=1b^*=1b∗=1); the identity E[f(Xτ∗∧t∗)]=f(u)\mathbb E[f(X^*_{\tau^*\wedge t})]=f(u)E[f(Xτ∗∧t∗​)]=f(u) along the feedback strategy; the inequality E[f(Xt∧τ)]≤f(u)\mathbb E[f(X_{t\wedge\tau})]\le f(u)E[f(Xt∧τ​)]≤f(u) for every strategy; Lemma 1 (almost surely, either ruin occurs or Xt→∞X_t\to\inftyXt​→∞); the existence of a strategy with P[τ=∞]>0\mathbb P[\tau=\infty]>0P[τ=∞]>0; the comparison δAb(u)≤f(u)/f(∞)\delta^{Ab}(u)\le f(u)/f(\infty)δAb(u)≤f(u)/f(∞) with equality for the feedback strategy; and the absence of ruin by creeping, P[τ∗<∞,Xτ∗∗=0]=0\mathbb P[\tau^*<\infty,X^*_{\tau^*}=0]=0P[τ∗<∞,Xτ∗∗​=0]=0.

Companion statements

The second sentence of Theorem 1 (that f(x)=1+∫0xg(z) dzf(x)=1+\int_0^xg(z)\,dzf(x)=1+∫0x​g(z)dz satisfies the hypotheses whenever ggg is a decreasing solution of the integral equation (5)) and its last sentence (at most one such solution of (1) with f(0)=1f(0)=1f(0)=1) are separate items.

Significance

Theorem 1 reduces a control problem over all predictable strategies to an analytic question: find one increasing smooth solution of (1). Combined with Theorem 2 (existence of a solution of (5)), it shows that the optimal survival probability is f(u)/f(∞)f(u)/f(\infty)f(u)/f(∞) and that the optimal strategy is a Markov feedback rule in the current surplus. It also yields that this solution is bounded, which Hipp and Plum (2000) had to assume, and closes the gap they left open on ruin by creeping (Remark (iii), p. 897). Numerical procedures for the optimal strategy (§5 of the paper) rest on this identification.

The theorem is proved in the paper; nothing in it is formalized. The mission produces a machine-checked verification theorem for a controlled jump-diffusion with an Itô integral against Brownian motion, a Poisson claim stream and a predictable control, together with a formal model of the Cramér–Lundberg process with investment and reinsurance that later results in risk theory can reuse.

Difficulty

The standard verification argument applies Itô's formula to f(Xt)f(X_t)f(Xt​) and uses (1) to show that f(Xt∧τ)f(X_{t\wedge\tau})f(Xt∧τ​) is a supermartingale, and a martingale under the feedback strategy. Here fff is not C2C^2C2 at 000 (f′′(0+)=−∞f''(0+)=-\inftyf′′(0+)=−∞), is discontinuous at 000 after the extension by 000, and is not assumed bounded, so the stochastic integral is only a local martingale and the passage t→∞t\to\inftyt→∞ needs both Lemma 1 and a separate argument that the feedback process does not creep through 000. Lemma 1 itself is only sketched in the paper ("We will just describe the argument"). The optimality part needs a surplus process following the feedback rule; its existence is not proved in the paper.

Formalization scope

The model is formalized on a measurable space with a probability measure: i.i.d. exponential interarrival times (realising the Poisson process), i.i.d. claim sizes with law ν\nuν, and a real Brownian motion (IsBrownianReal), the three families mutually independent. Independence of WWW from the claims is not printed in the paper but is used by (1) and its proof; it is a disclosed standing assumption. The filtration is Ft=⋂s>tσ(Sr,Wr:r≤s)\mathcal F_t=\bigcap_{s>t}\sigma(S_r,W_r:r\le s)Ft​=⋂s>t​σ(Sr​,Wr​:r≤s), not completed. The Itô integral is the published relation EthierKurtz.HasBrownianItoIntegral, and its paths are required to be continuous, so that the pathwise ruin event is well defined. The surplus equation holds for every ttt and every sample point.

Conventions: the premium c(b)c(b)c(b) is real valued (so c(0)<∞c(0)<\inftyc(0)<∞, which the paper allows to fail when E[Y]<∞\mathbb E[Y]<\inftyE[Y]<∞); the supremum in (1) is stated as a least upper bound equal to 000, so an unbounded family never counts as a solution; fff is C2C^2C2 on (0,∞)(0,\infty)(0,∞) and (1) is required for u>0u>0u>0; δ\deltaδ is a supremum over all admissible triples (strategy and surplus process); the controls of the feedback rule at non-positive pre-jump surplus are left free, and optimality is stated for u>0u>0u>0. Expectations of f(Xt∧τ)f(X_{t\wedge\tau})f(Xt∧τ​) are lower Lebesgue integrals of nonnegative functions, so no default value of a non-integrable expectation satisfies an inequality. The optimality clause is stated for every process following the feedback rule; it would be vacuous if no such process existed, and its existence is not part of the target.

Infrastructure needed: Itô's formula for a semimartingale with Brownian and compound-Poisson parts, the compensator of the compound Poisson random measure, localisation, and optional stopping. The model definitions, the HJB predicate and the comparison lemmas are reusable for other ruin-minimisation and dividend problems. Contributions to any milestone, and to general stochastic-calculus lemmas they need, are welcome.

Selected references

  • H. Schmidli, On minimizing the ruin probability by investment and reinsurance, Ann. Appl. Probab. 12(3) (2002), 890–907. https://doi.org/10.1214/aoap/1031863173
  • C. Hipp, M. Plum, Optimal investment for insurers, Insurance Math. Econom. 27 (2000), 215–228. https://doi.org/10.1016/S0167-6687(00)00049-4
  • H. Schmidli, Optimal proportional reinsurance policies in a dynamic setting, Scand. Actuar. J. (2001), 55–68. https://doi.org/10.1080/034612301750077338
  • P. Brémaud, Point Processes and Queues: Martingale Dynamics, Springer (1981). https://doi.org/10.1007/978-1-4684-9477-8
11 thms1 active userReviewed
Operations ResearchProbability·Captain: mikedeng1

Is Network Traffic Approximated by Stable Lévy Motion or Fractional Brownian Motion? 1: Infinite Source Poisson Input Under Slow Growth Converges (fidi) to Totally Skewed α-Stable Lévy MotionResearch Paper

Motivation

Measurements of Ethernet and Internet traffic in the 1990s showed that the amount of data offered to a link is bursty on every time scale and that the lengths of transmissions (file sizes, connection durations) have heavy, regularly varying tails. Two families of approximations for the cumulative input were proposed: fractional Brownian motion, which has dependent Gaussian increments, and α-stable Lévy motion, which has independent, heavy-tailed increments. The two lead to very different predictions for buffer overflow and link dimensioning.

T. Mikosch, S. Resnick, H. Rootzén and A. Stegeman (Ann. Appl. Probab. 12 (2002) 23–68) showed that both answers are correct in different regimes, and that the regime is decided by how fast the connection rate grows relative to the time scale. This mission formalizes their result for the infinite source Poisson model under slow growth, where the limit is a totally skewed α-stable Lévy motion. Companion missions treat the ON/OFF model and the fast-growth regime with its fractional Brownian limit.

Setting

A transmission length has law FonF_{\mathrm{on}}Fon​ on [0,∞)[0,\infty)[0,∞) with tail Fˉon(x)=Fon((x,∞))\bar F_{\mathrm{on}}(x)=F_{\mathrm{on}}((x,\infty))Fˉon​(x)=Fon​((x,∞)). Condition (2.8) asks

Fˉon(x)=x−αL(x),x>0,1<α<2,\bar F_{\mathrm{on}}(x)=x^{-\alpha}L(x),\qquad x>0,\quad 1<\alpha<2,Fˉon​(x)=x−αL(x),x>0,1<α<2,

with LLL slowly varying (L(cx)/L(x)→1L(cx)/L(x)\to1L(cx)/L(x)→1 for every c>0c>0c>0). The mean μon\mu_{\mathrm{on}}μon​ is finite and the variance infinite. The quantile function (2.9) is b(t)=(1/Fˉon)←(t)=inf⁡{x:1/Fˉon(x)≥t}b(t)=(1/\bar F_{\mathrm{on}})^{\leftarrow}(t)=\inf\{x:1/\bar F_{\mathrm{on}}(x)\ge t\}b(t)=(1/Fˉon​)←(t)=inf{x:1/Fˉon​(x)≥t}.

In the TTT-th model, connections start at the points (Γk)k∈Z(\Gamma_k)_{k\in\mathbb Z}(Γk​)k∈Z​ of a homogeneous Poisson process on R\mathbb RR with rate λ=λ(T)\lambda=\lambda(T)λ=λ(T), labelled so that Γ0<0<Γ1\Gamma_0<0<\Gamma_1Γ0​<0<Γ1​. Connection kkk transmits at unit rate for a time XkX_kXk​; the XkX_kXk​ are iid with law FonF_{\mathrm{on}}Fon​ and independent of the Γk\Gamma_kΓk​. The number of active connections and the cumulative input are

N(t)=∑k∈Z1[Γk≤t<Γk+Xk],A(t)=∫0tN(s) ds.N(t)=\sum_{k\in\mathbb Z}\mathbf 1[\Gamma_k\le t<\Gamma_k+X_k],\qquad A(t)=\int_0^tN(s)\,ds .N(t)=k∈Z∑​1[Γk​≤t<Γk​+Xk​],A(t)=∫0t​N(s)ds.

The rate λ(T)\lambda(T)λ(T) is a positive non-decreasing function of TTT. Slow Growth Condition 1 is

lim⁡T→∞b(λT)T=0,\lim_{T\to\infty}\frac{b(\lambda T)}{T}=0,T→∞lim​Tb(λT)​=0,

where b(λT)b(\lambda T)b(λT) is bbb evaluated at λ(T) T\lambda(T)\,Tλ(T)T.

The stable law Sα(σ,β,μ)S_\alpha(\sigma,\beta,\mu)Sα​(σ,β,μ) is the law with characteristic function exp⁡{−σα∣θ∣α(1−iβ sign(θ)tan⁡(πα/2))+iμθ}\exp\{-\sigma^\alpha|\theta|^\alpha(1-i\beta\,\mathrm{sign}(\theta)\tan(\pi\alpha/2))+i\mu\theta\}exp{−σα∣θ∣α(1−iβsign(θ)tan(πα/2))+iμθ} for α≠1\alpha\ne1α=1. α-stable Lévy motion Xα,σ,βX_{\alpha,\sigma,\beta}Xα,σ,β​ has independent stationary increments with X(t)−X(s)∼Sα(σ(t−s)1/α,β,0)X(t)-X(s)\sim S_\alpha(\sigma(t-s)^{1/\alpha},\beta,0)X(t)−X(s)∼Sα​(σ(t−s)1/α,β,0). Write

Cα=1−αΓ(2−α)cos⁡(πα/2)(5.1).C_\alpha=\frac{1-\alpha}{\Gamma(2-\alpha)\cos(\pi\alpha/2)}\quad(5.1).Cα​=Γ(2−α)cos(πα/2)1−α​(5.1).

Formalization targets

Goal: Theorem 1 (corrected scale)

Under (2.8) and Condition 1,

A(T⋅)−Tλμon(⋅)b(λT)→ fidi Xα,Cα−1/α,1(⋅),\frac{A(T\cdot)-T\lambda\mu_{\mathrm{on}}(\cdot)}{b(\lambda T)}\xrightarrow{\ fidi\ }X_{\alpha,C_\alpha^{-1/\alpha},1}(\cdot),b(λT)A(T⋅)−Tλμon​(⋅)​ fidi ​Xα,Cα−1/α​,1​(⋅),

convergence of the finite-dimensional distributions to a totally skewed (β=1\beta=1β=1) α-stable Lévy motion.

On the scale. The paper prints the limit Xα,1,1X_{\alpha,1,1}Xα,1,1​. Its own proof establishes λT P(j1>b(λT)x)→x−α\lambda T\,P(j_1>b(\lambda T)x)\to x^{-\alpha}λTP(j1​>b(λT)x)→x−α (pp. 37–38), which makes αx−α−1dx\alpha x^{-\alpha-1}dxαx−α−1dx the Lévy measure of the limit. The totally skewed stable law with that Lévy measure has σα=Γ(1−α)cos⁡(πα/2)=Cα−1\sigma^\alpha=\Gamma(1-\alpha)\cos(\pi\alpha/2)=C_\alpha^{-1}σα=Γ(1−α)cos(πα/2)=Cα−1​ (Samorodnitsky–Taqqu, Property 1.2.15; also the paper's own criterion on p. 47 with c=1c=1c=1, and the σ\sigmaσ the paper prints in Theorem 2). Since CαC_\alphaCα​ decreases from 2/π2/\pi2/π to 000 on (1,2)(1,2)(1,2) (C1.5≈0.399C_{1.5}\approx0.399C1.5​≈0.399), the printed limit has the wrong scale and the theorem as printed is false. The goal states the corrected scale Cα−1/αC_\alpha^{-1/\alpha}Cα−1/α​; milestones quote the page as printed.

Milestones, in attack order

(2.14), the covariance of NNN; Lemma 1 part 1 (Condition 1   ⟺  λTFˉon(T)→0  ⟺  Cov(NT(0),NT(T))→0\iff\lambda T\bar F_{\mathrm{on}}(T)\to0\iff\mathrm{Cov}(N_T(0),N_T(T))\to0⟺λTFˉon​(T)→0⟺Cov(NT​(0),NT​(T))→0); Lemma 2, slow part (λT2Fˉon(T)/b(λT)→0\lambda T^2\bar F_{\mathrm{on}}(T)/b(\lambda T)\to0λT2Fˉon​(T)/b(λT)→0); (4.15), negligibility of the boundary pieces A2,A3,A4A_2,A_3,A_4A2​,A3​,A4​; the tail limit of j1j_1j1​; (4.17), A12=OP([λT]1/2)=oP(b(λT))A_{12}=O_P([\lambda T]^{1/2})=o_P(b(\lambda T))A12​=OP​([λT]1/2)=oP​(b(λT)); (4.20)–(4.21), A13=o(b(λT))A_{13}=o(b(\lambda T))A13​=o(b(λT)); (4.19), corrected, the stable limit of A11A_{11}A11​; the corrected one-dimensional limit of A(T)A(T)A(T); and EA22=o(b(λT))EA_{22}=o(b(\lambda T))EA22​=o(b(λT)) of §4.5, which reduces the fidi convergence to the one-dimensional one.

Significance

The theorem shows that under slow connection growth the cumulative input is asymptotically a process with independent, infinite-variance increments. Long-range dependence present in each model (the covariance (2.14) decays like h−(α−1)L(h)h^{-(\alpha-1)}L(h)h−(α−1)L(h)) disappears on the time scale TTT, and the heavy tail of the transmission lengths dominates. Together with the fast-growth result (fractional Brownian motion) it explains why both approximations are found in measured traffic, and it identifies the critical quantity b(λT)/Tb(\lambda T)/Tb(λT)/T.

The result is proved in the paper, modulo the scale. No part of it is machine-checked. The mission produces a formal statement of the infinite source Poisson model with its marked point process structure, a formal statement of stable laws and stable Lévy motion through their characteristic functions, and machine-checked versions of the paper's estimates. Correcting the printed scale is part of the output.

Difficulty

The pieces A2,A3,A4,A12,A13,A22A_2,A_3,A_4,A_{12},A_{13},A_{22}A2​,A3​,A4​,A12​,A13​,A22​ are controlled by first moments, regular variation and Lemma 2. The central step is the stable limit of A11A_{11}A11​: a sum of a Poisson number of iid, heavy-tailed summands whose law changes with TTT. A classical central limit theorem does not apply because the variance is infinite, and the summands form a triangular array. The paper cites a point-process limit (Resnick's Exercise 4.4.2.8) for this step; a formal proof needs a convergence theorem for row-wise iid triangular arrays to stable laws, with the constant CαC_\alphaCα​ computed exactly.

Formalization scope

Each TTT has its own probability space carrying the TTT-th model, and every statement quantifies over all such families. The Poisson points are given by their iid exponential spacings −Γ0,Γ1,Γk+1−Γk-\Gamma_0,\Gamma_1,\Gamma_{k+1}-\Gamma_k−Γ0​,Γ1​,Γk+1​−Γk​ (k≠0)(k\ne0)(k=0), indexed by Z\mathbb ZZ. (2.8) is stated as "x↦xαFˉon(x)x\mapsto x^\alpha\bar F_{\mathrm{on}}(x)x↦xαFˉon​(x) is slowly varying", with lengths non-negative. b(t)b(t)b(t) is inf⁡{x>0:tFˉon(x)≤1}\inf\{x>0:t\bar F_{\mathrm{on}}(x)\le1\}inf{x>0:tFˉon​(x)≤1}, which equals the page's generalized inverse for t>0t>0t>0. N(t)N(t)N(t) is a cardinality and the region sums are sums of non-negative terms; their junk values (an infinite set, a non-summable family) occur only on null events. AAA is an interval integral. The growth hypothesis is: λ>0\lambda>0λ>0, non-decreasing, Condition 1. No other hypothesis is added.

The fidi limit is pinned by its characteristic function on Rk\mathbb R^kRk for sorted times 0≤t1≤⋯≤tk0\le t_1\le\dots\le t_k0≤t1​≤⋯≤tk​: the product of the characteristic functions of Sα(σ(tj−tj−1)1/α,1,0)S_\alpha(\sigma(t_j-t_{j-1})^{1/\alpha},1,0)Sα​(σ(tj​−tj−1​)1/α,1,0) evaluated at θj+⋯+θk\theta_j+\dots+\theta_kθj​+⋯+θk​. The existence of the limit law is part of the claim. One-dimensional limits are stated the same way on R\mathbb RR. Convergence in probability to 000 is PT(∣YT∣>η)→0P_T(|Y_T|>\eta)\to0PT​(∣YT​∣>η)→0 for every η>0\eta>0η>0.

Trivializing formalizations are excluded:

  • bbb is never the junk value 000, since its defining set is nonempty and bounded below.
  • The model hypothesis is satisfiable for every rate and length law; a sanity file builds it from product measures, together with a Pareto law satisfying (2.8) and a rate satisfying Condition 1.
  • The limit object is fixed by its characteristic function, not merely asserted to exist.
  • Only fidi convergence is claimed, as on the page. Convergence in the Skorokhod J1J_1J1​ topology fails for this model (Remark after Theorem 1).

A complete development needs regular variation (Karamata's theorem, Potter bounds, generalized inverses), the Poisson random measure of the marked points, and stable limits for triangular arrays. All three are reusable beyond this mission. Proofs of the milestones are welcome separately, as are general Mathlib-style lemmas on regular variation.

Selected references

  • T. Mikosch, S. Resnick, H. Rootzén, A. Stegeman, Is network traffic approximated by stable Lévy motion or fractional Brownian motion?, Ann. Appl. Probab. 12(1) (2002) 23–68. https://doi.org/10.1214/aoap/1015961155
  • G. Samorodnitsky, M. S. Taqqu, Stable Non-Gaussian Random Processes, Chapman & Hall, 1994. https://doi.org/10.1201/9780203738818
  • N. H. Bingham, C. M. Goldie, J. L. Teugels, Regular Variation, Cambridge University Press, 1987. https://doi.org/10.1017/CBO9780511721434
  • S. I. Resnick, Extreme Values, Regular Variation, and Point Processes, Springer, 1987. https://doi.org/10.1007/978-0-387-75953-1
12 thms1 active userReviewed
Operations ResearchProbability·Captain: mikedeng1

Inventory Management of a Fast-Fashion Retail Network 1: Expected Sales Under the Major-Size Display Policy Are Non-Decreasing, Discretely Concave and SupermodularResearch Paper

Motivation

Fast-fashion retailers such as Zara replenish their stores several times a week from a central warehouse, and the warehouse holds a limited stock of each garment that must be split across hundreds of stores. Caro and Gallien built the store-level sales model behind the shipment-allocation system they developed with Zara and tested in a live pilot (Caro and Gallien, Inventory Management of a Fast-Fashion Retail Network, working paper, August 2, 2007; published in Operations Research 58(2), 2010). One display policy shapes the model. A garment (a reference) comes in several sizes, a few of which are designated major sizes. As soon as one major size runs out in a store, the whole reference is removed from the shop floor, so the remaining stock of the other sizes stops selling.

The allocation optimization only works if expected store sales have the right shape. They must grow with inventory, show decreasing marginal returns, and show complementarity across sizes. Proposition 1 of the paper establishes these properties for the model. The paper also cites the analogous result of Lu and Song (2003) for assemble-to-order systems as the template for its proof.

Setting

Fix a finite set of sizes S\mathcal SS, split into the major sizes S+\mathcal S^+S+ and the minor sizes S−=S∖S+\mathcal S^- = \mathcal S \setminus \mathcal S^+S−=S∖S+. Time t≥0t \ge 0t≥0 is measured from the last replenishment, and the next replenishment comes at time T>0T > 0T>0.

Demand is random. On a probability space, each size sss has a counting process Ns(t)N_s(t)Ns​(t), the number of sale opportunities for sss in [0,t][0, t][0,t]. It is a Poisson process with rate λs>0\lambda_s > 0λs​>0:

  • Ns(0)=0N_s(0) = 0Ns​(0)=0;
  • its paths are non-decreasing and right-continuous with jumps of size one;
  • the increment Ns(t)−Ns(u)N_s(t) - N_s(u)Ns​(t)−Ns​(u) is Poisson with mean λs(t−u)\lambda_s (t-u)λs​(t−u);
  • increments over disjoint intervals are independent.

The processes of different sizes are mutually independent. In Lean this family is IsPoissonFamily lam N P.

An inventory vector q=(qs)∈NSq = (q_s) \in \mathbb N^{\mathcal S}q=(qs​)∈NS gives the stock of each size right after replenishment. The virtual stockout time of size sss is

τs(qs)=inf⁡{t≥0:Ns(t)=qs},\tau_s(q_s) = \inf\{t \ge 0 : N_s(t) = q_s\},τs​(qs​)=inf{t≥0:Ns​(t)=qs​},

the time at which size sss would run out if it stayed on display. For a set of sizes A\mathcal AA, write τA=min⁡s∈Aτs(qs)\tau_{\mathcal A} = \min_{s \in \mathcal A} \tau_s(q_s)τA​=mins∈A​τs​(qs​) and a∧b=min⁡(a,b)a \wedge b = \min(a, b)a∧b=min(a,b). Under the major-size policy, the random sales over one period are

G(q)=∑s∈S+Ns(τS+∧T)+∑s∈S−Ns(τS+∪{s}∧T).(1)G(q) = \sum_{s \in \mathcal S^+} N_s(\tau_{\mathcal S^+} \wedge T) + \sum_{s \in \mathcal S^-} N_s(\tau_{\mathcal S^+ \cup \{s\}} \wedge T). \tag{1}G(q)=s∈S+∑​Ns​(τS+​∧T)+s∈S−∑​Ns​(τS+∪{s}​∧T).(1)

The expected sales function is g(q)=E[G(q)]g(q) = \mathbb E[G(q)]g(q)=E[G(q)] (expectedSales). The proof also uses hA(q)=E[τA∧T]h^{\mathcal A}(q) = \mathbb E[\tau_{\mathcal A} \wedge T]hA(q)=E[τA​∧T] (hA) and the marginal difference Δsf(q)=f(q+es)−f(q)\Delta_s f(q) = f(q + e_s) - f(q)Δs​f(q)=f(q+es​)−f(q) (delta), where ese_ses​ is the sss-th unit vector.

Formalization targets

Goal: Proposition 1

For every q∈NSq \in \mathbb N^{\mathcal S}q∈NS and all sizes s≠s′s \ne s's=s′:

g is non-decreasing,Δsg(q+es)≤Δsg(q),Δsg(q)≤Δsg(q+es′),g \text{ is non-decreasing}, \qquad \Delta_s g(q + e_s) \le \Delta_s g(q), \qquad \Delta_s g(q) \le \Delta_s g(q + e_{s'}),g is non-decreasing,Δs​g(q+es​)≤Δs​g(q),Δs​g(q)≤Δs​g(q+es′​),

and ggg is supermodular on the lattice NS\mathbb N^{\mathcal S}NS:

g(q)+g(q′)≤g(q∨q′)+g(q∧q′).g(q) + g(q') \le g(q \vee q') + g(q \wedge q').g(q)+g(q′)≤g(q∨q′)+g(q∧q′).

The statement is uniform in the rates, the horizon and the choice of major sizes, so it covers every instance of the model.

Milestones (Appendix §5.1 and §3.1.3, in the order the proof uses them)

  1. On every sample path, q↦G(q)q \mapsto G(q)q↦G(q) is non-decreasing.
  2. Identity (2): g(q)=λS+hS+(q)+∑s∈S−λshS+∪{s}(q)g(q) = \lambda_{\mathcal S^+} h^{\mathcal S^+}(q) + \sum_{s \in \mathcal S^-} \lambda_s h^{\mathcal S^+ \cup \{s\}}(q)g(q)=λS+​hS+(q)+∑s∈S−​λs​hS+∪{s}(q), where λS+=∑s∈S+λs\lambda_{\mathcal S^+} = \sum_{s \in \mathcal S^+} \lambda_sλS+​=∑s∈S+​λs​.
  3. For s∈As \in \mathcal As∈A, ΔshA(q)\Delta_s h^{\mathcal A}(q)Δs​hA(q) equals an integral over [0,T][0, T][0,T] of Poisson probabilities, and that integral equals 1λsP(τs(qs+1)≤τA∖{s}∧T)\frac{1}{\lambda_s}\mathbb P(\tau_s(q_s+1) \le \tau_{\mathcal A \setminus \{s\}} \wedge T)λs​1​P(τs​(qs​+1)≤τA∖{s}​∧T).
  4. ΔshA\Delta_s h^{\mathcal A}Δs​hA is non-increasing in qsq_sqs​ and non-decreasing in qs′q_{s'}qs′​ for s′≠ss' \ne ss′=s.
  5. On every sample path, q↦τA∧Tq \mapsto \tau_{\mathcal A} \wedge Tq↦τA​∧T is supermodular.
  6. hAh^{\mathcal A}hA is supermodular.

Significance

The result. Proposition 1 justifies treating each store's expected sales as a concave, complementary function of the size profile. The paper's allocation MIP is built on that structure. It approximates ggg by a lower envelope of tangents and embeds the approximation in a mixed integer program that allocates warehouse stock across stores. The proposition explains why sending a unit of a major size can raise the value of the minor sizes already in a store. It also explains why the marginal value of a size falls as more of it is shipped. Without these properties a greedy or envelope-based allocation would have no structural footing.

Formalizing it. The result is proved on paper, with one error in the printed proof. The last line of the Appendix display gives ΔshA(q)\Delta_s h^{\mathcal A}(q)Δs​hA(q) as a probability, but the quantity is a time. The correct value carries a factor 1/λs1/\lambda_s1/λs​ and has qs+1q_s + 1qs​+1 in place of qsq_sqs​. This mission states the corrected identity. As far as is known, no machine-checked proof of any part of the result exists. A complete development would give a verified link from a continuous-time stochastic model to the discrete convexity properties that inventory optimization relies on. It would also produce reusable facts about Poisson processes and their hitting times along the way.

Difficulty

The monotonicity of ggg is pathwise and elementary. The other properties are not pathwise properties of GGG. Under the major-size policy, a realisation of GGG need not have decreasing increments in qsq_sqs​. The concavity and the complementarity appear only after taking expectations and rewriting ggg through the stopping times, using identity (2). That identity is an optional-sampling statement for the compensated Poisson processes at the bounded random times τA∧T\tau_{\mathcal A} \wedge TτA​∧T. These times depend on several independent processes at once, so the relevant filtration is the joint one. Mathlib has optional sampling only in discrete time.

The marginal-difference formula needs three ingredients:

  • the tail-integral representation of E[τA∧T]\mathbb E[\tau_{\mathcal A} \wedge T]E[τA​∧T];
  • the factorisation of P(τA>t)\mathbb P(\tau_{\mathcal A} > t)P(τA​>t) through independence across sizes;
  • the Erlang law of the hitting times τs(k)\tau_s(k)τs​(k).

The first idea, proving concavity of ggg directly from (1) path by path, fails for the reason above.

Formalization scope

All objects live in the namespace FastFashion.Structure:

  • Sizes: a Fintype with decidable equality. The major sizes are a Finset Sp and the minor sizes are its complement. No nonemptiness assumption is placed on the sizes or on S+\mathcal S^+S+; S+=∅\mathcal S^+ = \emptysetS+=∅ is allowed, as in the paper.
  • Inventories: vectors q:S→Nq : \mathcal S \to \mathbb Nq:S→N with the componentwise order and lattice operations. ese_ses​ is Pi.single s 1.
  • Stockout times: τs(qs)\tau_s(q_s)τs​(qs​) takes values in WithTop ℝ. It is +∞+\infty+∞ on paths that never reach qsq_sqs​, so it is never Lean's junk value 000, and τ∅=+∞\tau_\emptyset = +\inftyτ∅​=+∞. The truncation τA∧T\tau_{\mathcal A} \wedge TτA​∧T (stopMin) is a real number in [0,T][0, T][0,T].
  • Expectations and probabilities: expectations are Bochner integrals. They need no integrability hypothesis, because 0≤G(q)≤∑sNs(T)0 \le G(q) \le \sum_s N_s(T)0≤G(q)≤∑s​Ns​(T) and 0≤τA∧T≤T0 \le \tau_{\mathcal A} \wedge T \le T0≤τA​∧T≤T. Probabilities are real numbers.
  • Supermodularity: Topkis's lattice definition, the published platform definition Supermodularity.Monotonicity.SupermodularOn, applied on the whole lattice.
  • Poisson family: the processes are independent as whole processes. The σ-algebras generated by all times are independent, not only the one-dimensional marginals.

Two formalizations would trivialize the mission, and neither is used. ggg is defined as the expectation of GGG from (1), never by formula (2), and hAh^{\mathcal A}hA is never defined by a product-of-probabilities integral. Proposition 1 states both readings of "supermodular": the per-coordinate marginal-difference inequalities and the lattice inequality.

Deviations from the printed text:

  • The last line of the Appendix display is replaced by 1λsP(τs(qs+1)≤τA∖{s}∧T)\frac{1}{\lambda_s}\mathbb P(\tau_s(q_s+1) \le \tau_{\mathcal A\setminus\{s\}} \wedge T)λs​1​P(τs​(qs​+1)≤τA∖{s}​∧T).
  • "non-decreasing in xsx_sxs​" in Proposition 1 is read as qsq_sqs​.

Infrastructure a complete development needs:

  • hitting times of counting processes and their Erlang laws;
  • a continuous-time optional sampling theorem for the compensated Poisson process, or a direct computation from independent increments;
  • the tail formula E[X]=∫0∞P(X>t) dt\mathbb E[X] = \int_0^\infty \mathbb P(X > t)\,dtE[X]=∫0∞​P(X>t)dt for bounded non-negative XXX;
  • lattice facts about minima of single-variable increasing functions.

The Poisson-process and hitting-time lemmas are reusable well beyond this mission and are welcome as separate contributions. The companion mission on the paper's tangent-envelope approximation uses the same model layer.

Selected references

  • F. Caro, J. Gallien, Inventory Management of a Fast-Fashion Retail Network, working paper, August 2, 2007; published in Operations Research 58(2):257–273, 2010. https://doi.org/10.1287/opre.1090.0698
  • D. M. Topkis, Supermodularity and Complementarity, Princeton University Press, 1998. https://doi.org/10.1515/9781400822539
  • Y. Lu, J.-S. Song, Order-Based Cost Optimization in Assemble-to-Order Systems, Operations Research 53(1):151–169, 2005 (working paper 2003). https://doi.org/10.1287/opre.1040.0146
  • I. Karatzas, S. E. Shreve, Brownian Motion and Stochastic Calculus, 2nd ed., Springer, 1991. https://doi.org/10.1007/978-1-4612-0949-2
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Dynamical SystemsOperations ResearchTheoretical Computer Science·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 thms1 active userReviewed
Operations ResearchProbability·Captain: mikedeng1

Is Network Traffic Approximated by Stable Lévy Motion or Fractional Brownian Motion? 4: Superposed ON/OFF Input Under Fast Growth Converges in C[0,∞) to Fractional Brownian MotionResearch Paper

Why heavy-tailed input matters

Measurements of Ethernet and Internet traffic in the 1990s showed that cumulative traffic is self-similar and long-range dependent: correlations of the input rate decay so slowly that they are not summable, and fluctuations at large time scales do not average out the way Poisson-type models predict (Leland et al. 1994). A widely accepted explanation is that the lengths of individual transmissions (file sizes, session durations) are heavy tailed, with infinite variance. Queueing and capacity-planning calculations then depend on which stochastic process approximates the cumulative input over long horizons.

Two approximations had been proposed: fractional Brownian motion, a Gaussian self-similar process with dependent increments, and α-stable Lévy motion, a heavy-tailed process with independent increments. Mikosch, Resnick, Rootzén and Stegeman (Ann. Appl. Probab. 12 (2002) 23–68) showed that both arise from the same models and that the answer depends on how fast the number of sources grows relative to the time scale. This mission formalizes their Gaussian answer for the superposition of ON/OFF sources: Theorem 4.

  • 1995–1997: Willinger, Taqqu, Sherman and Wilson derive fractional Brownian motion from superposed ON/OFF sources with heavy-tailed periods, as an iterated limit: first the number of sources M→∞M\to\inftyM→∞, then the time scale T→∞T\to\inftyT→∞, and for finite-dimensional distributions only.
  • 1998: Heath, Resnick and Samorodnitsky (Math. Oper. Res. 23) give the exact decay of the covariance of a single stationary ON/OFF source.
  • 2002: Mikosch, Resnick, Rootzén and Stegeman let MMM and TTT grow together and show that fast growth gives fractional Brownian motion as a functional limit in C[0,∞)\mathbb C[0,\infty)C[0,∞), while slow growth gives stable Lévy motion.

The superposed ON/OFF model

A single ON/OFF source alternates between ON-periods, during which it sends work at rate 111, and silent OFF-periods. The ON-periods X1,X2,…X_1,X_2,\dotsX1​,X2​,… are iid with law FonF_{\mathrm{on}}Fon​ and the OFF-periods Yoff,Y1,Y2,…Y_{\mathrm{off}},Y_1,Y_2,\dotsYoff​,Y1​,Y2​,… iid with law FoffF_{\mathrm{off}}Foff​, both on [0,∞)[0,\infty)[0,∞), all independent, with means μon\mu_{\mathrm{on}}μon​, μoff\mu_{\mathrm{off}}μoff​ and μ=μon+μoff\mu=\mu_{\mathrm{on}}+\mu_{\mathrm{off}}μ=μon​+μoff​. The tails are regularly varying: for x>0x>0x>0,

Fˉon(x)=x−αLon(x),Fˉoff(x)=x−αoffLoff(x),1<α<αoff<2,\bar F_{\mathrm{on}}(x)=x^{-\alpha}L_{\mathrm{on}}(x),\qquad \bar F_{\mathrm{off}}(x)=x^{-\alpha_{\mathrm{off}}}L_{\mathrm{off}}(x),\qquad 1<\alpha<\alpha_{\mathrm{off}}<2,Fˉon​(x)=x−αLon​(x),Fˉoff​(x)=x−αoff​Loff​(x),1<α<αoff​<2,

with Lon,LoffL_{\mathrm{on}},L_{\mathrm{off}}Lon​,Loff​ slowly varying (L(cx)/L(x)→1L(cx)/L(x)\to1L(cx)/L(x)→1 for every c>0c>0c>0). So both periods have finite mean and infinite variance, and the ON-periods have the heavier tail.

To make the source stationary, a delay T0=B(Xon(0)+Yoff)+(1−B)Yoff(0)T_0=B(X^{(0)}_{\mathrm{on}}+Y_{\mathrm{off}})+(1-B)Y^{(0)}_{\mathrm{off}}T0​=B(Xon(0)​+Yoff​)+(1−B)Yoff(0)​ is used, where BBB is Bernoulli with P(B=1)=μon/μP(B=1)=\mu_{\mathrm{on}}/\muP(B=1)=μon​/μ and Xon(0),Yoff(0)X^{(0)}_{\mathrm{on}},Y^{(0)}_{\mathrm{off}}Xon(0)​,Yoff(0)​ have the integrated-tail laws F(0)(x)=μF−1∫0xFˉ(s) dsF^{(0)}(x)=\mu_F^{-1}\int_0^x\bar F(s)\,dsF(0)(x)=μF−1​∫0x​Fˉ(s)ds. With Tn=T0+∑i=1n(Xi+Yi)T_n=T_0+\sum_{i=1}^n(X_i+Y_i)Tn​=T0​+∑i=1n​(Xi​+Yi​) the source's activity is

Wt=B 1[0,Xon(0))(t)+∑n≥01[Tn,Tn+Xn+1)(t),t≥0,W_t=B\,\mathbf 1_{[0,X^{(0)}_{\mathrm{on}})}(t)+\sum_{n\ge0}\mathbf 1_{[T_n,T_n+X_{n+1})}(t),\qquad t\ge0,Wt​=B1[0,Xon(0)​)​(t)+n≥0∑​1[Tn​,Tn​+Xn+1​)​(t),t≥0,

a stationary process with EWt=μon/μEW_t=\mu_{\mathrm{on}}/\muEWt​=μon​/μ.

The TTT-th model superposes M=M(T)M=M(T)M=M(T) independent copies W(1),…,W(M)W^{(1)},\dots,W^{(M)}W(1),…,W(M), where MMM is integer valued, non-decreasing and M(T)→∞M(T)\to\inftyM(T)→∞. The cumulative input is A(t)=∫0t∑m=1MWs(m) dsA(t)=\int_0^t\sum_{m=1}^MW^{(m)}_s\,dsA(t)=∫0t​∑m=1M​Ws(m)​ds. With the quantile b(t)=(1/Fˉon)←(t)b(t)=(1/\bar F_{\mathrm{on}})^{\leftarrow}(t)b(t)=(1/Fˉon​)←(t), the fast growth condition is

Condition 2:lim⁡T→∞b(MT)T=∞,\text{Condition 2:}\qquad \lim_{T\to\infty}\frac{b(MT)}{T}=\infty,Condition 2:T→∞lim​Tb(MT)​=∞,

equivalently MTFˉon(T)→∞MT\bar F_{\mathrm{on}}(T)\to\inftyMTFˉon​(T)→∞. The normalisation and limit constants are

dT=[T3−αLon(T)M]1/2,σ02=2μoff2Γ(2−α)/(α−1)μ3Γ(4−α),H=3−α2∈(12,1).d_T=[T^{3-\alpha}L_{\mathrm{on}}(T)M]^{1/2},\qquad \sigma_0^2=\frac{2\mu_{\mathrm{off}}^2\Gamma(2-\alpha)/(\alpha-1)}{\mu^3\Gamma(4-\alpha)},\qquad H=\frac{3-\alpha}{2}\in(\tfrac12,1).dT​=[T3−αLon​(T)M]1/2,σ02​=μ3Γ(4−α)2μoff2​Γ(2−α)/(α−1)​,H=23−α​∈(21​,1).

A standard fractional Brownian motion BHB_HBH​ is a mean-zero Gaussian process on [0,∞)[0,\infty)[0,∞) with continuous paths and Cov(BH(t),BH(s))=12(t2H+s2H−∣t−s∣2H)\mathrm{Cov}(B_H(t),B_H(s))=\tfrac12(t^{2H}+s^{2H}-|t-s|^{2H})Cov(BH​(t),BH​(s))=21​(t2H+s2H−∣t−s∣2H).

Formalization targets

Goal: Theorem 4

If Condition 2 holds, then

A(T⋅)−TMμ−1μon(⋅)dT →d σ0BH(⋅)weakly in C[0,∞).\frac{A(T\cdot)-TM\mu^{-1}\mu_{\mathrm{on}}(\cdot)}{d_T}\ \xrightarrow{d}\ \sigma_0B_H(\cdot)\qquad\text{weakly in }\mathbb C[0,\infty).dT​A(T⋅)−TMμ−1μon​(⋅)​ d​ σ0​BH​(⋅)weakly in C[0,∞).

Intermediate targets

In the order of the paper's argument: the mean EWt=μon/μEW_t=\mu_{\mathrm{on}}/\muEWt​=μon​/μ (p. 27); the covariance decay (2.5) γW(h)∼μoff2(α−1)μ3h−(α−1)Lon(h)\gamma_W(h)\sim\frac{\mu_{\mathrm{off}}^2}{(\alpha-1)\mu^3}h^{-(\alpha-1)}L_{\mathrm{on}}(h)γW​(h)∼(α−1)μ3μoff2​​h−(α−1)Lon​(h); Condition 2 ⇔T=o(dT)\Leftrightarrow T=o(d_T)⇔T=o(dT​) (p. 61); the variance asymptotic (7.1) Var(GT)∼σ02T3−αLon(T)\mathrm{Var}(G_T)\sim\sigma_0^2T^{3-\alpha}L_{\mathrm{on}}(T)Var(GT​)∼σ02​T3−αLon​(T) for GT=∫0T(Wu−EWu) duG_T=\int_0^T(W_u-EW_u)\,duGT​=∫0T​(Wu​−EWu​)du; Lemma 13, the one-dimensional limit dT−1∑mGTt(m)→N(0,σ02t3−α)d_T^{-1}\sum_mG^{(m)}_{Tt}\to N(0,\sigma_0^2t^{3-\alpha})dT−1​∑m​GTt(m)​→N(0,σ02​t3−α); the covariance limit (7.4); and the second-moment bound E∣dT−1∑mGTu(m)∣2≤c u1+εE|d_T^{-1}\sum_mG^{(m)}_{Tu}|^2\le c\,u^{1+\varepsilon}E∣dT−1​∑m​GTu(m)​∣2≤cu1+ε behind tightness (p. 63). (2.5) and (7.1) are cited by the paper from Heath–Resnick–Samorodnitsky and Willinger–Taqqu–Sherman–Wilson; they are stated here as the paper states them.

Significance

Theorem 4 justifies fractional Brownian motion as the model of aggregate traffic from many heavy-tailed sources in a single, simultaneous limit, replacing the iterated limit of earlier work, and it upgrades finite-dimensional convergence to weak convergence of paths. Functionals of the path, such as the supremum of A(Tt)−ctA(Tt)-ctA(Tt)−ct that governs the buffer content of a fluid queue, therefore inherit Gaussian approximations. Together with Theorem 2 it shows that a single growth condition on MMM decides between Gaussian and stable approximations.

The result is proved in the paper; it is not formalized anywhere. A formalization adds a machine-checked statement of the theorem and reusable developments of regularly varying functions, the stationary alternating renewal process, fractional Brownian motion, and convergence in C[0,∞)\mathbb C[0,\infty)C[0,∞).

Difficulty

The obvious route is a central limit theorem for ∑mGTt(m)\sum_{m}G^{(m)}_{Tt}∑m​GTt(m)​, a sum of MMM iid bounded terms; but the number of terms and their distribution change with TTT, so one needs a triangular-array limit theorem whose variance condition rests on the exact asymptotic (7.1). That asymptotic in turn needs the covariance decay (2.5) of a single stationary source, which requires renewal theory for the alternating process with infinite-variance periods. Convergence of finite-dimensional distributions alone does not give the theorem: tightness in C[0,K]\mathbb C[0,K]C[0,K] needs a moment bound on increments that is uniform in TTT for small time lags, which requires Potter-type bounds for the regularly varying function x↦EGx2x\mapsto EG_x^2x↦EGx2​.

Formalization scope

  • Time and models. T→∞T\to\inftyT→∞ along atTop on R\mathbb RR. Each model TTT has its own probability space carrying M(T)M(T)M(T) independent sources; the theorems hold for every such family. Lean's X n, Y n are the paper's Xn+1X_{n+1}Xn+1​, Yn+1Y_{n+1}Yn+1​ and Lean's sources 0,…,M−10,\dots,M-10,…,M−1 are the paper's 1,…,M1,\dots,M1,…,M. Time in the normalised process runs over R≥0\mathbb R_{\ge0}R≥0​.
  • Standing hypotheses. Fon,FoffF_{\mathrm{on}},F_{\mathrm{off}}Fon​,Foff​ are probability measures on [0,∞)[0,\infty)[0,∞) (non-negativity is implicit in "lengths"); (2.1) is stated as "x↦xαFˉ(x)x\mapsto x^{\alpha}\bar F(x)x↦xαFˉ(x) is slowly varying"; 1<α<αoff<21<\alpha<\alpha_{\mathrm{off}}<21<α<αoff​<2; MMM non-decreasing with M→∞M\to\inftyM→∞ (§3.2); Condition 2 where §7 assumes it. No other hypothesis is added.
  • Junk values ruled out. bbb is an infimum over {x>0:tFˉon(x)≤1}\{x>0:t\bar F_{\mathrm{on}}(x)\le1\}{x>0:tFˉon​(x)≤1}, never a division by zero; the series defining WtW_tWt​ has non-negative terms and fails to converge only on a null event; equalities of laws come with measurability. The limit is pinned completely: Gaussian, mean zero, the covariance above with σH=1\sigma_H=1σH​=1 and H=(3−α)/2H=(3-\alpha)/2H=(3−α)/2, continuous paths, multiplied by σ0\sigma_0σ0​. Fidi convergence in place of the functional limit, a free scale in the limit, or a limit identified only by its marginals would each be a different, weaker theorem.
  • Weak convergence is stated in coupling form: for every sequence Tn→∞T_n\to\inftyTn​→∞ there are one probability space, copies YnY_nYn​ with continuous paths of the laws of the normalised processes at TnT_nTn​, and a standard fractional Brownian motion Y′Y'Y′ such that Yn→σ0Y′Y_n\to\sigma_0Y'Yn​→σ0​Y′ uniformly on every [0,K][0,K][0,K] almost surely. On the Polish space C[0,∞)\mathbb C[0,\infty)C[0,∞) this is equivalent to weak convergence.
  • Infrastructure needed: Karamata's theorem and Potter bounds; the stationary alternating renewal process and its covariance asymptotics; a triangular-array central limit theorem; existence of fractional Brownian motion; a moment criterion for tightness in C[0,K]\mathbb C[0,K]C[0,K]. The regular-variation and path-space material is reusable well beyond this mission; contributions of any of these pieces, and of any milestone, are welcome.

Selected references

  • T. Mikosch, S. Resnick, H. Rootzén and A. Stegeman, Is network traffic approximated by stable Lévy motion or fractional Brownian motion?, Ann. Appl. Probab. 12(1) (2002), 23–68. https://doi.org/10.1214/aoap/1015961155
  • D. Heath, S. Resnick and G. Samorodnitsky, Heavy tails and long range dependence in on/off processes and associated fluid models, Math. Oper. Res. 23 (1998), 145–165. https://doi.org/10.1287/moor.23.1.145
  • W. Willinger, M. S. Taqqu, R. Sherman and D. V. Wilson, Self-similarity through high-variability: statistical analysis of Ethernet LAN traffic at the source level, IEEE/ACM Trans. Networking 5 (1997), 71–86. https://doi.org/10.1109/90.554723
  • W. E. Leland, M. S. Taqqu, W. Willinger and D. V. Wilson, On the self-similar nature of Ethernet traffic (extended version), IEEE/ACM Trans. Networking 2 (1994), 1–15. https://doi.org/10.1109/90.282603
  • N. H. Bingham, C. M. Goldie and J. L. Teugels, Regular Variation, Cambridge University Press, 1987. https://doi.org/10.1017/CBO9780511721434
  • P. Billingsley, Convergence of Probability Measures, Wiley, 1968 (Theorem 12.3, moment criterion for tightness).
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Operations ResearchProbability·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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