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Stochastic Systems

166 missions · 63 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.

Missions

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Markov ChainOperations ResearchProbability·Captain: mikedeng1

Fundamentals of Queueing Theory I: Foster's Criterion for Positive RecurrenceTextbook

Motivation

Almost every model in queueing theory is analysed through a Markov chain. The number of customers in an M/M/c queue is a continuous-time birth–death chain; the number left behind by departing customers of an M/G/1 queue is a discrete-parameter chain on {0,1,2,… }\{0,1,2,\dots\}{0,1,2,…} (the imbedded Markov chain); networks of queues are chains on vectors of queue lengths. Before any steady-state formula (Erlang's formulas, the Pollaczek–Khintchine formula, product forms) can be used, one has to know that the chain has a steady state at all: that it is positive recurrent, so that a stationary distribution exists and equals the limiting distribution.

Chapter 1 of Gross, Shortle, Thompson and Harris, Fundamentals of Queueing Theory (4th ed., Wiley 2008, DOI 10.1002/9781118625651), collects the two ingredients the rest of the book stands on: the Poisson process with its exponential interarrival times (§§1.7–1.8), and the classification theory of discrete-parameter Markov chains (§1.9), ending with Foster's criterion (Theorem 1.2), a sufficient condition for positive recurrence in terms of a drift inequality. The criterion goes back to F. G. Foster, On the stochastic matrices associated with certain queuing processes, Ann. Math. Statist. 24 (1953) (DOI 10.1214/aoms/1177728976), and is the ancestor of the Foster–Lyapunov method used for stability of queueing networks and stochastic systems.

This mission is the first of a series formalizing the book chapter by chapter.

Setting

A homogeneous discrete-parameter Markov chain on {0,1,2,… }\{0,1,2,\dots\}{0,1,2,…} is given by a transition matrix P={pij}P=\{p_{ij}\}P={pij​} with pij≥0p_{ij}\ge0pij​≥0 and ∑jpij=1\sum_j p_{ij}=1∑j​pij​=1 for every iii. The mmm-step transition probabilities pij(m)p_{ij}^{(m)}pij(m)​ are the entries of PmP^mPm.

The first-passage probability fij(n)f_{ij}^{(n)}fij(n)​ is the probability that the chain started in iii enters jjj for the first time at step n≥1n\ge1n≥1; for i=ji=ji=j it is the probability of first return at step nnn. The return probability is fjj=∑n≥1fjj(n)f_{jj}=\sum_{n\ge1}f_{jj}^{(n)}fjj​=∑n≥1​fjj(n)​ and the mean recurrence time is mjj=∑n≥1nfjj(n)∈[0,∞]m_{jj}=\sum_{n\ge1}n f_{jj}^{(n)}\in[0,\infty]mjj​=∑n≥1​nfjj(n)​∈[0,∞]. A state is positive recurrent if fjj=1f_{jj}=1fjj​=1 and mjj<∞m_{jj}<\inftymjj​<∞; the chain is positive recurrent if every state is.

The chain is irreducible if for every pair of states (i,j)(i,j)(i,j) some pij(n)p_{ij}^{(n)}pij(n)​ is positive, and aperiodic if for every state kkk the greatest common divisor of {n≥1:pkk(n)>0}\{n\ge1:p_{kk}^{(n)}>0\}{n≥1:pkk(n)​>0} is 111. A stationary distribution is a probability vector π\piπ with π=πP\pi=\pi Pπ=πP, i.e. πj=∑iπipij\pi_j=\sum_i\pi_i p_{ij}πj​=∑i​πi​pij​ for every jjj.

For the Poisson part, T0,T1,…T_0,T_1,\dotsT0​,T1​,… are independent interarrival times, each exponentially distributed with rate λ>0\lambda>0λ>0; the arrival epochs are Sn=T0+⋯+Tn−1S_n=T_0+\dots+T_{n-1}Sn​=T0​+⋯+Tn−1​, and N(t)=#{n≥1:Sn≤t}N(t)=\#\{n\ge1:S_n\le t\}N(t)=#{n≥1:Sn​≤t} counts the arrivals in [0,t][0,t][0,t].

Formalization targets

Goal: Theorem 1.2 (Foster's criterion)

An irreducible, aperiodic chain is positive recurrent if there exist xj≥0x_j\ge0xj​≥0 with

∑j=0∞pijxj≤xi−1(i≠0),∑j=0∞p0jxj<∞.\sum_{j=0}^\infty p_{ij}x_j\le x_i-1\quad(i\ne0),\qquad\sum_{j=0}^\infty p_{0j}x_j<\infty .j=0∑∞​pij​xj​≤xi​−1(i=0),j=0∑∞​p0j​xj​<∞.

Milestones: the Markov chain theorems

  • Theorem 1.1(a). In an irreducible, positive recurrent chain, πj=1/mjj\pi_j=1/m_{jj}πj​=1/mjj​ is a stationary distribution, and it is the only one.
  • Theorem 1.1(c). If moreover the chain is aperiodic and all moments of π\piπ are finite, then lim⁡m→∞pij(m)=πj\lim_{m\to\infty}p_{ij}^{(m)}=\pi_jlimm→∞​pij(m)​=πj​ for all i,ji,ji,j.

Milestones: the Poisson process and the exponential distribution

  • Eqs. (1.11)–(1.14). The unique solution of p0′=−λp0p_0'=-\lambda p_0p0′​=−λp0​, pn′=−λpn+λpn−1p_n'=-\lambda p_n+\lambda p_{n-1}pn′​=−λpn​+λpn−1​ with p0(0)=1p_0(0)=1p0​(0)=1, pn(0)=0p_n(0)=0pn​(0)=0 is pn(t)=(λt)ne−λt/n!p_n(t)=(\lambda t)^n e^{-\lambda t}/n!pn​(t)=(λt)ne−λt/n!.
  • Eq. (1.15). With exponential interarrival times,
Pr⁡{N(t)≤n}=∫t∞λ(λx)nn!e−λxdx=∑i=0n(λt)ie−λti!.\Pr\{N(t)\le n\}=\int_t^\infty\frac{\lambda(\lambda x)^n}{n!}e^{-\lambda x}dx=\sum_{i=0}^n\frac{(\lambda t)^ie^{-\lambda t}}{i!}.Pr{N(t)≤n}=∫t∞​n!λ(λx)n​e−λxdx=i=0∑n​i!(λt)ie−λt​.
  • Eq. (1.16). Given N(L)=kN(L)=kN(L)=k, the arrival epochs have density k!/Lkk!/L^kk!/Lk on {0<t1<⋯<tk<L}\{0<t_1<\dots<t_k<L\}{0<t1​<⋯<tk​<L}.
  • Eq. (1.17) and its converse (p.21). The exponential law satisfies Pr⁡{T≤t1∣T≥t0}=Pr⁡{0≤T≤t1−t0}\Pr\{T\le t_1\mid T\ge t_0\}=\Pr\{0\le T\le t_1-t_0\}Pr{T≤t1​∣T≥t0​}=Pr{0≤T≤t1​−t0​}, and it is the only continuous distribution on [0,∞)[0,\infty)[0,∞) that does.
  • Nonhomogeneous Poisson law (p.22). With a continuous rate λ(t)\lambda(t)λ(t) the forward equations have the unique solution pn(t)=e−m(t)m(t)n/n!p_n(t)=e^{-m(t)}m(t)^n/n!pn​(t)=e−m(t)m(t)n/n!, m(t)=∫0tλ(s) dsm(t)=\int_0^t\lambda(s)\,dsm(t)=∫0t​λ(s)ds.

Significance

Foster's criterion reduces positive recurrence, a statement about return times, to exhibiting one test function xxx with negative drift outside a single state. In the book it is the tool that establishes the existence of steady state for imbedded chains of the M/G/1 and G/M/1 queues (Chapter 5); its generalizations are the standard stability proofs for queueing networks. Theorem 1.1 then supplies what positive recurrence buys: the stationary distribution exists, is unique, equals 1/mjj1/m_{jj}1/mjj​, and is the limit of the transition probabilities. The Poisson results justify the "Markovian" arrivals and services of Chapters 2–4.

All of these results are classical and proved in the literature; the book states Theorems 1.1 and 1.2 without proof. The Prove2Me platform already holds machine-checked versions of related Markov chain theorems in other missions (Levin–Peres–Wilmer's and Durrett's countable-chain convergence theorems), stated with different definitions and hypotheses. What this mission adds is a formal development in the book's own terms — first-passage probabilities fjj(n)f_{jj}^{(n)}fjj(n)​, mean recurrence times mjjm_{jj}mjj​, gcd periodicity — on which the later missions of the series (imbedded chains, birth–death processes) can build, together with a formal proof of Foster's criterion, which is not on the platform.

Difficulty

For Foster's criterion the natural first step, taking expectations of the drift inequality along the chain, only shows that the expected value of xxx decreases while the chain stays away from 000. Turning that into a bound on the expected return time to 000 requires an optional-stopping or telescoping argument over a random time, with the value xxx possibly unbounded, and a separate argument that positive recurrence of state 000 propagates to all states of an irreducible chain. The book's hypotheses include aperiodicity, which the argument does not use.

For Theorem 1.1, identifying the stationary distribution with 1/mjj1/m_{jj}1/mjj​ requires relating the matrix powers PnP^nPn to the first-passage probabilities (a renewal decomposition), and uniqueness over countably many states needs care with infinite sums. For the Poisson results, the difficulty is measure-theoretic: the distribution of the sum of n+1n+1n+1 exponential variables, and conditioning on the event {N(L)=k}\{N(L)=k\}{N(L)=k} for the order-statistics property.

Formalization scope

States are natural numbers; the transition matrix is a real function p:N×N→Rp:\mathbb N\times\mathbb N\to\mathbb Rp:N×N→R with nonnegative entries and rows summing to one (as a convergent series). The return probability and the mean recurrence time are valued in [0,∞][0,\infty][0,∞], so null recurrence (mjj=∞m_{jj}=\inftymjj​=∞) is representable. Irreducibility is the per-pair notion. Stationary equations are stated componentwise with convergent series.

In Foster's criterion the series ∑jpijxj\sum_j p_{ij}x_j∑j​pij​xj​ are required to converge for every iii, which is the book's condition ∑jp0jxj<∞\sum_j p_{0j}x_j<\infty∑j​p0j​xj​<∞ together with the finiteness implicit in the inequalities for i≠0i\ne0i=0; xxx is real-valued and nonnegative. Dropping the convergence requirement would let a divergent row series (whose Lean sum is 000) satisfy the inequality vacuously; allowing xj=∞x_j=\inftyxj​=∞ would make the hypothesis trivially satisfiable. Neither is permitted.

The closed forms stated explicitly are: πj=1/mjj\pi_j=1/m_{jj}πj​=1/mjj​ (Theorem 1.1(a), with both existence and uniqueness), the Poisson probabilities (λt)ne−λt/n!(\lambda t)^ne^{-\lambda t}/n!(λt)ne−λt/n! (1.14), the Erlang tail integral and the Poisson CDF (1.15), the density k!/Lkk!/L^kk!/Lk (1.16), and e−m(t)m(t)n/n!e^{-m(t)}m(t)^n/n!e−m(t)m(t)n/n! for the nonhomogeneous law. Equations (1.14) and the nonhomogeneous law are stated as "solves the equations with the initial conditions if and only if equals the closed form", so both existence and uniqueness are asserted.

The Poisson results use random variables on a probability space, with Mathlib's expMeasure for the exponential law and cond for conditional probability. The derivation of the forward equations from the o(Δt)o(\Delta t)o(Δt) axioms of §1.7 is not formalized; the Poisson law is reached from the equations and, separately, from exponential interarrival times.

Not formalized: Theorem 1.1(b) and the word "ergodic" in 1.1(c), which rest on the book's informal notion of ergodicity; Theorem 1.3, whose phrase "for Theorem 1.1 to be valid" for a continuous-time chain is not pinned down.

The Markov chain definitions are reusable by every later mission that studies an imbedded chain. Contributions welcome: proofs of the milestones, and supporting lemmas (Chapman–Kolmogorov, renewal decomposition of pjj(n)p_{jj}^{(n)}pjj(n)​, class properties of recurrence).

Selected references

  • D. Gross, J. F. Shortle, J. M. Thompson, C. M. Harris, Fundamentals of Queueing Theory, 4th ed., Wiley, 2008. https://doi.org/10.1002/9781118625651
  • F. G. Foster, On the stochastic matrices associated with certain queuing processes, Annals of Mathematical Statistics 24 (1953), 355–360. https://doi.org/10.1214/aoms/1177728976
11 thms1 active userReviewed
Dynamic ProgrammingMarkov ChainOperations Research+1·Captain: mikedeng1

Stochastic Dynamic Programming and the Control of Queueing Systems VII: The (BOR) Assumptions and Positive Recurrence of Optimal PoliciesTextbook

Motivation

Queueing control problems (admission control, routing, service rate selection) are naturally modelled as Markov decision chains with a countably infinite state space and unbounded costs, for instance a holding cost that grows with the queue length. For such models the long-run average cost criterion is often the relevant one, and the central question is whether an optimal stationary policy exists and can be computed from an average cost optimality equation (ACOE). Chapter 7 of Linn I. Sennott, Stochastic Dynamic Programming and the Control of Queueing Systems (Wiley, 1999, doi:10.1002/9780470317037) develops a verifiable set of conditions, the (SEN) assumptions, under which an average cost optimality inequality (ACOI) holds and yields an optimal stationary policy. The inequality may be strict (Example 7.3.1), and an optimal policy may induce a Markov chain without positive recurrent states.

Sections 7.4 and 7.5 answer two practical questions: when is the ACOI in fact an equation, and how can (SEN) be checked in a concrete model? The answer culminates in the (BOR) assumptions, which require only one well-behaved stationary policy and the finiteness of a set of low-cost states.

According to the book's bibliographic notes (p. 163): the (BOR) assumptions modify a line of development due to Borkar (SIAM J. Control Optim. 22, 1984, and 27, 1989; monograph 1991) and are weaker than his original conditions; the proof that (BOR) implies (SEN) is from Cavazos-Cadena and Sennott (Oper. Res. Letters 11, 1992), and the version of (BOR) used here is from Sennott (Prob. Eng. Inform. Sci. 7, 1993). Proposition 7.5.5 and the (CAV*) assumptions go back to Cavazos-Cadena (Kybernetika 25, 1989); Proposition 7.5.3 and Corollary 7.5.4 to Sennott (Oper. Res. 37, 1989).

Setting

A Markov decision chain consists of a countable state space SSS, finite nonempty action sets AiA_iAi​, nonnegative finite costs C(i,a)C(i,a)C(i,a) and transition probabilities Pij(a)P_{ij}(a)Pij​(a). A policy θ\thetaθ may use the whole history and randomize. For α∈(0,1)\alpha\in(0,1)α∈(0,1) the discount value function is Vα(i)=inf⁡θVθ,α(i)V_\alpha(i)=\inf_\theta V_{\theta,\alpha}(i)Vα​(i)=infθ​Vθ,α​(i), the infimum of ∑tαtEθ[C(Xt,At)∣X0=i]\sum_t\alpha^tE_\theta[C(X_t,A_t)\mid X_0=i]∑t​αtEθ​[C(Xt​,At​)∣X0​=i]; the average cost of θ\thetaθ is Jθ(i)=lim sup⁡n1nEθ[∑t<nC(Xt,At)∣X0=i]J_\theta(i)=\limsup_n\frac1nE_\theta[\sum_{t<n}C(X_t,A_t)\mid X_0=i]Jθ​(i)=limsupn​n1​Eθ​[∑t<n​C(Xt​,At​)∣X0​=i] and the minimum average cost is J(i)=inf⁡θJθ(i)J(i)=\inf_\theta J_\theta(i)J(i)=infθ​Jθ​(i). All of these lie in [0,∞][0,\infty][0,∞].

For a distinguished state zzz the relative value is hα(i)=Vα(i)−Vα(z)h_\alpha(i)=V_\alpha(i)-V_\alpha(z)hα​(i)=Vα​(i)−Vα​(z). The (SEN) assumptions are: (SEN1) (1−α)Vα(z)(1-\alpha)V_\alpha(z)(1−α)Vα​(z) is bounded on (0,1)(0,1)(0,1); (SEN2) hα≤Mh_\alpha\le Mhα​≤M for a finite function M≥0M\ge0M≥0; (SEN3) hα≥−Lh_\alpha\ge-Lhα​≥−L for a finite constant L≥0L\ge0L≥0. Under (SEN), J=lim⁡α→1−(1−α)Vα(i)J=\lim_{\alpha\to1^-}(1-\alpha)V_\alpha(i)J=limα→1−​(1−α)Vα​(i) is a finite constant, and a limit function hhh is a pointwise limit of hβnh_{\beta_n}hβn​​ along some βn→1−\beta_n\to1^-βn​→1−. The ACOI and ACOE read

J+h(i) ≥ (resp. =) min⁡a∈Ai{C(i,a)+∑jPij(a)h(j)},i∈S.J+h(i)\ \ge\ (\text{resp. }=)\ \min_{a\in A_i}\Big\{C(i,a)+\sum_jP_{ij}(a)h(j)\Big\},\qquad i\in S.J+h(i) ≥ (resp. =) a∈Ai​min​{C(i,a)+j∑​Pij​(a)h(j)},i∈S.

For a nonempty set GGG the first passage time is T=min⁡{n≥1:Xn∈G}T=\min\{n\ge1:X_n\in G\}T=min{n≥1:Xn​∈G}. The class ℜ(i,G)\Re(i,G)ℜ(i,G) consists of the policies that, from iii, enter GGG with probability one in finite expected time miG(θ)m_{iG}(\theta)miG​(θ); ℜ∗(i,G)\Re^*(i,G)ℜ∗(i,G) adds a finite expected first passage cost ciG(θ)=Eθ[∑t<TC(Xt,At)]c_{iG}(\theta)=E_\theta[\sum_{t<T}C(X_t,A_t)]ciG​(θ)=Eθ​[∑t<T​C(Xt​,At​)]. A (randomized) stationary policy ddd is zzz standard if the Markov chain it induces has miz<∞m_{iz}<\inftymiz​<∞ and ciz<∞c_{iz}<\inftyciz​<∞ for every iii; it then has a single positive recurrent class Rd∋zR_d\ni zRd​∋z and a finite constant average cost JdJ_dJd​.

Formalization targets

Goal: Theorem 7.5.6

Assume (BOR): (BOR1) a zzz standard policy ddd exists; (BOR2) for some ε>0\varepsilon>0ε>0 the set D={i:C(i,a)≤Jd+ε for some a}D=\{i: C(i,a)\le J_d+\varepsilon\text{ for some }a\}D={i:C(i,a)≤Jd​+ε for some a} is finite; (BOR3) every i∈D−Rdi\in D-R_di∈D−Rd​ can be reached from zzz by some θi∈ℜ∗(z,i)\theta_i\in\Re^*(z,i)θi​∈ℜ∗(z,i). Then (SEN) holds and every limit function satisfies the ACOE; every average cost optimal stationary policy eee has a positive recurrent state in

D(e)={i:C(i,e)≤J+ε},D(e)=\{i: C(i,e)\le J+\varepsilon\},D(e)={i:C(i,e)≤J+ε},

at most ∣D(e)∣|D(e)|∣D(e)∣ positive recurrent classes and no null recurrent class; and a policy realizing the minimum in the ACOE satisfies e∈ℜ∗(i,D(e)∩R(e))e\in\Re^*(i,D(e)\cap R(e))e∈ℜ∗(i,D(e)∩R(e)) for every iii.

Milestones

  • Lemma 7.4.1: hα(i)≤ciz(θi)h_\alpha(i)\le c_{iz}(\theta_i)hα​(i)≤ciz​(θi​) for θi∈ℜ∗(i,z)\theta_i\in\Re^*(i,z)θi​∈ℜ∗(i,z), hence (SEN2).
  • Lemma 7.4.2: h(i)≤ciG(θ)−JmiG(θ)+Eθ[h(XT)]h(i)\le c_{iG}(\theta)-Jm_{iG}(\theta)+E_\theta[h(X_T)]h(i)≤ciG​(θ)−JmiG​(θ)+Eθ​[h(XT​)] for θ∈ℜ(i,G)\theta\in\Re(i,G)θ∈ℜ(i,G) under an integrability condition.
  • Theorem 7.4.3: four sufficient conditions for equality in the ACOI at a state.
  • Lemma 7.5.2: Jd=(1−α)∑i∈Rπi(d)Vd,α(i)J_d=(1-\alpha)\sum_{i\in R}\pi_i(d)V_{d,\alpha}(i)Jd​=(1−α)∑i∈R​πi​(d)Vd,α​(i) for a zzz standard ddd.
  • Proposition 7.5.3: a zzz standard policy gives (SEN1–2).
  • Corollary 7.5.4: on S={0,1,… }S=\{0,1,\dots\}S={0,1,…}, increasing VαV_\alphaVα​ plus a 000 standard policy gives (SEN), with nonnegative increasing limit functions.
  • Proposition 7.5.5: an optimal stationary policy has a positive recurrent state of cost at most J+εJ+\varepsilonJ+ε, reachable from iii, when (7.33) holds.
  • Corollaries 7.5.9 and 7.5.10: the (CAV) and (CAV*) conditions imply (BOR).

Significance

Theorem 7.5.6 reduces the verification of the ACOE for a queueing model to three checks that do not involve the discount value function: exhibit one stationary policy with finite mean return times and costs to a fixed state (typically a stable "serve at maximal rate" policy), check that low costs occur on a finite set (automatic when the holding cost grows without bound, Corollaries 7.5.9–7.5.10), and check reachability of finitely many states. Its conclusions go beyond existence: optimal stationary policies induce chains with positive recurrent classes located in a known finite set, and ACOE-realizing policies reach them in finite expected time and cost. This is what makes value iteration and approximating-sequence methods in later chapters of the book applicable to these models.

The results are proved in the book. The present mission produces machine-checked statements of the first passage calculus for general (history-dependent, randomized) policies, of (SEN) and limit functions, and of the chain of implications from (CAV*) to the ACOE. No machine-checked version of these statements is known.

Difficulty

The obvious approach to the ACOE is to pass to the limit α→1−\alpha\to1^-α→1− in the discount optimality equation. Exchanging this limit with ∑jPij(a)hα(j)\sum_jP_{ij}(a)h_\alpha(j)∑j​Pij​(a)hα​(j) requires a dominating function, and (SEN2) only gives a pointwise bound MMM whose expectation may be infinite; Fatou's lemma then yields only the inequality. Obtaining equality requires tracking first passages to sets and showing that the discrepancy Φ\PhiΦ vanishes along them, which in turn needs finiteness of ciGc_{iG}ciG​ that is not assumed but has to be derived. On the recurrence side, the average cost criterion is a limit superior of Cesàro averages over a countable state space, and mass can escape to infinity; the finiteness of the set DDD is what prevents an optimal policy from spending its time in transient or null recurrent states, and turning that into positive recurrence requires the renewal-type identities of Appendix C.

Formalization scope

States form a countable type SSS; action sets are nonempty Finsets; costs are in ℝ≥0; transition probabilities are ℝ≥0∞-valued with row sums one on admissible actions. Policies are general: a history is a state sequence and an action sequence, and all probabilities and expectations (hitting probabilities, miGm_{iG}miG​, ciGc_{iG}ciG​, Pθ(XT=j)P_\theta(X_T=j)Pθ​(XT​=j), Qij(n)Q^{(n)}_{ij}Qij(n)​) are computed from the history probabilities of the process. VαV_\alphaVα​, JθJ_\thetaJθ​, miGm_{iG}miG​ and ciGc_{iG}ciG​ take values in [0,∞][0,\infty][0,∞]; miG=∞m_{iG}=\inftymiG​=∞ when GGG is missed with positive probability; the first passage time satisfies T≥1T\ge1T≥1. hαh_\alphahα​ and ∑jPij(a)h(j)\sum_jP_{ij}(a)h(j)∑j​Pij​(a)h(j) are in the extended reals, with the book's convention that a function bounded below has an expectation in (−∞,+∞](-\infty,+\infty](−∞,+∞]. Limit functions are real valued. Positive recurrence, communicating classes and steady state probabilities πj=(mjj)−1\pi_j=(m_{jj})^{-1}πj​=(mjj​)−1 are the notions for the chain induced by a (randomized) stationary policy. JdJ_dJd​ is the average cost of ddd from zzz.

A formalization in which the ACOE is asserted for some convenient function instead of every limit function, or in which ∣D(e)∣|D(e)|∣D(e)∣ is a natural-number cardinality that vanishes on infinite sets, would trivialize part of the goal; the statements quantify over all limit functions and use Set.encard.

A complete development needs: history-dependent policies and their path laws on countable spaces; first passage decompositions (strong Markov property at TTT); Abelian limits of ∑tαtP(T=t)\sum_t\alpha^tP(T=t)∑t​αtP(T=t); Fatou and dominated convergence for series; and the renewal reward theorem for positive recurrent classes (Appendix C of the book). The first passage and Markov chain layer is reusable beyond this mission. Proofs of individual milestones, and sharper statements of the Appendix C facts they use, are welcome.

Selected references

  • L. I. Sennott, Stochastic Dynamic Programming and the Control of Queueing Systems, Wiley Series in Probability and Statistics, John Wiley & Sons, 1999. doi:10.1002/9780470317037
  • V. S. Borkar, "On minimum cost per unit time control of Markov chains", SIAM J. Control Optim. 22 (1984), 965–978.
  • V. S. Borkar, "Control of Markov chains with long-run average cost criterion: the dynamic programming equations", SIAM J. Control Optim. 27 (1989), 642–657.
  • V. S. Borkar, Topics in Controlled Markov Chains, Pitman Research Notes in Mathematics 240, Longman, 1991.
  • R. Cavazos-Cadena, "Weak conditions for the existence of optimal stationary policies in average Markov decision chains with unbounded costs", Kybernetika 25 (1989), 145–156.
  • R. Cavazos-Cadena and L. I. Sennott, "Comparing recent assumptions for the existence of average optimal stationary policies", Oper. Res. Letters 11 (1992), 33–37.
  • L. I. Sennott, "The average cost optimality equation and critical number policies", Prob. Eng. Inform. Sci. 7 (1993).
  • L. I. Sennott, "Average cost optimal stationary policies in infinite state Markov decision processes with unbounded costs", Operations Research 37 (1989), 626–633. doi:10.1287/opre.37.4.626
  • K. L. Chung, Markov Chains with Stationary Transition Probabilities, 2nd ed., Springer, 1967.
15 thms1 active userReviewed
Dynamic ProgrammingOperations ResearchProbability·Captain: mikedeng1

Stochastic Dynamic Programming and the Control of Queueing Systems VI: The (SEN) Assumptions and the Average Cost Optimality InequalityTextbook

Motivation

Queueing control problems (admission control, routing, service-rate selection, flow control) are naturally posed as Markov decision chains with a denumerably infinite state space, such as the number of customers in a buffer, and are usually judged by their long-run average cost per unit time. When the state space is finite, Chapter 6 of Sennott's book shows that an average cost optimal stationary policy always exists. On a countable state space this fails: Section 7.1 of the book gives examples in which no average cost optimal policy exists, and one in which no stationary policy comes within a given distance of the minimum average cost. The question addressed by this mission is under which verifiable conditions on the discounted value functions a countable-state model has a constant minimum average cost and an optimal stationary policy.

Timeline, following the book's bibliographic notes (p. 163). The book names Taylor (1965) and Derman (1966) as earlier pivotal work and Ross (1968), and his 1983 textbook, as the direct predecessor. Sennott (1989, Operations Research 37) weakened Ross's assumptions to cover models with unbounded costs, and proved the main result of Section 7.2; the (SEN) assumptions of Chapter 7 are the cleaner version of Sennott (1993). Cavazos-Cadena (1991) gave the example, adapted as Example 7.3.1 of the book, showing that under these assumptions the optimality inequality can be strict. The weaker (H*) assumptions of Section 7.7 appear, in a slightly different form, in Sennott (1995). Part (iv) of Theorem 7.2.3 is new in the book.

Setting

A Markov decision chain (MDC) Δ\DeltaΔ has a countable state space SSS, for each state iii a finite nonempty action set AiA_iAi​, a nonnegative finite cost C(i,a)C(i,a)C(i,a), and transition probabilities Pij(a)P_{ij}(a)Pij​(a) with ∑jPij(a)=1\sum_j P_{ij}(a) = 1∑j​Pij​(a)=1. A policy θ\thetaθ chooses the action at time nnn at random according to a distribution that may depend on the whole history (X0,A0,…,Xn)(X_0, A_0, \dots, X_n)(X0​,A0​,…,Xn​); a stationary policy fff always chooses f(i)∈Aif(i) \in A_if(i)∈Ai​ in state iii.

For an initial state iii, the nnn-horizon cost is vθ,n(i)=∑t=0n−1Eθ[C(Xt,At)∣X0=i]v_{\theta,n}(i) = \sum_{t=0}^{n-1} E_\theta[C(X_t,A_t) \mid X_0 = i]vθ,n​(i)=∑t=0n−1​Eθ​[C(Xt​,At​)∣X0​=i], the average cost is Jθ(i)=lim sup⁡nvθ,n(i)/nJ_\theta(i) = \limsup_{n} v_{\theta,n}(i)/nJθ​(i)=limsupn​vθ,n​(i)/n, and the minimum average cost is J(i)=inf⁡θJθ(i)J(i) = \inf_\theta J_\theta(i)J(i)=infθ​Jθ​(i) over all policies. A policy is average cost optimal if Jθ≡JJ_\theta \equiv JJθ​≡J. For α∈(0,1)\alpha \in (0,1)α∈(0,1) the discounted value function is Vα(i)=inf⁡θ∑t≥0αtEθ[C(Xt,At)∣X0=i]V_\alpha(i) = \inf_\theta \sum_{t \ge 0} \alpha^t E_\theta[C(X_t,A_t) \mid X_0 = i]Vα​(i)=infθ​∑t≥0​αtEθ​[C(Xt​,At​)∣X0​=i]. All these quantities lie in [0,∞][0,\infty][0,∞].

Fix a distinguished state zzz and put hα(i)=Vα(i)−Vα(z)h_\alpha(i) = V_\alpha(i) - V_\alpha(z)hα​(i)=Vα​(i)−Vα​(z). The (SEN) assumptions are:

  • (SEN1) (1−α)Vα(z)(1-\alpha)V_\alpha(z)(1−α)Vα​(z) is bounded for α∈(0,1)\alpha \in (0,1)α∈(0,1);
  • (SEN2) there is a nonnegative finite function MMM with hα(i)≤M(i)h_\alpha(i) \le M(i)hα​(i)≤M(i) for all iii and α\alphaα;
  • (SEN3) there is a nonnegative finite constant LLL with −L≤hα(i)-L \le h_\alpha(i)−L≤hα​(i) for all iii and α\alphaα.

A limit function hhh is a pointwise limit of hβnh_{\beta_n}hβn​​ along some sequence βn→1−\beta_n \to 1^-βn​→1−. If fαf_\alphafα​ is a stationary policy realizing the discount optimality equation Vα(i)=min⁡a{C(i,a)+α∑jPij(a)Vα(j)}V_\alpha(i) = \min_a \{C(i,a) + \alpha\sum_j P_{ij}(a)V_\alpha(j)\}Vα​(i)=mina​{C(i,a)+α∑j​Pij​(a)Vα​(j)}, a limit point fff is a stationary policy with fβn(i)=f(i)f_{\beta_n}(i) = f(i)fβn​​(i)=f(i) for large nnn, for each iii, along some βn→1−\beta_n \to 1^-βn​→1−.

Formalization targets

Goal: Theorem 7.2.3

Under (SEN), there is a finite constant J=lim⁡α→1−(1−α)Vα(i)J = \lim_{\alpha\to1^-}(1-\alpha)V_\alpha(i)J=limα→1−​(1−α)Vα​(i) independent of iii; limit functions exist, satisfy −L≤h≤M-L \le h \le M−L≤h≤M and the average cost optimality inequality (ACOI)

J+h(i)≥min⁡a∈Ai{C(i,a)+∑jPij(a)h(j)},i∈S;J + h(i) \ge \min_{a \in A_i}\Big\{C(i,a) + \sum_j P_{ij}(a)h(j)\Big\}, \qquad i \in S;J+h(i)≥a∈Ai​min​{C(i,a)+j∑​Pij​(a)h(j)},i∈S;

every stationary policy realizing the minimum is average cost optimal with Je≡JJ_e \equiv JJe​≡J and Ee[h(Xn)]/n→0E_e[h(X_n)]/n \to 0Ee​[h(Xn​)]/n→0; every limit point of discount optimal stationary policies is average cost optimal and satisfies the corresponding inequality for an associated limit function; and the average cost of any optimal policy is a limit, not only a limit supremum.

Milestones

  • Proposition 7.1.1: finitely many initial transitions with finite cost do not change JθJ_\thetaJθ​.
  • Lemma 7.2.1: a bounded-below solution (J,h)(J,h)(J,h) of the ACOI inequality for a stationary eee gives Je≤JJ_e \le JJe​≤J.
  • Proposition B.6: a sequence of functions squeezed between −L-L−L and MMM on a countable set has a pointwise convergent subsequence.
  • Proposition 7.2.4: (SEN) does not depend on the choice of zzz.
  • Proposition 7.7.1: (SEN) ⇒\Rightarrow⇒ (H*) ⇒\Rightarrow⇒ (H).
  • Proposition 7.7.2: the conclusions of Theorem 7.2.3 hold under (H), with a state-dependent lower bound L(i)L(i)L(i).

Significance

Theorem 7.2.3 is the existence theorem the rest of Chapter 7 builds on (p. 128): the ACOE results of Section 7.4, the (BOR) and (CAV) sufficient conditions of Section 7.5, and the worked queueing models of Section 7.6 all work under (SEN) and invoke it. It justifies computing an average cost optimal policy for a queueing model as a limit of discount optimal policies, and it shows that the minimum average cost is the Abelian limit of the normalized discounted value.

The results are proved in the book and in Sennott (1989, 1993, 1995), but none of them has a machine-checked proof: Mathlib has no Markov decision processes, and the platform's average cost results concern finite state spaces or Borel models with different assumptions. The formalization produces a general-policy, countable-state MDC development with extended-real values, reusable by the later missions of this series.

Difficulty

On a finite state space the relative value functions are bounded and the Abelian limit (1−α)Vα(1-\alpha)V_\alpha(1−α)Vα​ can be controlled directly. Here hαh_\alphahα​ is bounded above only by a function MMM that may be unbounded, so passing to the limit in the discounted optimality equation ∑jPij(a)hα(j)\sum_j P_{ij}(a)h_\alpha(j)∑j​Pij​(a)hα​(j) cannot use dominated convergence, and in general only an inequality survives in the limit; Example 7.3.1 shows that the inequality in the ACOI can be strict. Showing that a policy realizing the ACOI is optimal requires control of Ee[h(Xn)]/nE_e[h(X_n)]/nEe​[h(Xn​)]/n for a function hhh that is unbounded above, and part (iv) requires comparing the limit inferior and limit superior of Cesàro averages for an arbitrary, possibly history-dependent optimal policy.

Formalization scope

The state space is any countable type ([Countable S]); actions form a type with finite nonempty Finset action sets; costs are ℝ≥0; transition probabilities, costs over time and value functions are ℝ≥0∞. Policies are general: randomized and history dependent, with histories encoded as finite state and action sequences and the process law built by an explicit recursive product. Finite horizon costs have terminal cost 000, as the chapter prescribes.

The relative value hα(i)=Vα(i)−Vα(z)h_\alpha(i) = V_\alpha(i) - V_\alpha(z)hα​(i)=Vα​(i)−Vα​(z) is computed in EReal, never through a truncated real subtraction: a state with Vα(i)=∞V_\alpha(i) = \inftyVα​(i)=∞ gives hα(i)=+∞h_\alpha(i) = +\inftyhα​(i)=+∞, so (SEN2) cannot hold through a junk value, and (SEN1) is a bound by a finite constant that itself forces Vα(z)<∞V_\alpha(z) < \inftyVα​(z)<∞. Sums ∑jPij(a)h(j)\sum_j P_{ij}(a)h(j)∑j​Pij​(a)h(j) and expectations E[h(Xn)]E[h(X_n)]E[h(Xn​)] of real functions are extended reals, computed as positive part minus negative part; they are never Bochner integrals and never default to 000 when not summable. The limit α→1−\alpha \to 1^-α→1− is the filter 𝓝[<] 1. Limit functions and limit points follow Definition 7.2.2 literally, over arbitrary sequences αn→1−\alpha_n \to 1^-αn​→1− in (0,1)(0,1)(0,1), and the (SEN), (H), (H*) sets are predicates carrying their witnesses MMM and LLL.

A development that bounds only hαh_\alphahα​ as a free function, rather than the one built from the infimum over all policies, or that quantifies only over stationary policies in J(i)J(i)J(i), proves a different and weaker theorem and does not count.

Needed infrastructure: the law of the controlled process under a general policy, monotone and Fatou-type limit interchanges for countable sums, the Abelian inequality lim sup⁡(1−α)∑αtct≤lim sup⁡1n∑t<nct\limsup(1-\alpha)\sum\alpha^t c_t \le \limsup \frac1n\sum_{t<n}c_tlimsup(1−α)∑αtct​≤limsupn1​∑t<n​ct​ (Proposition 6.1.1 of the book), and the existence and optimality of discount optimal stationary policies (Theorem 4.1.4). The MDC layer and these two results are shared with other missions of the series; contributions to them are welcome.

Selected references

  • L. I. Sennott, Stochastic Dynamic Programming and the Control of Queueing Systems, Wiley, 1999, Chapter 7 (pp. 127–166) and Appendix B. https://doi.org/10.1002/9780470317037
  • L. I. Sennott, Average cost optimal stationary policies in infinite state Markov decision processes with unbounded costs, Operations Research 37 (1989) 626–633. https://doi.org/10.1287/opre.37.4.626
  • L. I. Sennott, The average cost optimality equation and critical number policies, Probability in the Engineering and Informational Sciences 7 (1993). (Cited in the book's bibliography, p. 321.)
  • L. I. Sennott, Another set of conditions for average optimality in Markov control processes, Systems & Control Letters 24 (1995) 147–151. (Cited in the book's bibliography.)
  • R. Cavazos-Cadena, A counterexample on the optimality equation in Markov decision chains with the average cost criterion, Systems & Control Letters 16 (1991) 387–392. (Cited in the book's bibliography.)
  • S. M. Ross, Non-discounted denumerable Markovian decision models, Annals of Mathematical Statistics 39 (1968) 412–423. (Cited in the book's bibliography.)
  • H. M. Taylor, Markovian sequential replacement processes, Annals of Mathematical Statistics 36 (1965) 1677–1694. (Cited in the book's bibliography.)
  • E. A. Feinberg and Y. Liang, On the optimality equation for average cost Markov decision processes and its validity for inventory control; formalized on Prove2Me in the mission of the same name (Borel state spaces, a different model).
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Analysis and Algorithms for Service Parts Supply Chains VII: Palm's Theorem for Nonstationary DemandTextbook

Motivation

Spare-parts inventory models for repairable items rest on Palm's theorem: if demands arrive as a Poisson process with constant rate λ\lambdaλ and each demanded unit spends an independent, identically distributed resupply time with mean τˉ\bar\tauτˉ in the pipeline, the number of units in resupply is Poisson with mean λτˉ\lambda\bar\tauλτˉ in steady state. Stock levels, backorders and fill rates are all computed from that distribution.

Both assumptions fail in practice. Military flying programmes ramp up and down within weeks, repair shops close for periods, and commercial parts distribution centres see demand that varies by day of the week. Chapter 9 of Muckstadt's Analysis and Algorithms for Service Parts Supply Chains (Springer 2005, DOI 10.1007/b138879) extends Palm's theorem to a nonstationary Poisson demand process with time-dependent resupply-time distributions, gives the compound (multi-unit order) version, and uses the result to compute, at any time ttt, the distribution of units in repair at the depot of a two-echelon system.

Timeline: Palm (1938) proved the stationary result for telephone traffic; Feeney and Sherbrooke (1966) extended it to compound Poisson demand; Hillestad and Carrillo (RAND, 1980) and Crawford (RAND, 1981) developed the time-dependent extensions, summarized by Carrillo (RAND, 1989). The chapter presents these results.

Setting

A single item is stocked at one location, and every demand is for one unit.

  • Demand rate λ(s)≥0\lambda(s) \ge 0λ(s)≥0, integrable on bounded intervals, with mean function m(t)=∫0tλ(s) dsm(t) = \int_0^t \lambda(s)\,dsm(t)=∫0t​λ(s)ds.
  • Demand process: a nonstationary Poisson process with mean function mmm, with N(0)=0N(0) = 0N(0)=0. N(t)N(t)N(t) counts demands in [0,t][0,t][0,t] and T0<T1<⋯T_0 < T_1 < \cdotsT0​<T1​<⋯ are the demand epochs.
  • Resupply times: a unit demanded at time sss is resupplied within www time units with probability Gs(w)G_s(w)Gs​(w). Resupply times are nonnegative, have finite expectations, are independent from unit to unit, and are independent of the demand process.
  • X(t)X(t)X(t) is the number of units in resupply at time ttt: demands in [0,t][0,t][0,t] whose resupply is not complete at ttt.

The mean of X(t)X(t)X(t) is

α(t)=∫0t(1−Gs(t−s))λ(s) ds.\alpha(t) = \int_0^t \bigl(1 - G_s(t-s)\bigr)\lambda(s)\,ds.α(t)=∫0t​(1−Gs​(t−s))λ(s)ds.

In the compound version (Section 9.2), orders arrive as above and each order is for Q≥1Q \ge 1Q≥1 units, with a time-stationary law uj=P(Q=j)u_j = P(Q = j)uj​=P(Q=j). All units of an order share its resupply time, Y(t)Y(t)Y(t) counts units demanded in [0,t][0,t][0,t], and uk(n)u^{(n)}_kuk(n)​ is the nnn-fold convolution of (uj)(u_j)(uj​).

In the two-echelon version (Section 9.3), base iii has failure rate λi\lambda_iλi​. A failure is repaired at the base with probability rir_iri​ and at the depot otherwise. Depot repair of a failure occurring at time uuu takes a deterministic time D(u)D(u)D(u) with D(t)+t≥D(s)+sD(t) + t \ge D(s) + sD(t)+t≥D(s)+s for s<ts < ts<t (no crossing). Write t~=inf⁡{u≥0:D(u)+u>t}\tilde t = \inf\{u \ge 0 : D(u) + u > t\}t~=inf{u≥0:D(u)+u>t}.

Formalization targets

Goal: Theorem 13 (p. 216)

For every t≥0t \ge 0t≥0,

P{X(t)=k}=e−α(t)α(t)kk!,k=0,1,2,…P\{X(t) = k\} = e^{-\alpha(t)}\frac{\alpha(t)^k}{k!}, \qquad k = 0,1,2,\dotsP{X(t)=k}=e−α(t)k!α(t)k​,k=0,1,2,…

This is an exact statement at each finite time, not a limit. With constant λ\lambdaλ and Gs=GG_s = GGs​=G it reduces to the finite-time step of Palm's theorem.

Milestones

  1. E[N(t)]=m(t)E[N(t)] = m(t)E[N(t)]=m(t) (Section 9.1, p. 216).
  2. Theorem 12 (p. 216): given N(t)=nN(t) = nN(t)=n, the epochs T0,…,Tn−1T_0, \dots, T_{n-1}T0​,…,Tn−1​ are distributed as the order statistics of nnn i.i.d. variables with distribution function F(x)=m(x)/m(t)F(x) = m(x)/m(t)F(x)=m(x)/m(t) on [0,t)[0,t)[0,t).
  3. The binomial step of the proof of Theorem 13 (pp. 216–217): P{X(t)=k∣N(t)=n}=(nk)pk(1−p)n−kP\{X(t) = k \mid N(t) = n\} = \binom nk p^k(1-p)^{n-k}P{X(t)=k∣N(t)=n}=(kn​)pk(1−p)n−k, with p=∫0t(1−Gs(t−s))λ(s)/m(t) dsp = \int_0^t (1 - G_s(t-s))\lambda(s)/m(t)\,dsp=∫0t​(1−Gs​(t−s))λ(s)/m(t)ds.
  4. Section 9.2 (p. 218): E[Y(t)]=m(t)E[Q]E[Y(t)] = m(t)E[Q]E[Y(t)]=m(t)E[Q] and Var⁡[Y(t)]=m(t)E[Q2]\operatorname{Var}[Y(t)] = m(t)E[Q^2]Var[Y(t)]=m(t)E[Q2].
  5. Theorem 14 (p. 218): P[X(t)=k]=∑n≥1uk(n)e−α(t)α(t)n/n!P[X(t) = k] = \sum_{n\ge1} u^{(n)}_k e^{-\alpha(t)}\alpha(t)^n/n!P[X(t)=k]=∑n≥1​uk(n)​e−α(t)α(t)n/n! for k≥1k \ge 1k≥1, and e−α(t)e^{-\alpha(t)}e−α(t) at k=0k = 0k=0.
  6. Section 9.3.2 (p. 221): P{X0(t)=k}=e−m0(t~,t)m0(t~,t)k/k!P\{X_0(t) = k\} = e^{-m_0(\tilde t,t)} m_0(\tilde t,t)^k/k!P{X0​(t)=k}=e−m0​(t~,t)m0​(t~,t)k/k! with m0(t~,t)=∫t~t∑iλi(u)(1−ri) dum_0(\tilde t,t) = \int_{\tilde t}^t \sum_i \lambda_i(u)(1-r_i)\,dum0​(t~,t)=∫t~t​∑i​λi​(u)(1−ri​)du.

A plain supporting item states that N(t)N(t)N(t) is Poisson with mean m(t)m(t)m(t), the factor the proof of Theorem 13 uses.

Significance

Theorem 13 gives the full distribution of the pipeline at every instant. Time-dependent expected backorders, ∑x>s(t)(x−s(t))P{X(t)=x}\sum_{x > s(t)} (x - s(t)) P\{X(t) = x\}∑x>s(t)​(x−s(t))P{X(t)=x}, and fill rates P{X(t)<s(t)}P\{X(t) < s(t)\}P{X(t)<s(t)} follow from it, so stock levels can be planned against a surge or a repair outage without a steady-state approximation. Theorem 14 does the same for multi-unit orders. The depot result feeds the base-level convolution of Section 9.3.3, which in turn gives time-dependent performance measures for a two-echelon system.

These results are proved in the literature, and the chapter reproduces the proofs of Theorems 13 and 14. It cites Theorem 12 without proof ("similar to the one given in Chapter 3"). No machine-checked version of any of them is known, and neither Mathlib nor this platform has a Poisson process, stationary or not, a thinning theorem, or an order-statistics theorem. The formal content of this mission therefore includes the construction and the first distributional facts of the nonstationary Poisson process.

Difficulty

The algebra of the proof is a Poisson mixture of binomials and is short. The difficulty is Theorem 12 and its use. The obvious argument treats "the nnn demands in [0,t][0,t][0,t]" as nnn independent draws from FFF and assigns each an independent resupply time with law GdrawG_{\text{draw}}Gdraw​. Making this rigorous requires identifying the conditional joint law of the epochs given N(t)=nN(t) = nN(t)=n. The resupply time of the jjj-th demand is not independent of its epoch: its law depends on the epoch. So it must be shown that, after conditioning, the marks attached to sorted epochs behave like marks attached to unsorted i.i.d. draws. The book's constant-rate argument (Chapter 3) uses the uniform density n!/tnn!/t^nn!/tn on the simplex. Here the density involves λ\lambdaλ, which may vanish on intervals, and mmm need not be invertible.

Formalization scope

  • Demand process. The nonstationary Poisson process is constructed, not postulated. With i.i.d. exponential(1) gaps and unit-rate points Γk=A0+⋯+Ak\Gamma_k = A_0 + \cdots + A_kΓk​=A0​+⋯+Ak​, the kkk-th demand occurs at Tk=inf⁡{s≥0:m(s)≥Γk}T_k = \inf\{s \ge 0 : m(s) \ge \Gamma_k\}Tk​=inf{s≥0:m(s)≥Γk​}, and N(t)=#{k:Γk≤m(t)}N(t) = \#\{k : \Gamma_k \le m(t)\}N(t)=#{k:Γk​≤m(t)}.
  • Resupply times. Resupply times are ρ(Tk,Uk)\rho(T_k, U_k)ρ(Tk​,Uk​) for a jointly measurable ρ≥0\rho \ge 0ρ≥0 and i.i.d. marks UkU_kUk​ independent of the gaps, with Gs(w)=ν{ρ(s,⋅)≤w}G_s(w) = \nu\{\rho(s,\cdot) \le w\}Gs​(w)=ν{ρ(s,⋅)≤w}. Every measurable family GsG_sGs​ arises this way, and joint measurability makes α(t)\alpha(t)α(t) a genuine integral. Independence of resupply times from the demand process is not written in Theorem 12 or 13 but is used in the proof; it is part of the model.
  • Pinnings and conventions.
    • "λ\lambdaλ integrable" is read as integrable on bounded intervals.
    • Time is t≥0t \ge 0t≥0.
    • Theorem 12 assumes m(t)>0m(t) > 0m(t)>0, since FFF is 0/00/00/0 otherwise, and sets F=0F = 0F=0 on (−∞,0)(-\infty,0)(−∞,0).
    • Conditional probabilities are written as joint probabilities.
    • E[Y(t)]E[Y(t)]E[Y(t)] is stated in [0,∞][0,\infty][0,∞]; the variance identity assumes E[Q2]<∞E[Q^2] < \inftyE[Q2]<∞.
    • t~\tilde tt~ is an infimum over u≥0u \ge 0u≥0, and D≥0D \ge 0D≥0.
    • Counts are cardinalities, and are 000 on the null event where they would be infinite.
  • Corrections. Theorem 14's printed sum starts at n=1n = 1n=1, which gives P[X(t)=0]=0P[X(t) = 0] = 0P[X(t)=0]=0. The statement keeps the book's formula for k≥1k \ge 1k≥1 and adds P[X(t)=0]=e−α(t)P[X(t) = 0] = e^{-\alpha(t)}P[X(t)=0]=e−α(t). The depot's Poisson demand stream with rate ∑iλi(1−ri)\sum_i \lambda_i(1-r_i)∑i​λi​(1−ri​) is generated from the bases' processes and independent repair-location choices, not assumed.
  • Not stated.
    • Eqs. (9.1)–(9.2), the FCFS depot backorders owed to base iii: the derivation on p. 221 is informal, and (9.1) prints the exponent s0(t−1)s_0(t-1)s0​(t−1) for s0(t)−1s_0(t)-1s0​(t)−1.
    • The base analysis of Section 9.3.3.
    • The compound law of Y(t)Y(t)Y(t) on p. 217, which has the same n=0n = 0n=0 omission.
  • Trivialization ruled out. X(t)X(t)X(t) is computed from the demand epochs and resupply times, not defined by its law, and resupply times cannot depend on the demand epochs except through the prescribed GsG_sGs​. Either shortcut would make the goal empty or false.
  • Infrastructure. The time-changed Poisson construction, its count law, the order-statistics property and marked thinning are reusable well beyond this chapter: in queueing (Mt/Gt/∞M_t/G_t/\inftyMt​/Gt​/∞), in reliability, and in the stationary Palm mission of this series. Contributions of these general lemmas are welcome.

Selected references

  • J. A. Muckstadt, Analysis and Algorithms for Service Parts Supply Chains, Springer, 2005, Chapter 9, pp. 215–222. https://doi.org/10.1007/b138879
  • C. Palm, "Analysis of the Erlang traffic formulae for busy-signal arrangements", Ericsson Technics 5, 1938, 39–58.
  • G. J. Feeney and C. C. Sherbrooke, "The (s−1, s) inventory policy under compound Poisson demand", Management Science 12(5), 1966, 391–411. https://doi.org/10.1287/mnsc.12.5.391
  • R. J. Hillestad and M. J. Carrillo, Models and techniques for recoverable item stockage when demand and the repair processes are nonstationary — Part I: Performance measurement, Report N-1482-AF, RAND Corporation, 1980.
  • G. B. Crawford, Palm's theorem for nonstationary processes, Report R-2750-RC, RAND Corporation, 1981.
  • M. J. Carrillo, Generalizations of Palm's theorem and Dyna-METRIC's demand and pipeline variability, Report R-3698-AF, RAND Corporation, 1989.
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Elements of Queueing Theory V: Strassen's Theorems and the Stochastic Ordering of QueuesTextbook

Strassen's Theorems and the Stochastic Ordering of Queues

Background

Chapters 1–3 of Baccelli and Brémaud's Elements of Queueing Theory compute exact quantities: Palm identities, stability criteria, PASTA, Pollaczek–Khinchin. Chapter 4 asks a different question. When you cannot compute a queue, can you at least say it is better than another one?

That requires an order on distributions. The chapter builds a family of them — integral orders — by choosing a class ℒ of test functions and declaring F ≤_ℒ G when ∫f dF ≤ ∫f dG for all f ∈ ℒ. Three matter: {i} the non-decreasing functions, giving the strong (stochastic) order; {cx} the convex functions, giving the convex order; and their intersection {icx}.

The goal

An integral order compares two distributions that need not live on the same probability space, and that is both its convenience and its difficulty. Strassen's theorems say each of these orders is secretly a statement about a coupling.

Theorem 4.2.2 (p.278), Strassen's ≤_cx theorem:

F ≤_cx G   ⟺   ∃ X ~ F, Y ~ G on one space with  E[Y | X] = X  a.s.
F ≤_icx G  ⟺   the same with  E[Y | X] ≥ X  a.s.

The convex order holds exactly when G is a martingale dilation of F — obtained by spreading each point out without moving its conditional mean. That is what makes the order usable: comparison results for queues become induction arguments on a coupling instead of analytic manipulations of convolutions of c.d.f.'s.

Its companion Theorem 4.2.1 is the ≤_st version, where the coupling is the simpler X ≤ Y a.s. In dimension one both are explicit — take X = F⁻¹(U), Y = G⁻¹(U) for a uniform U. In dimension n there is no such formula, and that is why these are Strassen's theorems. The book attributes both to Strassen (1965) and proves neither.

Why FIFO is optimal

§4.1 is a different kind of comparison: not between two queues, but between two service disciplines for the same queue. The order there is majorization ≺, which compares how spread out two vectors of the same total are.

The answer is that FIFO minimizes E⁰[f(V)] for every convex f (Property 4.1.3), and the proof is an interchange argument. Under any non-preemptive discipline that uses no information on the service times, customer k effectively receives service σ_{γ(k)} for some permutation γ; Lemma 4.1.3 shows the same queue is produced by FIFO fed with that reordered input, and that the reordering does not change the law of the input. Lemma 4.1.4 passes to the limit, which needs ρ < 1. Lemmas 4.1.1 and 4.1.2 then do the combinatorics: undoing one inversion of γ makes the waiting-time vector less spread out, so the identity permutation — FIFO — is extremal.

Feller's paradox, and what survives it

§4.4 compares time-stationary queues, and opens with a warning. T_n[P⁰] ≤_i T̃_n[P̃⁰] for every n does not imply T_n[P] ≤_i T̃_n[P̃]: Example 4.4.1, "Feller's paradox revisited", exhibits a Poisson process and a renewal process where the Palm order holds and the stationary one fails. The order does not pass from the Palm probability to the stationary one.

For ≤_cx it does. Lemma 4.4.1 is why: it expands E_P[f(N[0,x))] as a series of second differences of f against Palm expectations, and a convex f makes every coefficient non-negative. Lemma 4.4.2 handles the S-orders, built by dividing Palm integrals by the mean cycle length, and shows that the normalisation does not hide the comparison it normalises by.

Formalization scope

  • Orders. ≤_i, ≤_cx, ≤_icx on distributions on ℝⁿ are integral orders over the book's test classes (§4.2.1), with the page's qualification that only test functions with well-defined integrals count. Majorization ≺ is (4.1.2) with increasing reorderings of both vectors.
  • Strassen. Both theorems are stated as equivalences, with the coupling existential over the probability space. Theorem 4.2.2 carries both clauses — E[Y | X] = X for ≤_cx, E[Y | X] ≥ X for ≤_icx, as conditional expectations given σ(X) — and assumes both distributions integrable; Theorem 4.2.1 has no integrability hypothesis. A one-directional statement (the Jensen half) is not the theorem.
  • The queue of §4.1.3 is constructed: a GI/GI input (i.i.d. inter-arrival and service times, independent), a single work-conserving server started empty, and any non-preemptive discipline whose choices are measurable in the information the book's σ-field 𝒢_t carries (arrivals, service times of customers already started) plus external randomisation. FIFO is one such discipline. The interchange permutations γ_n and their limit γ are built from the schedule as on pp.268–270; Lemma 4.1.4 assumes ρ = E[σ₀]/E[τ₀] < 1.
  • Lemma 4.4.1 is stated with the exact second-difference series and assumes that series converges absolutely; the page states it for all f, which fails for heavy-tailed counts and sparse f.
  • The S-orders test against {I-ℒ} — primitives ∫_0^t f(u, x) du of test functions — and apply only to distributions whose first coordinate is a.s. positive with a finite mean.

What this mission provides

None of it exists. Mathlib has no stochastic order, no convex order, no increasing-convex order, no majorization, no Schur-convexity and no Strassen theorem; the platform returns zero hits for q=stochastic ordering. Everything in this chapter is new substrate — and §§4.1–4.2 need nothing from Palm calculus, so this mission can be read on its own.

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Elements of Queueing Theory IV: PASTA and the Formulas of Palm CalculusTextbook

PASTA and the Formulas of Palm Calculus

Background

Chapter 1 of Baccelli and Brémaud's Elements of Queueing Theory builds Palm calculus. Chapter 2 settles when a queue has a stationary regime. Chapter 3 is called simply Formulas, and it is what the first two chapters were for: it computes.

The pattern is always the same. A quantity of interest is observed two ways — from a clock fixed in time, and from an arriving customer — and Palm calculus converts between them. Little's law, the Pollaczek–Khinchin formula and the rate conservation principle are all instances.

The goal

Theorem 3.3.1 (p.211) is the one that says when the two views coincide.

This classical result of queueing theory states, in rough terms, that if the arrival point process is Poisson, operational characteristics of the system computed just before arrival times and at arbitrary times are the same (Poisson Arrivals See Time Averages). Some care must be exercised in the application of this principle, and we now give a precise statement, in the θ_t-framework.

E⁰_A[f(Z(0))] = E[f(Z(0))]                                                            (3.3.1)

for every F_t-predictable, flow-compatible {Z(t)} and every non-negative measurable f, whenever A admits the constant F_t-intensity λ; and, under ergodicity,

lim_N (1/N) Σ_{n=1}^N f(Z(T_n)) = lim_T (1/T) ∫_0^T f(Z(s)) ds .                       (3.3.2)

The "some care" is the word predictable. PASTA is false without it: an arrival that changes the state it then observes does not see the time average, and that is exactly what predictability — measurability for the F_t-predictable σ-field, generated by the sets (a,b] × A with A ∈ F_a — rules out.

The hypothesis is the constant F_t-intensity, not "A is Poisson". By Watanabe's theorem the two are equivalent, but that equivalence is a remark on the page and not part of this theorem.

Why it earns its place: Pollaczek–Khinchin

§3.4 derives formulas from conservation equations. Applying the rate conservation principle of Chapter 1 to Y(t) = e^{iuW(t)} in a GI/GI/1/∞ queue gives Takács' formula

iu E[e^{iuW(0)}] = λ E⁰_A[e^{iuW(0−)}] (E[e^{iuσ_0}] − 1) + iu(1 − ρ) ,                (3.4.44)

an identity between a stationary expectation and a Palm expectation of the workload just before an arrival. One substitution turns it into a closed form — and that substitution is PASTA. When the arrivals are Poisson, E⁰_A[e^{iuW(0−)}] = E[e^{iuW(0)}], and

E[e^{iuW(0)}] = iu(1 − ρ) / ( iu − λ(Ψ_σ(u) − 1) ) ,                                   (3.4.45)

the Pollaczek–Khinchin characteristic function formula. The most quoted formula in single-server queueing theory is one application of this mission's goal theorem.

The rest of the chapter

§3.1 carries Little's formula to fluid queues. Lemma 3.1.1 is the set identity that turns the fluid workload into an integral against the arrival measure — the same two instants described from the server's side and from the arrivals' side.

§3.2 applies Campbell's formula to rare events. Lemma 3.2.1 gives a closed form, in a countable-state Markov chain, for the mean time to make an excursion to a rare set and return; its two expressions count the same cycle rate from the two ends. Theorem 3.2.1 generalizes Keilson's asymptotic equivalence to a stationary θ_t-compatible process, replacing cycles by thinnings of the entrance processes of two disjoint sets.

§3.5 applies the stochastic intensity integration formula to a superposition of on-off fluid sources. Lemma 3.5.1 identifies a conditional expectation with a Palm expectation through Papangelou's theorem — the mean workload while a source is idle equals the mean workload that source sees when it wakes. Lemma 3.5.2 measures the gap between the two Palm expectations of the workload taken with respect to a source's start process and its fluid process.

What this mission provides

Nothing here is on the platform or in Mathlib. The nearest platform item, queueing_general_littles_law, is Stidham's deterministic sample-path law; its own docstring disclaims probability, expectation, stationarity, ergodicity and FIFO. Baccelli's L = λW is the Palm identity for a stationary ergodic marked point process, derived from the inversion formula (1.2.25) — an identity between an expectation under P and a Palm expectation under P⁰_N, not a pathwise limit. Different framework, different hypotheses, and neither implies the other.

Mathlib has filtrations and adapted processes but no predictability in the form this chapter needs, and no stochastic intensity.

Formalization scope

  • PASTA carries both displays. (3.3.1) is an equality in [0, ∞] for every non-negative measurable f. (3.3.2) asserts that, P-almost surely, both averages converge in [0, ∞] to one common limit, so both limits exist. Predictability is measurability for the predictable σ-field P(F_t) of p.55. The concrete form Z(t,ω) = v(t, θ_t ω) of (1.8.1) is not used as the hypothesis, because for a general history it is strictly weaker. The hypothesis is the constant F_t-intensity, E[A(a,b] | F_a] = λ(b − a), and not "A is Poisson".
  • Takács (3.4.44) and Pollaczek–Khinchin (3.4.45) are stated for every real u, and for u ≠ 0 respectively. Their hypotheses are the page's: σ_n is independent of W(T_n−) under P⁰_A, E⁰_A[e^{iuσ_0}] = E[e^{iuσ_0}], P(W(0) = 0) = 1 − ρ, and ρ < 1. The workload is a measurable, flow-compatible solution of Lindley's equation. (3.4.45) adds PASTA's hypotheses for {W(t−)}, and it asserts that its denominator is non-zero.
  • Lemma 3.2.1 asserts both closed forms of E_α R. The chain is irreducible, F is non-empty, and hitting times are counted from time 0.
  • Theorem 3.2.1 asserts the equality in (3.2.43), the convergence to 1, and E⁰_{F_n(→A)}[τ(F_n)] · Λ_n → 1. Its hypotheses are the section's standing ones: P is flow-invariant, {X(t)} is flow-compatible, and A and every F_n are regular and disjoint.
  • Lemmas 3.5.1 and 3.5.2 are stated for the full on-off model of §3.5.3. The on-off point processes are independent, their on periods, off periods and fluid functions are i.i.d. and independent, P⁰_{A^i} is the Palm probability of the random measure A^i, and the workload is the stationary solution of the fluid-queue equation. Lemma 3.5.1 is an identity in [0, ∞]. Lemma 3.5.2 assumes that E⁰_{A^i}[W(0)] and the expectation defining C_i are finite.

A formalization that makes Palm probability an opaque measure with the formulas as axioms, or that weakens predictability to adaptedness, trivializes this mission or makes it false, and is out of scope.

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Elements of Queueing Theory III: Stationary Regimes of Stochastic RecurrencesTextbook

Stationary Regimes of Stochastic Recurrences

Background

Chapter 2 of Baccelli and Brémaud's Elements of Queueing Theory asks when a queue has a stationary regime. §§2.1–2.4 answer it for the single-server and multiserver queues by Loynes' monotone construction. §§2.5 and 2.11 answer it for the general object those constructions are instances of: a stochastic recurrence

W_{n+1} = h(W_n, ξ_n),

driven by a sequence {ξ_n} compatible with an ergodic shift θ. Two questions arise, and this mission is about both.

Exact sampling, and what "exact" means

§2.5.3 treats the finite-state case. An ergodic transition matrix on E = {1, …, r} has a stationary law π, and the classical way to sample it is to run the chain and wait. That gives a sample whose law converges to π and is never equal to it.

Coupling from the past (Propp and Wilson, 1996) does better. Run one chain from every state, all sharing a single array {ξ_k(i)} of i.i.d. uniforms indexed by time and current state, started further and further in the past. Once two chains meet they stay together, so eventually all r coalesce before time 0 — and Theorem 2.5.1 says the common value they reach has the distribution π exactly. Theorem 2.5.2 makes it practical: if the updating function preserves a partial order with a least and a greatest state, and a single uniform sequence drives every chain, the two extremal chains funnel all the others and their coalescence suffices.

Neither theorem is a statement about a program. Each says that a random variable is almost surely finite, and that another has a distribution equal to π.

Renovating events: sufficient, and then necessary

§2.5.4 treats the general case, through Borovkov's idea. An event A_n is renovating of length m when, on it, W_{n+m} = Φ(ξ_n, …, ξ_{n+m-1}) — the sequence's value m steps ahead forgets where it came from. Theorem 2.5.3 turns a condition on how often renovating events occur into the existence of a finite stationary solution Z with Z ∘ θ = h(Z, ξ), and into strong backwards coupling: W_n ∘ θ^{-n} is not merely convergent to Z but equal to it after a finite random index.

Corollary 2.5.1 makes the limit independent of the initial condition — one stationary regime, reached from every starting point. Theorem 2.5.4 is the converse: for ℝ₊^K-valued recurrences with a constant initial condition, strong backwards coupling produces renovating events. So the method characterises stability rather than merely detecting it.

The saturation rule

§2.11 treats the multidimensional case, where the state is a vector and the natural models are monotone and homogeneous. Theorem 2.11.1, due to Crandall and Tartar, is the key that unlocks it: under homogeneity, monotone and non-expansive are the same property. That is what puts these models within reach of Kingman's subadditive ergodic theorem, and Theorem 2.11.2 collects the payoff — asymptotic growth rates γ̄ and γ_ exist, both almost surely and in L¹, and do not depend on the initial condition.

The goal

Queueing folklore has a rule of thumb for the stability of an open network: saturate the queues fed by the external stream, measure the departure intensity µ of the saturated system, and declare the network stable when λ < µ. The book is careful that this saturation rule "does not hold for all systems".

Theorem 2.11.3 (p.166), "the main result on the stability region", proves it for Monotone-Homogeneous-Separable networks:

If lim Z_{[-n,0]} → ∞ a.s., then λ γ(0) ≥ 1.    If λ γ(0) > 1, then lim Z_{[-n,0]} → ∞ a.s.

Here γ(c) is the growth rate of the network fed by the scaled process cN, so c = 0 places every arrival at the origin: γ(0) is exactly the saturated system's rate, and µ = γ(0)⁻¹.

Two implications, with a gap between ≥ 1 and > 1 that the book leaves open — as it leaves open the critical case ρ = 1 of Loynes' theorem. Closing it would assert more than is proved.

What this mission provides

Nothing here is on the platform or in Mathlib. There is no coupling from the past, no theory of renovating events, and no Crandall–Tartar theorem. Order/Hom/* has monotone maps and Topology/MetricSpace/* has LipschitzWith 1, which is the right ambient notion for non-expansiveness in the sup-norm, but the equivalence between them under homogeneity is absent.

Formalization scope

  • The standing assumptions of §2.5.1 (p.104) are part of every §2.5.4 statement: (P⁰, θ) is ergodic and {ξ_n} is compatible with θ. The relation Z ∘ θ = h(Z, ξ) holds P⁰-a.s.
  • Theorem 2.5.4 is stated for {W_n^{[C]}}, the sequence its proof on p.119 builds the renovating events for. The page prints {W_n^{[0]}} in the conclusion, and that version is false. Corollary 2.5.1 uses the renovating condition of (2.5.14), W_{n+m} = Φ(ξ_n, …, ξ_{n+m-1}), where the page prints W_n.
  • Theorem 2.11.2 carries all four limits, a.s. and in expectation, for every integrable ℝ^K-valued random initial condition Y, under the book's linear lower bound E[X_n^{[0]}] > −Cn.
  • The goal is stated on the Palm space of a stationary ergodic marked point process: T_0 = 0, T_n ∘ θ = T_{n+1} − T_1, ξ_n ∘ θ = ξ_{n+1}, E⁰τ_n = λ^{-1}, E⁰Z_n < ∞. The map X satisfies (2.11.16) (it depends only on the points and marks in the index window) and the four framework assumptions for every point process. γ(0) is the a.s. limit of Z_{[-n,-1]}(0·N)/n. Dropping the marks would reduce the theorem to deterministic service, and dropping the link between the points and θ makes the second implication false. Neither is done.
  • Stating only one of the goal's two implications, or collapsing them into an equivalence, would be a different theorem. Both implications are stated, with the gap between ≥ 1 and > 1 left open.
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Elements of Queueing Theory II: The Loynes Stability Theorem and CouplingTextbook

The Loynes Stability Theorem and Coupling

Background

Chapter 1 of Baccelli and Brémaud's Elements of Queueing Theory builds a calculus for stationary queues. Chapter 2 asks the prior question: when is there a stationary queue at all?

The G/G/1/∞ queue is one server at unit rate, infinite waiting room, fed by a stationary marked point process {(T_n, σ_n)} — arrival epochs and required service times. Its workload W(t), the service still owed by the server, obeys Lindley's equation between arrivals:

W(t) = (W(T_n−) + σ_n − (t − T_n))⁺,    t ∈ [T_n, T_{n+1}).                          (2.1.6)

Nothing in that equation says a solution exists on the whole line, let alone a stationary one. The answer is a sharp criterion in the traffic intensity ρ = λE⁰_A[σ_0].

The goal

Theorem 2.1.1 (p.80), which the book calls "the fundamental result of stability". Under ρ < 1 there is a unique finite workload process on all of ℝ, compatible with the flow, and it is given explicitly by the Loynes supremum

W(0) = sup_{n ≤ 0} ( T_n + Σ_{i=n}^{0} σ_i )⁺ ,                                      (2.1.12)

with W(T_n−) = 0 for infinitely many negative and infinitely many positive n (2.1.13). If ρ > 1 there is no finite stationary workload process at all.

Each half earns its place. The supremum is what "the Loynes construction" means: look back from the origin, take the work brought by customers n, …, 0 less the time −T_n since elapsed, and maximise over how far back you look. The ρ > 1 half is what turns ρ < 1 from a sufficient condition into a criterion. The critical case ρ = 1 is an explicit non-result in the book — there "may or may not" be a stationary workload — and is deliberately absent from the statement.

The route, and what it produces on the way

§2.2 proves the theorem by Loynes' monotone scheme on the Palm space, and two of its steps are worth stating in their own right.

Lemma 2.2.1 (p.87) is the uniqueness engine: a non-negative, a.s. finite Z with Z − Z∘θ ∈ L¹(P⁰) has E⁰[Z − Z∘θ] = 0. Applied to the difference of two stationary solutions, it forces that difference to be invariant, and ergodicity then forces it to be zero.

Theorem 2.2.1 (p.90) runs the argument backwards. Its section is titled "Queueing Proof of the Ergodic Theorem", and it is exactly that: the queueing construction yields the pointwise ergodic theorem, in the ratio form

lim_n ( Σ_{i=0}^n σ∘θ^{-i} ) / ( Σ_{i=0}^n τ∘θ^{-i} ) = E⁰[σ]/E⁰[τ],    P⁰-a.s.

Mathlib has the mean (von Neumann) ergodic theorem and no pointwise one, so this is absent substrate rather than a restatement.

Three extensions

The multiserver queue (§2.3). With s servers and the least-loaded-server rule, the state is the ordered workload vector obeying the Kiefer–Wolfowitz recurrence, and the criterion becomes E⁰[σ] < s E⁰[τ] (Theorem 2.3.1, p.93). Here uniqueness fails: p.94 exhibits a two-point space with a whole interval of stationary solutions. What survives is that the solution set is bracketed — M_∞ is minimal, and V^∞_∞ is the largest finite solution (Theorem 2.3.2, p.95).

Coupling (§2.4). Theorem 2.4.1 (p.99) is what "reaches the stationary regime" means: if a sequence couples with a θ-compatible one, then the law of its whole shifted trajectory converges in variation to the stationary trajectory's. The proof is one inequality, |P̃_{X,k} − P̃_{Z,k}| ≤ P(N > k), and the finiteness of the coupling time.

The fluid queue (§2.7). Theorem 2.7.1 (p.131) replaces customers by two θ_t-compatible random measures, the arrivals A and the service capacity C, and recovers the Loynes supremum W(t) = sup_{u ≤ t}(A_{u,t} − C_{u,t}) under λ < µ — as the minimal solution, the book claiming no uniqueness here.

Formalization scope

  • ρ = λE⁰_A[σ_0] takes values in [0, ∞], so an input with E⁰_A[σ_0] = ∞ has ρ = ∞ and falls under the non-existence half rather than being read as ρ = 0.
  • The explicit formulas are carried: the Loynes supremum (2.1.12) with the boundedness of its set as a conclusion, the construction points (2.1.13), the ratio limit E⁰[σ]/E⁰[τ] of Theorem 2.2.1, the threshold s E⁰[τ] of Theorem 2.3.1, and the fluid supremum (2.7.7).
  • Identities between random variables hold almost surely, as in the book: the workload equations, (2.1.12)–(2.1.13), (2.7.7), and the solutions of (2.3.2). A statement "for every sample point" would be false, because on a null invariant set of sample paths no finite solution exists.
  • Uniqueness in Theorem 2.1.1 is among measurable, θ_t-compatible workload processes; maximality in Theorem 2.3.2 is among measurable finite solutions; the coupling time of Theorem 2.4.1 is a random variable. A formalization that dropped the explicit supremum, or the ρ > 1 half, would trivialize the goal and is ruled out.

What this mission provides

None of it is on the platform or in Mathlib. The nearest platform item, single_server_queueing_convergence_of_subcritical, presupposes a stationary workload and proves two-time finite-dimensional convergence to it; Theorem 2.1.1 constructs that workload, proves it unique, gives it in closed form, and adds the non-existence half. Different conclusion, different generality, different Mathlib revision.

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Elements of Queueing Theory Ib: Ergodicity and Stochastic IntensityTextbook

Ergodicity and Stochastic Intensity

Background

Chapter 1 of Baccelli and Brémaud's Elements of Queueing Theory has two halves. The first builds Palm calculus from the Matthes definition of P⁰_N and reaches the Swiss army formula. This mission is the second: §§1.6, 1.8 and 1.9, which supply the two things the rest of the book runs on.

Ergodic theory, quoted

§1.6 states, in its own words, "the ergodic theory results to be used later in this book". Five of them, and the book proves none: Birkhoff's pointwise ergodic theorem in discrete (Theorem 1.6.1) and continuous time (Theorem 1.6.4), Kingman's sub-additive ergodic theorem (Theorem 1.6.2), and the extremal characterizations of ergodicity in both settings (Theorems 1.6.3 and 1.6.5) — ergodicity is exactly the impossibility of splitting an invariant probability into two distinct ones.

They are quoted, but they are not decoration. Kingman's theorem is what produces the asymptotic growth rates of Theorem 2.11.2 and the constant γ(c) on which the saturation rule rests. Birkhoff's theorem is what makes the time average in PASTA's (3.3.2) a well-defined object, and what the fluid Loynes theorem invokes for lim_{u→−∞}(A_{u,0} − C_{u,0}) = −∞.

None of the three analytic ones exists in Mathlib. Analysis/InnerProductSpace/MeanErgodic is the mean (von Neumann, L²) theorem, not almost-everywhere convergence, and there is no sub-additive ergodic theorem at all. The platform has neither.

Predictability, and why PASTA can be stated

§1.8 introduces the stochastic intensity: a point process N admits the (P, F_t)-intensity {λ(t)} when E[N(a,b] 1_A] = E[(∫_a^b λ(t)dt) 1_A] for A ∈ F_a. Around it sits the notion of a predictable process — one measurable with respect to the strict past.

Theorem 1.8.1 is the structural fact that makes predictability usable. For the internal history of a marked point process, every predictable process has the concrete form

Z(t, ω) = v(t, θ_t ω),    v(t, ·) F_{0−}-measurable.                                   (1.8.1)

That is why mission IV can take this form as PASTA's hypothesis rather than constructing a predictable σ-field: Theorem 1.8.1 says nothing is lost.

The goal

Theorem 1.8.2 (p.61), §1.8.4, Watanabe's characterization of Poisson processes. For a history F_t = F_t^N ∨ G and a G-measurable, locally integrable {λ(t)}, if N admits the F_t-intensity {λ(t)} then N is a G-conditional Poisson process:

E[ e^{iuN(a,b]} | G ∨ F^N_a ] = exp{ (e^{iu} − 1) ∫_a^b λ(t) dt } .                    (1.8.12)

A stochastic intensity that carries no information beyond G forces the process to be Poisson conditionally on G, with the compensator as the parameter — and the conditional characteristic function is the exact Poisson one, not an approximation. With G trivial and λ constant this is the ordinary Poisson process, which is the equivalence Remark 3.3.1 of Chapter 3 invokes to explain the name PASTA. The book: "This result plays a role in queueing theory, especially for proving that some streams in a queueing network are or are not Poissonian."

Palm probability meets stochastic intensity

§1.9 asks whether the stochastic intensity is the same under P and under P⁰_N — whether the two probabilities describe the same dynamics. Theorem 1.9.1 says yes, on ℝ₊: the same process {λ(t)} serves both.

Theorem 1.9.2 is Papangelou's theorem, and it is the deepest statement of the section: N admits a stochastic intensity if and only if P⁰_N ≪ P on F_{0−}, and then λ(t) = (μ ∘ θ_t)λ with μ the Radon–Nikodým derivative. A dynamic property and a static one turn out to be the same thing.

Theorem 1.9.3 is Mecke's characterization: N is Poisson exactly when P ≡ P⁰_N on F_{0−}. The view from a point of the process and the view from a deterministic instant agree on the strict past precisely when the process has no memory. It follows in one line from the two theorems before it.

What this mission provides

Four of the five missions in this series import the Chapter 1 substrate; this one adds the two pieces they need from its second half — ergodic theory and the stochastic intensity. Nothing here is on the platform, and Mathlib has filtrations and adapted processes but no predictability in this form, no stochastic intensity, no pointwise ergodic theorem and no Kingman.

Formalization scope

Every result is stated in the book's strength, with the book's standing definitions as binders. A discrete flow is a bijective, measurable, P⁰-preserving map (p.46); a continuous flow is jointly measurable in (t, ω) (p.3, clause (a)). A history compatible with the flow satisfies θ_t F_s = F_{s−t} (p.57), and an F_t-intensity is a non-negative, measurable, locally integrable, adapted process (p.58). The limits of Theorems 1.6.1, 1.6.2 and 1.6.4 are asserted to exist; Kingman's constant h̄ lies in ℝ ∪ {−∞} and is identified with inf_n (1/n) E⁰[h_n], the means being extended reals so that E⁰[h_n] = −∞ is not read as 0. Theorems 1.6.3, 1.6.5, 1.9.2 and 1.9.3 are equivalences, and Theorem 1.9.2 carries the closed form λ(t) = (μ ∘ θ_t)λ with μ = dP⁰_N/dP on F_{0−}. The goal's conclusion is the exact conditional characteristic function (1.8.12); a formalization that only asserted some conditional Poisson law, or conditioned on G alone, would not be this theorem.

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Elements of Queueing Theory I: The Swiss Army Formula of Palm CalculusTextbook

The Swiss Army Formula of Palm Calculus

Background

Chapter 1 of Baccelli and Brémaud's Elements of Queueing Theory builds the calculus that the rest of the book runs on. Its subject is the relation between two ways of looking at the same stationary system: from a clock fixed in time, and from a customer arriving into it. The two are not the same — the interval a random instant falls into is longer than a typical interval, a fact every queueing student meets as the inspection paradox — and the object that makes the difference precise is the Palm probability P⁰_N.

The chapter defines P⁰_N by the Matthes definition in terms of counting,

λ t P⁰_N(A) = E[ Σ_{n ∈ ℤ} 1_A(θ_{T_n}) 1_{(0,t]}(T_n) ],                          (1.2.1)

and everything else is a theorem about it. That ordering is deliberate here too: P⁰_N is carried in the formalization as a predicate satisfying (1.2.1), not as a measure constructed to make Mecke's formula true. If it were the latter, Mecke's formula would be a definition and the inversion formula and the goal theorem would inherit that emptiness.

From (1.2.1) the chapter derives, in order: that P⁰_N is invariant under the point shift (1.2.16); Mecke's formula (1.2.17), which the literature also knows as the generalized Campbell formula; the inversion formula of Ryll-Nardzewski and Slivnyak (1.2.25), which runs back from P⁰_N to P; the mean-value formulas (1.3.2)–(1.3.3); the Neveu exchange formula (1.3.4), which relates two point processes stationary for the same flow; and the Miyazawa rate conservation principle (1.3.10), which balances the drift of a process between its jumps against the rate at which it jumps.

The goal

§1.3.7 then collects all of them into one identity. Its name is the book's own:

Depending on which blade is selected, a Swiss army knife transforms itself into various useful tools. The formula obtained in this subsection is called the Swiss army formula of Palm calculus because it contains the main formulas of this theory, as well as some new ones.

Theorem 1.3.1 (p.29). For arrivals {T_n} with counting measure A and intensity λ_A, departures {τ_n} with counting measure D — not assumed ordered — sojourn times W_n = τ_n − T_n ≥ 0 forming a sequence of marks of A, the number in system {X(t)} with X(b) − X(a) = A((a,b]) − D((a,b]), a non-decreasing corlol integrator {B(t)} and a non-negative process {Z(t)}, all compatible with a measurable flow under which P is invariant:

λ_A E⁰_A [ ∫_(0,W_0] Z(s) dB(s) ] = (1/t) E [ ∫_(0,t] X(s−) Z(s) dB(s) ].              (1.3.28)

Selecting the blade Z ≡ 1, B(t) = t turns it into λ_A E⁰_A[W_0] = E[X(0)] — Little's law, here in its full stationary-ergodic form rather than as a deterministic sample-path identity. Other choices give the inversion formula, the Miyazawa conservation principle and the rate conservation law.

The local meaning of P⁰_N

One milestone stands slightly apart. Theorem 1.5.1 (p.45) is what licenses the whole reading of P⁰_N as "what an arriving customer sees":

lim_{t→0} sup_{A ∈ F} | P⁰_N(A) − P(θ_{T_1} ∈ A | T_1 ≤ t) | = 0.                       (1.5.3)

The supremum is inside the limit. The convergence is uniform over every measurable event, which is what Dobrushin's estimate of §1.5.1 buys and what a pointwise limit would not give.

What this mission provides

Nothing in this chapter exists on the platform or in Mathlib: not stationary marked point processes, not Palm probability, not the Campbell measure. Four of the five missions in this series import the vocabulary built here, and the two definition items — the substrate of §§1.1–1.2 and the setting of §1.3.7 — are as much of the deliverable as the theorems are.

Formalization scope

  • The flow {θ_t} is a one-parameter group with (t, ω) ↦ θ_t ω jointly measurable (p.5 (a)); a point process is its strictly increasing points {T_n}_{n ∈ ℤ} with T_0 ≤ 0 < T_1, infinitely many on each side (Hypothesis 1.1.1), with finite non-null intensity λ = E[N((0,1])].
  • P⁰_N is characterized by (1.2.1) for every t > 0, which determines it uniquely; nothing is axiomatized. A formalization that introduced P⁰_N as any measure satisfying Mecke's formula would make the milestones and the goal trivial and is ruled out.
  • Every "for all non-negative measurable" formula (Mecke, inversion, mean-value, Neveu, Wald, the goal) is stated in [0, ∞] with lower Lebesgue integrals, for all such functions, not only bounded or integrable ones.
  • Three hypotheses the book uses without listing them are explicit: the Swiss army formula assumes the integrator {B(t)} is θ_t-compatible (the proof uses it, and without it the identity fails); it is stated for t > 0, the only values at which 1/t and (0, t] give it content; and the Miyazawa principle assumes Y'(0) ∈ L¹(P), which its E[Y'(0)] presupposes.
  • Theorem 1.5.1 keeps the supremum over all events inside the limit (one δ for every A).
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Markov ChainOperations ResearchProbability·Captain: mikedeng1

Stochastic Dynamic Programming and the Control of Queueing Systems XIV: Conforming Approximating Sequences for Markov ChainsTextbook

Motivation

Countable-state Markov chains are the standard model of queues with unbounded buffers, but any numerical computation of their long-run behaviour works on a finite state space. The usual remedy is truncation: restrict the chain to a finite set SNS_NSN​ and redistribute the probability of leaving SNS_NSN​ back into it. Whether the steady state probabilities and average costs of the truncated chains converge to those of the original chain depends on how that probability is redistributed. Gibson and Seneta studied this question for the stationary distributions of chains without costs (Gibson and Seneta, J. Appl. Prob., 1987). Sennott extended it to chains with costs and expected first passage costs (Sennott, Adv. Appl. Prob. 29, 1997; ZOR Math. Meth. Oper. Res. 45, 1997), and used it as the basis of the approximating sequence method for average-cost Markov decision chains (Sennott, 1999, Chapter 8). This mission covers Appendix C, Sections C.4–C.5 of the 1999 book, the Markov-chain results that the book's average-cost approximation theorems use.

Setting

A Markov chain with costs Γ\GammaΓ on a denumerable state space SSS has transition probabilities PijP_{ij}Pij​ with ∑jPij=1\sum_jP_{ij}=1∑j​Pij​=1 and a finite nonnegative cost C(i)C(i)C(i) at each state. For a set G⊆SG\subseteq SG⊆S and a start iii, TiG≥1T_{iG}\ge 1TiG​≥1 is the first passage time to GGG. The taboo probability GPik(t){}_GP^{(t)}_{ik}G​Pik(t)​ is the probability of moving from iii to kkk in ttt steps with no intermediate state in GGG. The expected visits Guik{}_Gu_{ik}G​uik​ count the visits to kkk at times 0≤t<TiG0\le t<T_{iG}0≤t<TiG​. The mean first passage time is miG=E[TiG]m_{iG}=E[T_{iG}]miG​=E[TiG​], infinite when GGG is missed with positive probability. The first passage cost is ciG=E[∑t<TiGC(Xt)]c_{iG}=E\big[\sum_{t<T_{iG}}C(X_t)\big]ciG​=E[∑t<TiG​​C(Xt​)]. A state iii is positive recurrent when mii<∞m_{ii}<\inftymii​<∞, and the steady state probability is πi=mii−1\pi_i=m_{ii}^{-1}πi​=mii−1​. On a positive recurrent class RRR the average cost is JR=∑j∈RπjC(j)J_R=\sum_{j\in R}\pi_jC(j)JR​=∑j∈R​πj​C(j). The chain is zzz standard when miz<∞m_{iz}<\inftymiz​<∞ and ciz<∞c_{iz}<\inftyciz​<∞ for every iii. Such a chain has one positive recurrent class R∋zR\ni zR∋z with JR<∞J_R<\inftyJR​<∞, and every other state is transient.

An approximating sequence (AS) (ΓN)N≥N0(\Gamma_N)_{N\ge N_0}(ΓN​)N≥N0​​ consists of increasing nonempty finite sets SNS_NSN​ with ⋃NSN=S\bigcup_NS_N=S⋃N​SN​=S and, for each NNN, a chain ΓN\Gamma_NΓN​ on SNS_NSN​ with the same costs and transition probabilities Pij(N)→PijP_{ij}(N)\to P_{ij}Pij​(N)→Pij​. The quantities of ΓN\Gamma_NΓN​ are written miG(N)m_{iG}(N)miG​(N), ciG(N)c_{iG}(N)ciG​(N), πi(N)\pi_i(N)πi​(N) and J(i)(N)J(i)(N)J(i)(N). An AS is conforming (for a zzz standard Γ\GammaΓ) if, for large NNN, ΓN\Gamma_NΓN​ is unichain with zzz in its positive recurrent class, and miz(N)→mizm_{iz}(N)\to m_{iz}miz​(N)→miz​ and ciz(N)→cizc_{iz}(N)\to c_{iz}ciz​(N)→ciz​ for all iii. It is conforming on RRR if πi(N)→πi\pi_i(N)\to\pi_iπi​(N)→πi​ and J(i)(N)→JRJ(i)(N)\to J_RJ(i)(N)→JR​ on RRR.

An augmentation type approximating sequence (ATAS) keeps the original probabilities inside SNS_NSN​ and redistributes the probability of each excluded target r∉SNr\notin S_Nr∈/SN​ according to an augmentation distribution q⋅(i,r,N)q_\cdot(i,r,N)q⋅​(i,r,N) on SNS_NSN​:

Pij(N)=Pij+∑r∈S−SNPir qj(i,r,N),j∈SN.P_{ij}(N)=P_{ij}+\sum_{r\in S-S_N}P_{ir}\,q_j(i,r,N),\qquad j\in S_N.Pij​(N)=Pij​+r∈S−SN​∑​Pir​qj​(i,r,N),j∈SN​.

It sends excess probability to GGG if every q⋅(i,r,N)q_\cdot(i,r,N)q⋅​(i,r,N) is concentrated on GGG.

Formalization targets

Goal: Proposition C.5.2

For a zzz standard chain Γ\GammaΓ and a finite nonempty G⊆SG\subseteq SG⊆S,

every ATAS that sends excess probability to G is conforming,\text{every ATAS that sends excess probability to } G \text{ is conforming},every ATAS that sends excess probability to G is conforming,

and if G⊆RG\subseteq RG⊆R it is also conforming on RRR. No rate of convergence and no constants are involved, and GGG need not contain zzz.

Milestones

  1. Proposition C.4.2: for fixed ttt, lim⁡NGPik(t)(N)=GPik(t)\lim_N{}_GP^{(t)}_{ik}(N)={}_GP^{(t)}_{ik}limN​G​Pik(t)​(N)=G​Pik(t)​; also lim inf⁡NGuik(N)≥Guik\liminf_N{}_Gu_{ik}(N)\ge{}_Gu_{ik}liminfN​G​uik​(N)≥G​uik​ and lim inf⁡NmiG(N)≥miG\liminf_Nm_{iG}(N)\ge m_{iG}liminfN​miG​(N)≥miG​.
  2. Proposition C.4.3: πi(N)→0\pi_i(N)\to0πi​(N)→0 off the positive recurrent states, and along subsequences πi(Ns)→bπi\pi_i(N_s)\to b\pi_iπi​(Ns​)→bπi​ on a class, with 0≤b≤10\le b\le10≤b≤1.
  3. Proposition C.4.5: lim inf⁡NciG(N)≥ciG\liminf_Nc_{iG}(N)\ge c_{iG}liminfN​ciG​(N)≥ciG​.
  4. Proposition C.4.6: on a positive recurrent class, convergence of π\piπ, of mzzm_{zz}mzz​ and of all miGm_{iG}miG​ are equivalent. Given these, convergence of J(i)J(i)J(i), of czzc_{zz}czz​ and of all ciGc_{iG}ciG​ are equivalent.
  5. Proposition C.4.9: conformity implies πi(N)→πi\pi_i(N)\to\pi_iπi​(N)→πi​ for all iii, and that the constant average costs J(N)J(N)J(N) of ΓN\Gamma_NΓN​ converge to JRJ_RJR​.

Further results

  1. Proposition C.5.3: an ATAS is conforming when, for N≥N∗N\ge N^*N≥N∗, the augmentation distributions satisfy ∑j≠zqj(i,r,N)mjz≤mrz\sum_{j\ne z}q_j(i,r,N)m_{jz}\le m_{rz}∑j=z​qj​(i,r,N)mjz​≤mrz​ and ∑j≠zqj(i,r,N)cjz≤crz\sum_{j\ne z}q_j(i,r,N)c_{jz}\le c_{rz}∑j=z​qj​(i,r,N)cjz​≤crz​.
  2. Corollary C.5.4: for a 000 standard chain on {0,1,2,… }\{0,1,2,\dots\}{0,1,2,…} with an upper Hessenberg transition matrix, truncated to SN={0,…,N}S_N=\{0,\dots,N\}SN​={0,…,N} with the excess sent to NNN, the ATAS is conforming.

Significance

The result. Conformity is the hypothesis under which the book's approximating sequence method works for average-cost queueing control (Chapter 8). The method computes optimal policies for finite truncations and passes to the limit. That argument needs the first passage times and costs to a distinguished state to converge along the chains induced by fixed policies. Propositions C.5.2 and C.5.3 turn this analytic requirement into conditions on the truncation scheme that can be checked in practice: send the overflow to a fixed finite set, or to states from which reaching zzz is no more expensive. Examples C.4.4 and C.4.7 of the book show that an arbitrary approximating sequence can fail. The limit of the steady state probabilities can be a strict multiple bπb\pibπ with b<1b<1b<1. First passage costs can converge to the wrong value even when the steady state probabilities converge.

Formalizing it. The results are proved in the book, some in abbreviated form ("the proof for the costs is similar and is omitted"). The Prove2Me library had no statement on truncation or augmentation of countable Markov chains when this mission was drafted (September 2026). A formalization supplies the omitted cost arguments, makes the passage between lim inf⁡\liminfliminf bounds and limits in [0,∞][0,\infty][0,∞] explicit, and produces a reusable library of first passage quantities for countable chains.

Difficulty

The lower bounds of Propositions C.4.2 and C.4.5 are the routine part. The difficulty is the matching upper bound: in ΓN\Gamma_NΓN​, a first passage that leaves SNS_NSN​ is restarted elsewhere, which can lengthen it without bound. Taking limits termwise in the first passage equation miz(N)=1+∑j≠zPij(N)mjz(N)m_{iz}(N)=1+\sum_{j\ne z}P_{ij}(N)m_{jz}(N)miz​(N)=1+∑j=z​Pij​(N)mjz​(N) fails, because no dominating function is available and mass can escape to infinity. Example C.4.4 exhibits exactly this. Unichain structure is also not automatic: ΓN\Gamma_NΓN​ may have several recurrent classes, or a recurrent class not containing zzz, and ruling this out is part of the conclusion rather than an assumption.

Formalization scope

The Lean development works in SennottDP.ChainASM. A chain is a structure MC S with P : S → S → ℝ≥0∞, ∑' j, P i j = 1 and C : S → ℝ≥0. Theorems assume [Countable S] [Infinite S], matching the book's denumerable state space. Taboo probabilities, expected visits, miGm_{iG}miG​, ciGc_{iG}ciG​, πj=(mjj)−1\pi_j=(m_{jj})^{-1}πj​=(mjj​)−1 and JR=∑j∈RπjC(j)J_R=\sum_{j\in R}\pi_jC(j)JR​=∑j∈R​πj​C(j) are defined as sums in [0,∞][0,\infty][0,∞]. miG=∑t≥0P(TiG>t)m_{iG}=\sum_{t\ge0}P(T_{iG}>t)miG​=∑t≥0​P(TiG​>t) is infinite whenever GGG is missed with positive probability. The average cost J(i)J(i)J(i) is the lim sup⁡\limsuplimsup of the Cesàro cost averages.

An AS is a structure carrying N0N_0N0​, the finite sets SNS_NSN​ (as Finset S) and Pij(N)P_{ij}(N)Pij​(N). ΓN\Gamma_NΓN​ is built as an MC on the subtype of SNS_NSN​, and a set GGG is read in ΓN\Gamma_NΓN​ as G∩SNG\cap S_NG∩SN​. Quantities of ΓN\Gamma_NΓN​ are lifted to functions of NNN and of states of SSS with the value 000 where they are undefined (N<N0N<N_0N<N0​ or a state outside SNS_NSN​). For fixed states this affects finitely many NNN, and all statements are limits, lim inf⁡\liminfliminfs or eventual equalities. All convergence is in [0,∞][0,\infty][0,∞]. The conformity predicate includes the standing assumption that Γ\GammaΓ is zzz standard. The positive recurrent class RRR of a zzz standard chain is the communicating class of zzz.

A trivializing formalization is excluded: the AS of Example C.4.4, whose positive recurrent class {N}\{N\}{N} excludes z=0z=0z=0, is not conforming under these definitions. The ATAS predicate requires the augmentation distributions to be probability distributions and to reproduce Pij(N)P_{ij}(N)Pij​(N) exactly by (C.27).

A complete development needs first passage decompositions for countable chains, the renewal-reward identity JR=czz/mzzJ_R=c_{zz}/m_{zz}JR​=czz​/mzz​, and dominated and Fatou-type limit theorems for sums (the book's Appendix A). The first passage library and the lifted-quantity conventions can be reused by the average-cost approximation chapters. Contributions of intermediate lemmas are welcome, especially the finite-state unichain facts of Section C.3 and the identities of Propositions C.1.4 and C.2.2.

Proposition C.5.5 (lower Hessenberg chains, from Gibson and Seneta) is stated in the book without proof and without naming the distinguished state, and is not included.

Selected references

  • L. I. Sennott, Stochastic Dynamic Programming and the Control of Queueing Systems, Wiley, 1999, Appendix C, Sections C.4–C.5. https://doi.org/10.1002/9780470317037
  • L. I. Sennott, "The computation of average optimal policies in denumerable state Markov decision chains", Advances in Applied Probability 29 (1997) 114–137 (cited in the book as Sennott 1997a).
  • L. I. Sennott, "On computing average cost optimal policies with application to routing to parallel queues", ZOR Mathematical Methods of Operations Research 45 (1997) 45–62 (cited in the book as Sennott 1997b).
  • D. Gibson and E. Seneta, "Augmented truncations of infinite stochastic matrices", Journal of Applied Probability (1987).
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Numerical AnalysisProbability·Captain: mikedeng1

Euler Approximations with Varying Coefficients III: Uniform Lq-Convergence with Order 1/2Research Paper

Motivation

Stochastic differential equations whose coefficients grow faster than linearly (for instance stochastic volatility models such as the 3/2-model) cannot be simulated with the classical explicit Euler–Maruyama scheme: Hutzenthaler, Jentzen and Kloeden showed that its moments diverge when the drift or diffusion grows superlinearly (Proc. R. Soc. A, 2011). Implicit schemes avoid the divergence but require solving a nonlinear equation at every step. Tamed Euler schemes keep the scheme explicit and damp the coefficients by a factor depending on the step size.

  • 2012: Hutzenthaler, Jentzen and Kloeden introduce a tamed Euler scheme for SDEs with superlinearly growing drift (Ann. Appl. Probab. 22, 2012).
  • 2013: Sabanis extends the taming analysis for superlinearly growing drift (Electron. Commun. Probab. 18, no. 10, 2013, MR3070913).
  • 2015: Hutzenthaler and Jentzen survey explicit schemes for non-globally Lipschitz coefficients (Mem. Amer. Math. Soc. 236, no. 1112, 2015); for the 3/2-model their results give Lp\mathcal L^pLp-convergence without rate only for p<1/2p<1/2p<1/2, as Sabanis (2016, p. 2) notes.
  • 2016: Sabanis (Ann. Appl. Probab. 26(4), 2016, arXiv:1308.1796v4) treats schemes with varying coefficients bn,σnb_n,\sigma_nbn​,σn​, covering superlinearly growing diffusion coefficients, and proves Lp\mathcal L^pLp convergence (Theorem 1), the Lp\mathcal L^pLp rate 1/2 (Theorem 2) and the uniform Lq\mathcal L^qLq rate 1/2 (Theorem 3). A motivating example is the ddd-dimensional analogue of the 3/2-model of stochastic volatility, dX=λX(μ−∣X∣) dt+ξ∣X∣3/2 dWdX=\lambda X(\mu-|X|)\,dt+\xi|X|^{3/2}\,dWdX=λX(μ−∣X∣)dt+ξ∣X∣3/2dW, used for pricing VIX options.

Theorem 3 is the target here; Theorems 1 and 2 are the targets of companion missions.

Setting

Fix a filtered probability space (Ω,{Ft}t≥0,F,P)(\Omega,\{\mathcal F_t\}_{t\ge0},\mathcal F,P)(Ω,{Ft​}t≥0​,F,P) satisfying the usual conditions, a d1d_1d1​-dimensional Wiener martingale WWW, a horizon T>0T>0T>0, and exponents p0,p1≥2p_0,p_1\ge2p0​,p1​≥2. For x∈Rdx\in\mathbb R^dx∈Rd, ∣x∣|x|∣x∣ is the Euclidean norm; for a d×d1d\times d_1d×d1​ matrix AAA, ∣A∣|A|∣A∣ is the Hilbert–Schmidt norm; xyxyxy is the scalar product. The coefficients are Borel functions b:[0,∞)×Rd→Rdb:[0,\infty)\times\mathbb R^d\to\mathbb R^db:[0,∞)×Rd→Rd and σ:[0,∞)×Rd→Rd×d1\sigma:[0,\infty)\times\mathbb R^d\to\mathbb R^{d\times d_1}σ:[0,∞)×Rd→Rd×d1​, and the SDE is

dX(t)=b(t,X(t)) dt+σ(t,X(t)) dW(t),t∈[0,T],(2.1)dX(t)=b(t,X(t))\,dt+\sigma(t,X(t))\,dW(t),\qquad t\in[0,T],\qquad(2.1)dX(t)=b(t,X(t))dt+σ(t,X(t))dW(t),t∈[0,T],(2.1)

with an F0\mathcal F_0F0​-measurable initial value X(0)X(0)X(0). With κn(t)=⌊nt⌋/n\kappa_n(t)=\lfloor nt\rfloor/nκn​(t)=⌊nt⌋/n, the scheme (2.2) is

dXn(t)=bn(t,Xn(κn(t))) dt+σn(t,Xn(κn(t))) dW(t),Xn(0)=X(0),dX_n(t)=b_n(t,X_n(\kappa_n(t)))\,dt+\sigma_n(t,X_n(\kappa_n(t)))\,dW(t),\qquad X_n(0)=X(0),dXn​(t)=bn​(t,Xn​(κn​(t)))dt+σn​(t,Xn​(κn​(t)))dW(t),Xn​(0)=X(0),

and in this mission bn,σnb_n,\sigma_nbn​,σn​ are the tamed coefficients of Model 2 with α=1/2\alpha=1/2α=1/2:

bn(t,x)=b(t,x)1+n−1/2∣x∣l,σn(t,x)=σ(t,x)1+n−1/2∣x∣l.b_n(t,x)=\frac{b(t,x)}{1+n^{-1/2}|x|^l},\qquad \sigma_n(t,x)=\frac{\sigma(t,x)}{1+n^{-1/2}|x|^l}.bn​(t,x)=1+n−1/2∣x∣lb(t,x)​,σn​(t,x)=1+n−1/2∣x∣lσ(t,x)​.

The conditions used are: A-2, local boundedness of bbb on balls; A-4, the coercivity bound 2xb(t,x)+(p0−1)∣σ(t,x)∣2≤K(1+∣x∣2)2xb(t,x)+(p_0-1)|\sigma(t,x)|^2\le K(1+|x|^2)2xb(t,x)+(p0​−1)∣σ(t,x)∣2≤K(1+∣x∣2); A-5, E∣X(0)∣p0<∞\mathbb E|X(0)|^{p_0}<\inftyE∣X(0)∣p0​<∞; and A-6, the global monotonicity

2(x−y)(b(t,x)−b(t,y))+(p1−1)∣σ(t,x)−σ(t,y)∣2≤L∣x−y∣22(x-y)(b(t,x)-b(t,y))+(p_1-1)|\sigma(t,x)-\sigma(t,y)|^2\le L|x-y|^22(x−y)(b(t,x)−b(t,y))+(p1​−1)∣σ(t,x)−σ(t,y)∣2≤L∣x−y∣2

together with the polynomial Lipschitz bound ∣b(t,x)−b(t,y)∣≤L(1+∣x∣l+∣y∣l)∣x−y∣|b(t,x)-b(t,y)|\le L(1+|x|^l+|y|^l)|x-y|∣b(t,x)−b(t,y)∣≤L(1+∣x∣l+∣y∣l)∣x−y∣, with l,L>0l,L>0l,L>0. The p\mathfrak pp-condition asks l≤p0−24l\le\frac{p_0-2}{4}l≤4p0​−2​ and a moment exponent ppp with 0<p<p10<p<p_10<p<p1​ and p≤p02l+1p\le\frac{p_0}{2l+1}p≤2l+1p0​​.

Formalization targets

Goal: Theorem 3 (p. 6)

Under A-2, A-4–A-6 and the p\mathfrak pp-condition, for every 0<q<p0<q<p0<q<p there is CCC independent of nnn with

E[sup⁡0≤t≤T∣X(t)−Xn(t)∣q]≤Cn−q/2,n≥1.(2.14)\mathbb E\Big[\sup_{0\le t\le T}|X(t)-X_n(t)|^q\Big]\le Cn^{-q/2},\qquad n\ge1.\qquad(2.14)E[0≤t≤Tsup​∣X(t)−Xn​(t)∣q]≤Cn−q/2,n≥1.(2.14)

The supremum is inside the expectation, which distinguishes it from Theorem 2.

Milestones

  1. Lemma 2 (p. 8): the moments of XXX and of XnX_nXn​ up to order p0p_0p0​ are bounded on [0,T][0,T][0,T] uniformly in nnn (for general coefficients bn,σnb_n,\sigma_nbn​,σn​ under A-1–A-5, B-2, B-3).
  2. Lemma 5 (p. 19): the Gyöngy–Krylov maximal inequality. If nonnegative continuous adapted f,gf,gf,g satisfy E[fτ1{g0≤c}]≤E[gτ1{g0≤c}]\mathbb E[f_\tau\mathbb 1_{\{g_0\le c\}}]\le\mathbb E[g_\tau\mathbb 1_{\{g_0\le c\}}]E[fτ​1{g0​≤c}​]≤E[gτ​1{g0​≤c}​] for all c>0c>0c>0 and stopping times τ≤T\tau\le Tτ≤T, then
E[sup⁡t≤τftγ]≤2−γ1−γ E[sup⁡t≤τgtγ],γ∈(0,1).\mathbb E\Big[\sup_{t\le\tau}f_t^\gamma\Big]\le\frac{2-\gamma}{1-\gamma}\,\mathbb E\Big[\sup_{t\le\tau}g_t^\gamma\Big],\qquad\gamma\in(0,1).E[t≤τsup​ftγ​]≤1−γ2−γ​E[t≤τsup​gtγ​],γ∈(0,1).
  1. Lemma 4 (p. 16): sup⁡0≤t≤TE∣Xn(t)−Xn(κn(t))∣p≤Cn−p/2\sup_{0\le t\le T}\mathbb E|X_n(t)-X_n(\kappa_n(t))|^p\le Cn^{-p/2}sup0≤t≤T​E∣Xn​(t)−Xn​(κn​(t))∣p≤Cn−p/2.
  2. Lemma 3 (p. 15): the taming errors E∫0T∣b−bn∣p(s,Xn(κn(s))) ds\mathbb E\int_0^T|b-b_n|^p(s,X_n(\kappa_n(s)))\,dsE∫0T​∣b−bn​∣p(s,Xn​(κn​(s)))ds and the analogue for σ\sigmaσ are ≤Cn−αp\le Cn^{-\alpha p}≤Cn−αp.

Significance

Theorem 3 gives the optimal strong rate 1/2 for an explicit scheme, uniformly over the time interval, for SDEs whose diffusion coefficient may grow superlinearly. Uniform-in-time error bounds are what pathwise functionals need (running maxima, barrier options, hitting times), and via Borel–Cantelli they give the almost-sure rate of Corollary 1 in the paper. Lemma 5 is a general-purpose tool: a domination inequality of Lenglart type, used throughout stochastic analysis to pass from bounds at stopping times to bounds on running suprema.

The results are proved in the paper; to our knowledge none of them has been formalized. Formalizing them would produce the first machine-checked convergence rate of a numerical scheme for SDEs, and a Lean proof of a Lenglart-type inequality, which Mathlib does not currently contain.

Difficulty

The error X−XnX-X_nX−Xn​ is controlled by the monotonicity condition A-6, which is one-sided: it bounds 2(x−y)(b(t,x)−b(t,y))2(x-y)(b(t,x)-b(t,y))2(x−y)(b(t,x)−b(t,y)) from above but gives no Lipschitz bound on bbb or σ\sigmaσ with a constant independent of ∣x∣,∣y∣|x|,|y|∣x∣,∣y∣. The first idea, estimating Esup⁡t∣X−Xn∣p\mathbb E\sup_t|X-X_n|^pEsupt​∣X−Xn​∣p directly by applying the Burkholder–Davis–Gundy inequality to the martingale part of the error equation, therefore does not close: it produces terms of the same order as the quantity being estimated, weighted by polynomial factors in ∣X∣|X|∣X∣ and ∣Xn∣|X_n|∣Xn​∣, and the argument that gives Theorem 2 controls E∣X(t)−Xn(t)∣p\mathbb E|X(t)-X_n(t)|^pE∣X(t)−Xn​(t)∣p only for fixed ttt. Passing from fixed times to the supremum is what forces the loss from ppp to q<pq<pq<p in Theorem 3, and it is where Lemma 5 enters. On the formal side, the Itô integral against Brownian motion, Itô's formula for functions of multidimensional Itô processes and the Burkholder–Davis–Gundy inequality are not in Mathlib.

Formalization scope

Processes are indexed by t∈[0,∞)t\in[0,\infty)t∈[0,∞) (ℝ≥0) with values in EuclideanSpace ℝ (Fin d); diffusion values live in EuclideanSpace ℝ (Fin d × Fin d₁), whose norm is the Hilbert–Schmidt norm. The stochastic integral is the Ethier–Kurtz platform relation EthierKurtz.HasBrownianItoIntegral, applied coordinatewise, with integrands cut off after TTT. Solutions are hypotheses: the theorems apply to any solution XXX of (2.1) and any family (Xn)n≥1(X_n)_{n\ge1}(Xn​)n≥1​ of solutions of (2.2) on one probability space with one WWW and one X(0)X(0)X(0); existence is not claimed. Processes are required to be adapted to the filtration augmented by null sets (weaker than a complete filtration), the filtration is right-continuous, and nothing is required after TTT. Expectations and suprema are computed in [0,∞][0,\infty][0,∞], so no statement holds through an integral defaulting to 000. Constants CCC depend on everything except nnn (and, in Theorem 3, may depend on qqq); only n≥1n\ge1n≥1 is used, and q>0q>0q>0, p>0p>0p>0 follow the paper's Lp\mathcal L^pLp convention.

Two hypotheses are added to the printed statements, both because the printed proofs need them:

  • p1>2p_1>2p1​>2 in Theorem 3. The proof applies Itô's formula for p≥2p\ge2p≥2; an admissible p<2p<2p<2 is handled through p′=2p'=2p′=2, which satisfies the p\mathfrak pp-condition exactly when p1>2p_1>2p1​>2.
  • B-3 in Lemma 4. The proof uses moment bounds uniform in nnn (Lemma 2), which need B-3. Model 2 satisfies B-3.

Lemma 2 drops the dependence clause C=C(p,T,K,E∣X(0)∣p)C=C(p,T,K,\mathbb E|X(0)|^p)C=C(p,T,K,E∣X(0)∣p) and asserts only finiteness. Lemma 5 assumes neither that ggg is nondecreasing nor anything beyond the printed hypotheses.

A trivializing formalization is ruled out: the supremum sits inside a Lebesgue integral in [0,∞][0,\infty][0,∞], so the goal cannot hold because of a junk value, and the hypotheses are satisfiable (zero coefficients, constant solutions), which a sorry-free check confirms.

Needed infrastructure: Itô's formula for multidimensional Itô processes, the Burkholder–Davis–Gundy inequality (for Lemma 4), Gronwall's inequality in integral form, and stopping-time localisation for continuous adapted processes. Contributions to any of these are welcome, and all are reusable far beyond this mission. Lemma 5 is independent of the SDE part and can be attacked first.

Selected references

  • S. Sabanis, Euler approximations with varying coefficients: the case of superlinearly growing diffusion coefficients, Ann. Appl. Probab. 26(4), 2083–2105, 2016. https://doi.org/10.1214/15-AAP1140 — arXiv:1308.1796v4, https://arxiv.org/abs/1308.1796v4
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong and weak divergence in finite time of Euler's method for stochastic differential equations with non-globally Lipschitz continuous coefficients, Proc. R. Soc. A 467, 1563–1576, 2011. https://doi.org/10.1098/rspa.2010.0348
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong convergence of an explicit numerical method for SDEs with nonglobally Lipschitz continuous coefficients, Ann. Appl. Probab. 22(4), 1611–1641, 2012. https://doi.org/10.1214/11-AAP803
  • M. Hutzenthaler, A. Jentzen, Numerical approximations of stochastic differential equations with non-globally Lipschitz continuous coefficients, Mem. Amer. Math. Soc. 236, no. 1112, 2015 (reference [5] of the paper).
  • S. Sabanis, A note on tamed Euler approximations, Electron. Commun. Probab. 18, no. 10, 2013. MR3070913
  • I. Gyöngy, N. V. Krylov, On the rate of convergence of splitting-up approximations for SPDEs, in Stochastic Inequalities and Applications, Progr. Probab. 56, 301–321, Birkhäuser, 2003 (cited by the paper for Lemma 5). MR2073438
  • N. V. Krylov, Introduction to the Theory of Diffusion Processes, Transl. Math. Monographs 142, AMS, 1995 (cited by the paper for Lemma 5). MR1311478
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Numerical AnalysisProbability·Captain: mikedeng1

Euler Approximations with Varying Coefficients II: Strong Order 1/2 in Lp for Superlinearly Growing Diffusion CoefficientsResearch Paper

Motivation

Stochastic differential equations with superlinearly growing coefficients appear throughout applied probability: population models with cubic damping, Langevin dynamics with polynomial potentials, and stochastic volatility models such as the 3/2-model used for pricing VIX options, whose diffusion coefficient grows like ∣x∣3/2|x|^{3/2}∣x∣3/2. For such equations the classical explicit Euler–Maruyama method fails: Hutzenthaler, Jentzen and Kloeden (2011) proved that its ppp-th moments diverge whenever a coefficient grows superlinearly, so it cannot converge in Lp\mathcal L^pLp. Implicit methods converge (Higham–Mao–Stuart 2002) but cost a nonlinear solve per step.

The tamed Euler schemes are the explicit response.

  • Hutzenthaler, Jentzen and Kloeden (2012) tamed a superlinear drift and proved strong order 1/21/21/2 for globally Lipschitz diffusion coefficients.
  • Sabanis (2013) gave a simpler proof for a family of tamed drifts.
  • Hutzenthaler and Jentzen (2015) treated superlinear diffusion coefficients, obtaining Lp\mathcal L^pLp-convergence without a rate and only for small ppp.
  • Sabanis (2016), the source of this mission, tames drift and diffusion together and proves the optimal strong rate 1/21/21/2 in Lp\mathcal L^pLp under a one-sided (monotonicity) condition and polynomial growth. For the 3/2-model with p1=3.5p_1=3.5p1​=3.5, p0=6p_0=6p0​=6 this gives L2\mathcal L^2L2-convergence with order 1/21/21/2, which earlier results did not cover (p. 2).

This mission is the second of three on the paper. Mission I formalizes Lp\mathcal L^pLp-convergence without a rate (Theorem 1), mission III the uniform-in-time rate (Theorem 3).

Setting

Fix a filtered probability space (Ω,{Ft}t≥0,F,P)(\Omega,\{\mathcal F_t\}_{t\ge0},\mathcal F,P)(Ω,{Ft​}t≥0​,F,P) with right-continuous filtration, a horizon T>0T>0T>0, dimensions d,d1d,d_1d,d1​, and a d1d_1d1​-dimensional Wiener martingale WWW: a standard Brownian motion adapted to {Ft}\{\mathcal F_t\}{Ft​} whose future increments are independent of Ft\mathcal F_tFt​. The coefficients are Borel maps b:[0,∞)×Rd→Rdb:[0,\infty)\times\mathbb R^d\to\mathbb R^db:[0,∞)×Rd→Rd and σ:[0,∞)×Rd→Rd×d1\sigma:[0,\infty)\times\mathbb R^d\to\mathbb R^{d\times d_1}σ:[0,∞)×Rd→Rd×d1​; ∣x∣|x|∣x∣ is the Euclidean norm, ∣A∣|A|∣A∣ the Hilbert–Schmidt norm, xyxyxy the scalar product. The SDE is

dX(t)=b(t,X(t)) dt+σ(t,X(t)) dW(t),t∈[0,T],(2.1)dX(t)=b(t,X(t))\,dt+\sigma(t,X(t))\,dW(t),\qquad t\in[0,T],\qquad(2.1)dX(t)=b(t,X(t))dt+σ(t,X(t))dW(t),t∈[0,T],(2.1)

with an F0\mathcal F_0F0​-measurable initial value X(0)=ξX(0)=\xiX(0)=ξ. For n≥1n\ge1n≥1 let κn(t)=⌊nt⌋/n\kappa_n(t)=\lfloor nt\rfloor/nκn​(t)=⌊nt⌋/n and consider the scheme

dXn(t)=bn(t,Xn(κn(t))) dt+σn(t,Xn(κn(t))) dW(t),Xn(0)=ξ,(2.2)dX_n(t)=b_n(t,X_n(\kappa_n(t)))\,dt+\sigma_n(t,X_n(\kappa_n(t)))\,dW(t),\qquad X_n(0)=\xi,\qquad(2.2)dXn​(t)=bn​(t,Xn​(κn​(t)))dt+σn​(t,Xn​(κn​(t)))dW(t),Xn​(0)=ξ,(2.2)

whose coefficients are frozen at the last grid point, so that XnX_nXn​ is computable step by step. The tamed coefficients of Model 2 are

bn(t,x)=b(t,x)1+n−α∣x∣l,σn(t,x)=σ(t,x)1+n−α∣x∣l.(2.11)–(2.12)b_n(t,x)=\frac{b(t,x)}{1+n^{-\alpha}|x|^l},\qquad \sigma_n(t,x)=\frac{\sigma(t,x)}{1+n^{-\alpha}|x|^l}.\qquad(2.11)\text{–}(2.12)bn​(t,x)=1+n−α∣x∣lb(t,x)​,σn​(t,x)=1+n−α∣x∣lσ(t,x)​.(2.11)–(2.12)

The hypotheses, with constants p0,p1≥2p_0,p_1\ge2p0​,p1​≥2:

  • A-2: bbb is bounded on balls, uniformly in t∈[0,T]t\in[0,T]t∈[0,T].
  • A-4 (coercivity): 2xb(t,x)+(p0−1)∣σ(t,x)∣2≤K(1+∣x∣2)2xb(t,x)+(p_0-1)|\sigma(t,x)|^2\le K(1+|x|^2)2xb(t,x)+(p0​−1)∣σ(t,x)∣2≤K(1+∣x∣2).
  • A-5: E∣X(0)∣p0<∞\mathbb E|X(0)|^{p_0}<\inftyE∣X(0)∣p0​<∞.
  • A-6 (global monotonicity, polynomial growth): for positive lll and LLL, 2(x−y)(b(t,x)−b(t,y))+(p1−1)∣σ(t,x)−σ(t,y)∣2≤L∣x−y∣22(x-y)(b(t,x)-b(t,y))+(p_1-1)|\sigma(t,x)-\sigma(t,y)|^2\le L|x-y|^22(x−y)(b(t,x)−b(t,y))+(p1​−1)∣σ(t,x)−σ(t,y)∣2≤L∣x−y∣2 and ∣b(t,x)−b(t,y)∣≤L(1+∣x∣l+∣y∣l)∣x−y∣|b(t,x)-b(t,y)|\le L(1+|x|^l+|y|^l)|x-y|∣b(t,x)−b(t,y)∣≤L(1+∣x∣l+∣y∣l)∣x−y∣.
  • The p\mathfrak pp-condition: the scheme uses (2.11)–(2.12) with α=1/2\alpha=1/2α=1/2, l≤p0−24l\le\frac{p_0-2}{4}l≤4p0​−2​, and 0<p<p10<p<p_10<p<p1​, p≤p02l+1p\le\frac{p_0}{2l+1}p≤2l+1p0​​.
  • B-2 and B-3 (for the milestones): ∣bn∣≤min⁡(Cnα(1+∣x∣),∣b∣)|b_n|\le\min(Cn^\alpha(1+|x|),|b|)∣bn​∣≤min(Cnα(1+∣x∣),∣b∣), ∣σn∣2≤min⁡(Cnα(1+∣x∣2),∣σ∣2)|\sigma_n|^2\le\min(Cn^\alpha(1+|x|^2),|\sigma|^2)∣σn​∣2≤min(Cnα(1+∣x∣2),∣σ∣2), and A-4 for bn,σnb_n,\sigma_nbn​,σn​ with a constant uniform in nnn.

Formalization targets

Goal: Theorem 2 (p. 6)

Under A-2, A-4–A-6, the p\mathfrak pp-condition and p1>2p_1>2p1​>2, there is a constant CCC independent of nnn with

sup⁡0≤t≤TE[∣X(t)−Xn(t)∣p]≤Cn−p/2(n≥1).(2.13)\sup_{0\le t\le T}\mathbb E\big[|X(t)-X_n(t)|^p\big]\le Cn^{-p/2}\qquad(n\ge1).\qquad(2.13)0≤t≤Tsup​E[∣X(t)−Xn​(t)∣p]≤Cn−p/2(n≥1).(2.13)

The constant is existential and may depend on all data except nnn.

Milestones

  1. Lemma 2 (p. 8): sup⁡tE∣X(t)∣p\sup_t\mathbb E|X(t)|^psupt​E∣X(t)∣p and sup⁡n≥1sup⁡tE∣Xn(t)∣p\sup_{n\ge1}\sup_t\mathbb E|X_n(t)|^psupn≥1​supt​E∣Xn​(t)∣p are finite for 0<p≤p00<p\le p_00<p≤p0​, under A-1–A-5, B-2, B-3.
  2. Lemma 3 (p. 15): for Model 2, E∫0T∣b(s,Xn(κn(s)))−bn(s,Xn(κn(s)))∣p ds≤Cn−αp\mathbb E\int_0^T|b(s,X_n(\kappa_n(s)))-b_n(s,X_n(\kappa_n(s)))|^p\,ds\le Cn^{-\alpha p}E∫0T​∣b(s,Xn​(κn​(s)))−bn​(s,Xn​(κn​(s)))∣pds≤Cn−αp, and the same for σ\sigmaσ.
  3. Lemma 4 (p. 16): sup⁡tE∣Xn(t)−Xn(κn(t))∣p≤Cn−p/2\sup_t\mathbb E|X_n(t)-X_n(\kappa_n(t))|^p\le Cn^{-p/2}supt​E∣Xn​(t)−Xn​(κn​(t))∣p≤Cn−p/2.

Significance

Theorem 2 shows that an explicit scheme costing one coefficient evaluation per step attains the same strong order as the classical Euler method under global Lipschitz conditions. It does so for drift and diffusion coefficients that grow polynomially, and for moment orders ppp that are small relative to p0p_0p0​ and p1p_1p1​. Strong Lp\mathcal L^pLp rates are what multilevel Monte Carlo needs: the variance of level corrections is controlled by the L2\mathcal L^2L2 rate. When lll could be taken to be 000 the statement specializes to the classical globally Lipschitz rate (Remark 6).

The result is proved on paper; it has no machine-checked proof. Stochastic integrals are not in Mathlib; this mission uses the Brownian Itô-integral relation published by the Ethier–Kurtz series on the platform. A formal proof would give the first verified strong convergence rate for any Euler-type scheme. Along the way it produces reusable moment bounds for tamed schemes and the LpL^pLp control of one-step increments.

Difficulty

The obvious argument applies Itô's formula to ∣X−Xn∣p|X-X_n|^p∣X−Xn​∣p and closes a Gronwall inequality. Two steps of it fail without taming. First, the error splits into the monotone part, handled by A-6, and cross terms such as ∣Xn(s)−Xn(κn(s))∣p|X_n(s)-X_n(\kappa_n(s))|^p∣Xn​(s)−Xn​(κn​(s))∣p multiplied by (1+∣Xn∣2l)p/2(1+|X_n|^{2l})^{p/2}(1+∣Xn​∣2l)p/2; they are controlled only through moments of XnX_nXn​ of order well above ppp that are uniform in nnn, which the untamed scheme lacks. Second, the taming itself introduces an error b−bnb-b_nb−bn​ that must be shown to be O(n−1/2)O(n^{-1/2})O(n−1/2) in Lp\mathcal L^pLp and not merely o(1)o(1)o(1). The exponents in the p\mathfrak pp-condition are exactly what the Hölder splittings of these two terms require.

Formalization scope

  • Processes. Solutions are hypotheses, not constructed: XXX solves (2.1) and each XnX_nXn​ solves (2.2), on one probability space, with one WWW and one ξ\xiξ, on [0,T][0,T][0,T] only. An Itô process is a measurable process adapted to the null-set completion of the filtration, with continuous paths on [0,T][0,T][0,T], and a.s. for all t≤Tt\le Tt≤T simultaneously X(t)=ξ+∫0tB ds+∫0tS dWX(t)=\xi+\int_0^t B\,ds+\int_0^t S\,dWX(t)=ξ+∫0t​Bds+∫0t​SdW. The stochastic integral is the platform relation EthierKurtz_HasBrownianItoIntegral, with the integrand cut off after TTT.
  • Expectations and suprema are computed in [0,∞][0,\infty][0,∞] (lower Lebesgue integrals), so no junk value of a non-integrable Bochner integral or of an unbounded real supremum enters. Rates are stated as ≤Cn−p/2\le Cn^{-p/2}≤Cn−p/2 for every n≥1n\ge1n≥1, with CCC real and quantified after all data.
  • Added hypotheses, disclosed. Theorem 2 carries p1>2p_1>2p1​>2: the printed proof covers 2≤p<p12\le p<p_12≤p<p1​ and reduces p<2p<2p<2 to p=2p=2p=2, which the p\mathfrak pp-condition admits exactly when p1>2p_1>2p1​>2. Lemma 4 carries B-3, which its proof uses through Lemma 2. Lemma 2 drops the stated dependence of CCC on (p,T,K,E∣X(0)∣p)(p,T,K,\mathbb E|X(0)|^p)(p,T,K,E∣X(0)∣p) and keeps only its finiteness uniformly in nnn.
  • Ruling out trivialization. The hypotheses are satisfiable, e.g. by b=σ=0b=\sigma=0b=σ=0 with constant solutions and p0=6p_0=6p0​=6, p1=3p_1=3p1​=3, l=1l=1l=1, p=2p=2p=2. The rate is a bound for every n≥1n\ge1n≥1, not an eventual or o(1)o(1)o(1) statement. A proof that uses a constant depending on nnn, or treats only X≡XnX\equiv X_nX≡Xn​, does not prove the goal.
  • Infrastructure needed: Itô's formula for ∣x∣p|x|^p∣x∣p against the platform's Itô integral, the Burkholder–Davis–Gundy inequality (or its Lp\mathcal L^pLp moment form), the zero-expectation property of Itô integrals of square-integrable integrands, and Gronwall's lemma in integral form. These are reusable far beyond this mission, and contributions of any of them are welcome.

Selected references

  • S. Sabanis, Euler approximations with varying coefficients: the case of superlinearly growing diffusion coefficients, Ann. Appl. Probab. 26(4), 2016. https://arxiv.org/abs/1308.1796 (v4)
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong and weak divergence in finite time of Euler's method for stochastic differential equations with non-globally Lipschitz continuous coefficients, Proc. R. Soc. A 467, 2011. https://doi.org/10.1098/rspa.2010.0348
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong convergence of an explicit numerical method for SDEs with non-globally Lipschitz continuous coefficients, Ann. Appl. Probab. 22, 2012. https://mathscinet.ams.org/mathscinet-getitem?mr=MR2985171
  • M. Hutzenthaler, A. Jentzen, Numerical approximations of stochastic differential equations with non-globally Lipschitz continuous coefficients, Mem. Amer. Math. Soc. 236(1112), 2015. https://doi.org/10.1090/memo/1112
  • S. Sabanis, A note on tamed Euler approximations, Electron. Commun. Probab. 18, 2013. https://mathscinet.ams.org/mathscinet-getitem?mr=MR3070913
  • D. J. Higham, X. Mao, A. M. Stuart, Strong convergence of Euler-type methods for nonlinear stochastic differential equations, SIAM J. Numer. Anal. 40, 2002. https://mathscinet.ams.org/mathscinet-getitem?mr=MR1949404
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Numerical AnalysisProbability·Captain: mikedeng1

Euler Approximations with Varying Coefficients I: Lp-Convergence of Explicit Euler Schemes under Local MonotonicityResearch Paper

Motivation

Stochastic differential equations (SDEs) whose coefficients grow faster than linearly appear throughout applied probability: population and epidemic models with cubic damping, Langevin dynamics with non-quadratic potentials, and stochastic volatility models such as the 3/2-model used for pricing VIX options (Goard–Mazur 2013). Their solutions are almost never available in closed form, so they are simulated, and the method of choice is the explicit Euler–Maruyama scheme, because it is cheap and easy to implement.

For superlinearly growing coefficients the classical explicit scheme fails: its moments can diverge even when those of the true solution are finite, so it does not converge in Lp\mathcal L^pLp. Implicit schemes repair this at a higher computational cost (Higham–Mao–Stuart 2002). A second repair is to keep the scheme explicit but modify ("tame") its coefficients by an amount that vanishes as the step size goes to zero.

Timeline.

  • 2002: Higham, Mao and Stuart prove strong convergence of implicit Euler-type methods under a one-sided Lipschitz condition (MR1949404).
  • 2012: Hutzenthaler, Jentzen and Kloeden introduce the tamed Euler scheme for superlinearly growing drift and globally Lipschitz diffusion (Ann. Appl. Probab. 22, MR2985171).
  • 2013: Sabanis gives a short proof of convergence of tamed schemes with rate, again for superlinear drift (Electron. Commun. Probab. 18, MR3070913); Gyöngy and Sabanis prove convergence in probability of Euler approximations under local monotonicity conditions (Appl. Math. Optim. 68, MR3131501).
  • 2015: Hutzenthaler and Jentzen obtain Lp\mathcal L^pLp-convergence of explicit schemes with superlinear diffusion coefficients, in the 3/2-model only for p<1/2p<1/2p<1/2 (Mem. Amer. Math. Soc. 236, no. 1112).
  • 2016: Sabanis treats superlinearly growing drift and diffusion coefficients under a local monotonicity condition, with Lp\mathcal L^pLp-convergence for every p<p0p<p_0p<p0​ (Ann. Appl. Probab. 26, arXiv:1308.1796). This mission formalizes that Lp\mathcal L^pLp-convergence theorem.

Setting

Fix a filtered probability space (Ω,{Ft}t≥0,F,P)(\Omega,\{\mathcal F_t\}_{t\ge0},\mathcal F,P)(Ω,{Ft​}t≥0​,F,P) satisfying the usual conditions, a Wiener martingale WWW in Rd1\mathbb R^{d_1}Rd1​ (a standard Brownian motion adapted to Ft\mathcal F_tFt​ whose future increments are independent of Ft\mathcal F_tFt​), and a horizon T>0T>0T>0. For x∈Rdx\in\mathbb R^dx∈Rd, ∣x∣|x|∣x∣ is the Euclidean norm and xyxyxy the scalar product; for a d×d1d\times d_1d×d1​ matrix, ∣A∣|A|∣A∣ is the Hilbert–Schmidt norm.

The SDE is

dX(t)=b(t,X(t)) dt+σ(t,X(t)) dW(t),t∈[0,T],(2.1)dX(t)=b(t,X(t))\,dt+\sigma(t,X(t))\,dW(t),\qquad t\in[0,T],\tag{2.1}dX(t)=b(t,X(t))dt+σ(t,X(t))dW(t),t∈[0,T],(2.1)

with Borel coefficients b(t,x)∈Rdb(t,x)\in\mathbb R^db(t,x)∈Rd, σ(t,x)∈Rd×d1\sigma(t,x)\in\mathbb R^{d\times d_1}σ(t,x)∈Rd×d1​ and an F0\mathcal F_0F0​-measurable initial value X(0)X(0)X(0).

For n≥1n\ge1n≥1 let κn(t)=⌊nt⌋/n\kappa_n(t)=\lfloor nt\rfloor/nκn​(t)=⌊nt⌋/n, the last grid point of mesh 1/n1/n1/n before ttt. The scheme is

dXn(t)=bn(t,Xn(κn(t))) dt+σn(t,Xn(κn(t))) dW(t),t∈[0,T],(2.2)dX_n(t)=b_n(t,X_n(\kappa_n(t)))\,dt+\sigma_n(t,X_n(\kappa_n(t)))\,dW(t),\qquad t\in[0,T],\tag{2.2}dXn​(t)=bn​(t,Xn​(κn​(t)))dt+σn​(t,Xn​(κn​(t)))dW(t),t∈[0,T],(2.2)

with the same initial value X(0)X(0)X(0) and Borel coefficient sequences bn,σnb_n,\sigma_nbn​,σn​ ("varying coefficients"). Between grid points the coefficients are frozen at Xn(κn(t))X_n(\kappa_n(t))Xn​(κn​(t)), so the scheme is explicit.

The hypotheses, with p0,p1∈[2,∞)p_0,p_1\in[2,\infty)p0​,p1​∈[2,∞): A-1 continuity of bbb in xxx; A-2 local boundedness of bbb; A-3 local monotonicity 2(x−y)(b(t,x)−b(t,y))+(p1−1)∣σ(t,x)−σ(t,y)∣2≤LR∣x−y∣22(x-y)(b(t,x)-b(t,y))+(p_1-1)|\sigma(t,x)-\sigma(t,y)|^2\le L_R|x-y|^22(x−y)(b(t,x)−b(t,y))+(p1​−1)∣σ(t,x)−σ(t,y)∣2≤LR​∣x−y∣2 on ∣x∣,∣y∣≤R|x|,|y|\le R∣x∣,∣y∣≤R; A-4 coercivity 2xb(t,x)+(p0−1)∣σ(t,x)∣2≤K(1+∣x∣2)2xb(t,x)+(p_0-1)|\sigma(t,x)|^2\le K(1+|x|^2)2xb(t,x)+(p0​−1)∣σ(t,x)∣2≤K(1+∣x∣2); A-5 E∣X(0)∣p0<∞\mathbb E|X(0)|^{p_0}<\inftyE∣X(0)∣p0​<∞. For the scheme: B-1 ∫0Tsup⁡∣x∣≤R[∣bn−b∣p0+∣σn−σ∣p0] dt→0\int_0^T\sup_{|x|\le R}[|b_n-b|^{p_0}+|\sigma_n-\sigma|^{p_0}]\,dt\to0∫0T​sup∣x∣≤R​[∣bn​−b∣p0​+∣σn​−σ∣p0​]dt→0 for every RRR; B-2 ∣bn∣≤min⁡(Cnα(1+∣x∣),∣b∣)|b_n|\le\min(Cn^\alpha(1+|x|),|b|)∣bn​∣≤min(Cnα(1+∣x∣),∣b∣) and ∣σn∣2≤min⁡(Cnα(1+∣x∣2),∣σ∣2)|\sigma_n|^2\le\min(Cn^\alpha(1+|x|^2),|\sigma|^2)∣σn​∣2≤min(Cnα(1+∣x∣2),∣σ∣2) for some α∈(0,1/2]\alpha\in(0,1/2]α∈(0,1/2]; B-3 the coercivity bound of A-4 for bn,σnb_n,\sigma_nbn​,σn​, uniformly in nnn.

Formalization targets

Goal: Theorem 1 (p. 5)

Under A-1–A-5 and B-1–B-3 with α∈(0,1/2]\alpha\in(0,1/2]α∈(0,1/2], for every 0<p<p00<p<p_00<p<p0​,

lim⁡n→∞sup⁡0≤t≤TE[∣X(t)−Xn(t)∣p]=0.\lim_{n\to\infty}\sup_{0\le t\le T}\mathbb E\big[|X(t)-X_n(t)|^p\big]=0.n→∞lim​0≤t≤Tsup​E[∣X(t)−Xn​(t)∣p]=0.

No rate is claimed; the statement holds for every coefficient sequence satisfying B-1–B-3, not only for the paper's tamed Models 1 and 2.

Milestones

  • Lemma 1 (p. 7): under A-5, B-2, B-3, sup⁡n≥1sup⁡0≤u≤TE∣Xn(u)∣2<∞\sup_{n\ge1}\sup_{0\le u\le T}\mathbb E|X_n(u)|^2<\inftysupn≥1​sup0≤u≤T​E∣Xn​(u)∣2<∞.
  • Lemma 2 (p. 8): under A-1–A-5, B-2, B-3, for every p≤p0p\le p_0p≤p0​,
sup⁡0≤t≤TE∣X(t)∣p ∨ sup⁡n≥1sup⁡0≤t≤TE∣Xn(t)∣p<∞.\sup_{0\le t\le T}\mathbb E|X(t)|^p\ \vee\ \sup_{n\ge1}\sup_{0\le t\le T}\mathbb E|X_n(t)|^p<\infty.0≤t≤Tsup​E∣X(t)∣p ∨ n≥1sup​0≤t≤Tsup​E∣Xn​(t)∣p<∞.
  • Theorem 4 (p. 6): under A-1–A-4 and B-1, sup⁡0≤t≤T∣Xn(t)−X(t)∣→0\sup_{0\le t\le T}|X_n(t)-X(t)|\to0sup0≤t≤T​∣Xn​(t)−X(t)∣→0 in probability.

Significance

Theorem 1 gives Lp\mathcal L^pLp-convergence of a whole class of explicit schemes, with no global Lipschitz condition on either coefficient, for every ppp below the coercivity order p0p_0p0​. In the 3/2-model of the introduction (p1=3.5p_1=3.5p1​=3.5, p0=6p_0=6p0​=6), earlier explicit results gave Lp\mathcal L^pLp-convergence only for p<1/2p<1/2p<1/2 (Hutzenthaler–Jentzen 2015, §4.10.3); Theorem 1 gives it for all p<6p<6p<6. The theorem is also the qualitative base on which the paper's rate results (Theorems 2 and 3, separate missions of this series) are built, and it justifies Monte Carlo estimates of moments computed with such schemes.

The result is proved in the paper. It has, to our knowledge, no machine-checked proof anywhere; Mathlib has Brownian motion but no stochastic integral, and the Itô integral used here is the relational definition published by the Ethier–Kurtz series on this platform. A formal proof needs Itô's formula for ∣x∣p|x|^p∣x∣p, Gronwall's lemma for moment functions, the convergence in probability of Theorem 4 (which the paper cites from Gyöngy–Sabanis rather than proving), and a uniform-integrability argument. Each of these is reusable well beyond this paper.

Difficulty

The natural first idea, estimating E∣X(t)−Xn(t)∣p\mathbb E|X(t)-X_n(t)|^pE∣X(t)−Xn​(t)∣p directly by Itô's formula and Gronwall, fails: under only local monotonicity the difference of drifts cannot be bounded by ∣X−Xn∣|X-X_n|∣X−Xn​∣ with a constant uniform in the state, so the Gronwall constant blows up. The route through convergence in probability and uniform moment bounds is forced, and the hard step is Lemma 2: bounding E∣Xn(t)∣p0\mathbb E|X_n(t)|^{p_0}E∣Xn​(t)∣p0​ uniformly in nnn. The coefficients of the scheme may grow like nαn^\alphanα, and the frozen argument Xn(κn(s))X_n(\kappa_n(s))Xn​(κn​(s)) produces a correction term E∫∣Xn(s)∣p0−2(Xn(s)−Xn(κn(s)))bn ds\mathbb E\int|X_n(s)|^{p_0-2}(X_n(s)-X_n(\kappa_n(s)))b_n\,dsE∫∣Xn​(s)∣p0​−2(Xn​(s)−Xn​(κn​(s)))bn​ds whose control is exactly where the restriction α≤1/2\alpha\le1/2α≤1/2 enters. For fixed nnn finiteness of moments is easy (linear growth); uniformity in nnn is the content.

Formalization scope

States are EuclideanSpace ℝ (Fin d); diffusion values are EuclideanSpace ℝ (Fin d × Fin d₁), whose norm is the Hilbert–Schmidt norm. Time is ℝ≥0; coefficients are uncurried maps on ℝ≥0 × ℝ^d, assumed Borel measurable. An Itô process on [0,T][0,T][0,T] is a measurable process, adapted to the filtration augmented by all PPP-null sets, with continuous paths on [0,T][0,T][0,T], satisfying the integral equation almost surely simultaneously for all t≤Tt\le Tt≤T; the stochastic integral is the platform relation EthierKurtz.HasBrownianItoIntegral, applied coordinatewise with the integrand cut off after TTT. Nothing is required of the processes after TTT, so no existence beyond the horizon is assumed. Right-continuity of the filtration is a hypothesis; completeness is replaced by adaptedness to the augmented filtration, which is weaker, so the formal theorems are at least as strong as the paper's.

The solutions XXX and (Xn)n≥1(X_n)_{n\ge1}(Xn​)n≥1​ are hypotheses, all on one probability space with one Wiener process and one initial value; the theorems do not construct them. Expectations are lower Lebesgue integrals in [0,∞][0,\infty][0,∞] and suprema over ttt are taken in [0,∞][0,\infty][0,∞], so no statement can hold because an expectation or a supremum takes a default value. B-1's integrand, a supremum over an uncountable ball, is required to be a.e. measurable in ttt, as the paper's Lebesgue integral presupposes. The exponent in Theorem 1 and Lemma 2 is restricted to p>0p>0p>0, the paper's convention for Lp\mathcal L^pLp. The dependence clauses "C:=C(T,K,E∣X(0)∣2)C:=C(T,K,\mathbb E|X(0)|^2)C:=C(T,K,E∣X(0)∣2)" (Lemma 1) and "C:=C(p,T,K,E∣X(0)∣p)C:=C(p,T,K,\mathbb E|X(0)|^p)C:=C(p,T,K,E∣X(0)∣p)" (Lemma 2) are not formalized: only finiteness, i.e. a bound independent of nnn, is stated, which is what the proofs establish. Theorem 4 is stated with exactly its printed hypotheses.

A trivializing formalization, in which the moment bounds or the limit hold because the expectation or the supremum defaults to 000, or because the hypotheses on the solutions cannot be met, is ruled out: all quantities live in [0,∞][0,\infty][0,∞], and a sorry-free check shows every hypothesis is satisfiable (zero coefficients, constant solutions).

Contributions welcome: Itô's formula for the platform's integral relation, Burkholder–Davis–Gundy or Doob inequalities for it, a Gronwall lemma for measurable moment functions, and the Gyöngy–Sabanis convergence-in-probability theorem.

Selected references

  • S. Sabanis, Euler approximations with varying coefficients: the case of superlinearly growing diffusion coefficients, Ann. Appl. Probab. 26(4), 2016. https://arxiv.org/abs/1308.1796 (v4)
  • I. Gyöngy, S. Sabanis, A note on Euler approximations for stochastic differential equations with delay, Appl. Math. Optim. 68, 2013. https://mathscinet.ams.org/mathscinet-getitem?mr=MR3131501
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong convergence of an explicit numerical method for SDEs with non-globally Lipschitz continuous coefficients, Ann. Appl. Probab. 22, 2012. https://mathscinet.ams.org/mathscinet-getitem?mr=MR2985171
  • M. Hutzenthaler, A. Jentzen, Numerical approximations of stochastic differential equations with non-globally Lipschitz continuous coefficients, Mem. Amer. Math. Soc. 236(1112), 2015. https://doi.org/10.1090/memo/1112
  • S. Sabanis, A note on tamed Euler approximations, Electron. Commun. Probab. 18, 2013. https://mathscinet.ams.org/mathscinet-getitem?mr=MR3070913
  • D. J. Higham, X. Mao, A. M. Stuart, Strong convergence of Euler-type methods for nonlinear stochastic differential equations, SIAM J. Numer. Anal. 40, 2002. https://mathscinet.ams.org/mathscinet-getitem?mr=MR1949404
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Exit Problems for Spectrally Negative Lévy Processes and Applications to (Canadized) Russian Options III: Optimal Stopping for the Canadized Russian OptionResearch Paper

Motivation

The Russian option of Shepp and Shiryaev pays its holder, at an exercise time of their choosing, the running maximum of the stock price, discounted, with no fixed maturity. It is the standard example of a perpetual lookback option, and its value is a model problem of optimal stopping for a two-dimensional Markov process (the price and its running maximum). Perpetual contracts are simple to analyse but economically unrealistic: every real contract ends. Canadization (Carr, Randomization and the American put, Rev. Financial Stud. 11, 1998, https://doi.org/10.1093/rfs/11.3.597) replaces a fixed maturity by an independent exponential time η(λ)\eta(\lambda)η(λ). The holder must exercise before η(λ)\eta(\lambda)η(λ); if they have not, they are paid the claim evaluated at η(λ)\eta(\lambda)η(λ). Because the exponential law is memoryless, the problem stays time-homogeneous and its value can be computed in closed form, while it approximates a contract of finite expected life 1/λ1/\lambda1/λ.

Avram, Kyprianou and Pistorius (AKP04) solved both the perpetual and the Canadized Russian problem when the log-price is a spectrally negative Lévy process: a process with stationary independent increments whose only jumps are downward. This covers Brownian motion with drift, the Black–Scholes model, and jump-diffusions with downward jumps (crashes). Their answer is written with the scale functions W(q)W^{(q)}W(q), Z(q)Z^{(q)}Z(q) of the process. This mission is the third of three drawn from that paper, and formalizes the Canadized problem (§7, Theorem 3).

Timeline. Shepp and Shiryaev (1993) solved the Russian option for geometric Brownian motion. Carr (1998) introduced Canadization for the American put. Kyprianou and Pistorius (Ann. Appl. Probab. 13, 2003) studied perpetual options through fluctuation theory; §7 of [AKP04] builds on their calculations. Avram, Kyprianou and Pistorius (2004) solved the perpetual and Canadized problems for general spectrally negative Lévy processes.

Setting

Let (Ω,F,F={Ft}t≥0,P)(\Omega,\mathcal F,\mathbf F=\{\mathcal F_t\}_{t\ge0},\mathbb P)(Ω,F,F={Ft​}t≥0​,P) be a filtered probability space with F\mathbf FF right-continuous, and let X={Xt}t≥0X=\{X_t\}_{t\ge0}X={Xt​}t≥0​ be a spectrally negative Lévy process adapted to F\mathbf FF: X0=0X_0=0X0​=0, paths càdlàg with no upward jumps and not monotone, increments Xs+t−XsX_{s+t}-X_sXs+t​−Xs​ stationary and independent of Fs\mathcal F_sFs​. The standing assumption is that XXX has unbounded variation, or bounded variation and a Lévy measure Λ(dx)≪dx\Lambda(dx)\ll dxΛ(dx)≪dx.

The Laplace exponent is ψ(θ)=log⁡E[eθX1]\psi(\theta)=\log\mathbb E[e^{\theta X_1}]ψ(θ)=logE[eθX1​]. Fix r≥0r\ge0r≥0 with ψ(1)=r\psi(1)=rψ(1)=r, and let P1\mathbb P^1P1 be the Esscher measure, dP1/dP∣Ft=eXt−rtd\mathbb P^1/d\mathbb P|_{\mathcal F_t}=e^{X_t-rt}dP1/dP∣Ft​​=eXt​−rt.

For q≥0q\ge0q≥0 the qqq-scale function W(q):R→[0,∞)W^{(q)}:\mathbb R\to[0,\infty)W(q):R→[0,∞) vanishes on (−∞,0](-\infty,0](−∞,0], is continuous on (0,∞)(0,\infty)(0,∞), and satisfies ∫0∞e−θxW(q)(x) dx=(ψ(θ)−q)−1\int_0^\infty e^{-\theta x}W^{(q)}(x)\,dx=(\psi(\theta)-q)^{-1}∫0∞​e−θxW(q)(x)dx=(ψ(θ)−q)−1 for θ>Φ(q)\theta>\Phi(q)θ>Φ(q), where Φ(q)\Phi(q)Φ(q) is the largest root of ψ(θ)=q\psi(\theta)=qψ(θ)=q. Further, Z(q)(x)=1+q∫−∞xW(q)(y) dyZ^{(q)}(x)=1+q\int_{-\infty}^xW^{(q)}(y)\,dyZ(q)(x)=1+q∫−∞x​W(q)(y)dy. All scale functions in this mission are those of (X,P)(X,\mathbb P)(X,P).

Starting from Y0=z≥0Y_0=z\ge0Y0​=z≥0 (the paper's P−z1\mathbb P^1_{-z}P−z1​), the reflected process is Yt=X‾t−XtY_t=\overline X_t-X_tYt​=Xt​−Xt​, where X‾t=max⁡{0,sup⁡u≤t(−z+Xu)}\overline X_t=\max\{0,\sup_{u\le t}(-z+X_u)\}Xt​=max{0,supu≤t​(−z+Xu​)} and the position is −z+Xt-z+X_t−z+Xt​. Its passage time above kkk is τk=inf⁡{t≥0:Yt∉[0,k)}\tau_k=\inf\{t\ge0:Y_t\notin[0,k)\}τk​=inf{t≥0:Yt​∈/[0,k)}.

Let α>0\alpha>0α>0, and let η(λ)\eta(\lambda)η(λ) be an exponential random variable of rate λ>0\lambda>0λ>0 which under P1\mathbb P^1P1 is independent of F∞\mathcal F_\inftyF∞​. The Canadized Russian problem (32) is

wCR(z)=sup⁡τ E−z1[e−α(τ∧η(λ))+Yτ∧η(λ)],w^{CR}(z)=\sup_\tau\ \mathbb E^1_{-z}\Big[e^{-\alpha(\tau\wedge\eta(\lambda))+Y_{\tau\wedge\eta(\lambda)}}\Big],wCR(z)=τsup​ E−z1​[e−α(τ∧η(λ))+Yτ∧η(λ)​],

over all P1\mathbb P^1P1-a.s. finite F\mathbf FF-stopping times τ\tauτ. Write p=α+λ+rp=\alpha+\lambda+rp=α+λ+r.

Formalization targets

Goal: Theorem 3

With

κ∗=inf⁡{x≥0: Z(p)(x)−pW(p)(x)≤−λ/(p−λ)},h(z)=(p−λ)ezZ(p)(κ∗−z)p+λezp,\kappa_*=\inf\{x\ge0:\ Z^{(p)}(x)-pW^{(p)}(x)\le-\lambda/(p-\lambda)\},\qquad h(z)=\frac{(p-\lambda)e^zZ^{(p)}(\kappa_*-z)}{p}+\frac{\lambda e^z}{p},κ∗​=inf{x≥0: Z(p)(x)−pW(p)(x)≤−λ/(p−λ)},h(z)=p(p−λ)ezZ(p)(κ∗​−z)​+pλez​,

for every z≥0z\ge0z≥0:

wCR(z)=h(z),w^{CR}(z)=h(z),wCR(z)=h(z),

and τκ∗\tau_{\kappa_*}τκ∗​​ is a P1\mathbb P^1P1-a.s. finite F\mathbf FF-stopping time attaining the supremum. The statement covers every variation regime at once.

Milestones

In attack order:

  1. Lemma 2 (i), which gives the monotonicity behind κ∗\kappa_*κ∗​.
  2. Corollary 1 (29), the value of stopping at τk\tau_kτk​ at discount rate α+λ\alpha+\lambdaα+λ.
  3. The elimination of η(λ)\eta(\lambda)η(λ) (display after (32)):
E−z1[e−α(τ∧η)+Yτ∧η]=E−z1[e−(α+λ)τ+Yτ+λ∫0τe−(α+λ)t+Ytdt].\mathbb E^1_{-z}\big[e^{-\alpha(\tau\wedge\eta)+Y_{\tau\wedge\eta}}\big]=\mathbb E^1_{-z}\Big[e^{-(\alpha+\lambda)\tau+Y_\tau}+\lambda\int_0^\tau e^{-(\alpha+\lambda)t+Y_t}dt\Big].E−z1​[e−α(τ∧η)+Yτ∧η​]=E−z1​[e−(α+λ)τ+Yτ​+λ∫0τ​e−(α+λ)t+Yt​dt].
  1. The Itô identity (34).
  2. The expected dX‾d\overline XdX-integral up to τk\tau_kτk​.
  3. Lemma 3 (33), the value of τk∧η(λ)\tau_k\wedge\eta(\lambda)τk​∧η(λ).
  4. Lemma 4, with two misprints corrected.
  5. The supermartingale property of Ut=e−(α+λ)th(Yt)+λ∫0te−(α+λ)u+YuduU_t=e^{-(\alpha+\lambda)t}h(Y_t)+\lambda\int_0^te^{-(\alpha+\lambda)u+Y_u}duUt​=e−(α+λ)th(Yt​)+λ∫0t​e−(α+λ)u+Yu​du.
  6. The identity h(z)=ez+(p−λ)ez∫0κ∗−zW(p)≥ezh(z)=e^z+(p-\lambda)e^z\int_0^{\kappa_*-z}W^{(p)}\ge e^zh(z)=ez+(p−λ)ez∫0κ∗​−z​W(p)≥ez.

Significance

The result. Theorem 3 gives the price and the optimal exercise rule of a Russian option with random (exponential) maturity, for every spectrally negative Lévy model at once. It makes three things explicit. The optimal rule is a threshold rule for the reflected process YYY. The threshold κ∗\kappa_*κ∗​ is the crossing point of one explicit function of the scale functions. Whenever W(p)(0+)≥(p−λ)−1W^{(p)}(0+)\ge(p-\lambda)^{-1}W(p)(0+)≥(p−λ)−1 (possible only with bounded variation), immediate exercise is optimal. Because scale functions are known in closed form for many models, including Brownian motion with drift and hyper-exponential jump-diffusions (§8 of the paper), the theorem produces explicit prices.

Formalizing it. The result is proved on paper. It is not formalized in any proof assistant, and none of its infrastructure is available in Lean. This mission produces:

  • a path-level definition of spectrally negative Lévy processes;
  • scale functions defined as definite descriptions;
  • the reflected process and its passage times;
  • the Esscher change of measure as data;
  • a continuous-time optimal stopping problem with an independent random horizon, valued in [0,∞][0,\infty][0,∞].

A machine-checked proof would also check the verification argument, which the paper states in detail only for the unbounded-variation case.

Difficulty

The obvious route is to compute the value of every threshold rule (Lemma 3) and optimize over kkk. That identifies the right candidate, but it does not show that no other stopping time does better. The verification step needs two things for all regimes of W(p)(0+)W^{(p)}(0+)W(p)(0+): that UUU is a supermartingale, and that UUU stopped at τκ∗\tau_{\kappa_*}τκ∗​​ is a martingale. For processes of bounded variation, hhh is only continuous, not C1C^1C1, at κ∗\kappa_*κ∗​, so a smooth Itô formula does not apply directly. Computing the expected dX‾d\overline XdX-integral up to τk\tau_kτk​ uses excursion theory of YYY away from 000, which Mathlib does not have. Eliminating η(λ)\eta(\lambda)η(λ) is easy only if η\etaη is independent of the whole filtration. If it is independent of XXX alone, a stopping time could depend on η\etaη.

Formalization scope

  • Conventions. Time is [0,∞)[0,\infty)[0,∞) (ℝ≥0) and values are real. Random times take values in WithTop ℝ≥0, and the payoff is 000 on {τ=∞}\{\tau=\infty\}{τ=∞}. Expectations of nonnegative payoffs are lower Lebesgue integrals in [0,∞][0,\infty][0,∞], and wCRw^{CR}wCR is an extended-real supremum, so no expectation defaults to 000. Equalities with a real right-hand side also assert finiteness.
  • Readings of informal words.
    • "The usual conditions" means right-continuity of F\mathbf FF, without completeness. Completing F0\mathcal F_0F0​ with P\mathbb PP-null sets would contradict the Esscher relation, since P1\mathbb P^1P1 and P\mathbb PP are typically singular on F∞\mathcal F_\inftyF∞​.
    • "Unbounded variation" means "not almost surely of bounded variation on compacts". (AC) is stated through jumps.
    • "ψ(v) < ∞" means integrability of evX1e^{vX_1}evX1​.
    • "Decreases monotonically" means strictly decreasing, and "the unique root" means unique on [0,∞)[0,\infty)[0,∞).
    • W(p)(0+)W^{(p)}(0+)W(p)(0+) is the right limit.
    • "Almost surely finite" and the law and independence of η(λ)\eta(\lambda)η(λ) are all under P1\mathbb P^1P1, where independence is from F∞\mathcal F_\inftyF∞​. "Parameter λ\lambdaλ" is the rate.
    • Ps,x1\mathbb P^1_{s,x}Ps,x1​ is encoded pathwise through the reflected process with Y0=s−xY_0=s-xY0​=s−x.
    • The elimination of η\etaη is stated τ by τ, which implies the page's equality of suprema.
    • The supermartingale claim, derived on the page in the unbounded-variation case, is stated for all cases.
    • Corollary 1's discount rate is renamed aaa.
    • (34) is stated as pA+B=es−x+CpA+B=e^{s-x}+CpA+B=es−x+C with AAA, BBB, CCC finite.
  • Definition choices. Scale functions are defined by choice from their defining property, never as hypotheses on an arbitrary function. W(q)W^{(q)}W(q) for q<0q<0q<0 is the series (5), not the tilting formula of Remark 4. P1\mathbb P^1P1 is a measure given with the Esscher relation. dX‾td\overline X_tdXt​ is the Lebesgue–Stieltjes measure of the running-maximum path.
  • Corrected misprints. Lemma 4 is printed with p−1p^{-1}p−1 and −λ/p-\lambda/p−λ/p. The definition of κ∗\kappa_*κ∗​ (p. 233) and the proof of Theorem 3 (p. 235) require (p−λ)−1(p-\lambda)^{-1}(p−λ)−1 and −λ/(p−λ)-\lambda/(p-\lambda)−λ/(p−λ), and the printed version is false when p−1≤W(p)(0+)<(p−λ)−1p^{-1}\le W^{(p)}(0+)<(p-\lambda)^{-1}p−1≤W(p)(0+)<(p−λ)−1. The corrected statement is formalized.
  • Ruled out. A supremum over stopping times of a filtration containing σ(η)\sigma(\eta)σ(η), or a real-valued supremum or Bochner expectation that could be 000 by default, would trivialize the goal or change it. The admissible class is every P1\mathbb P^1P1-a.s. finite stopping time of the given filtration, of which η\etaη is independent. Replacing the goal by the η\etaη-free rewriting would state milestone 3 as if it were Theorem 3.
  • Needed and reusable. A complete development needs Lévy process theory, scale functions, fluctuation identities for the reflected process, optional stopping in continuous time, and Itô or change-of-variable formulas for semimartingales with jumps. The Lévy-process, scale-function and reflected-process definitions are shared with the other two missions of the series and are reusable in ruin theory and queueing. Proofs of any milestone, and sorry-free facts about the definitions, are welcome.

Selected references

  • F. Avram, A. E. Kyprianou, M. R. Pistorius, Exit problems for spectrally negative Lévy processes and applications to (Canadized) Russian options, Ann. Appl. Probab. 14(1), 215–238, 2004. https://doi.org/10.1214/aoap/1075828052
  • P. Carr, Randomization and the American put, Rev. Financial Stud. 11(3), 597–626, 1998. https://doi.org/10.1093/rfs/11.3.597
  • L. A. Shepp, A. N. Shiryaev, The Russian option: reduced regret, Ann. Appl. Probab. 3, 603–631, 1993. https://doi.org/10.1214/aoap/1177005715
  • A. E. Kyprianou, M. R. Pistorius, Perpetual options through fluctuation theory, Ann. Appl. Probab. 13, 1077–1098, 2003. https://doi.org/10.1214/aoap/1060202835
  • J. Bertoin, Lévy Processes, Cambridge University Press, 1996.
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Operations ResearchProbability·Captain: mikedeng1

Diffusion approximations for open queueing networks with service interruptions 2: jump-diffusion heavy-traffic limit for long up and down timesResearch Paper

Motivation

Servers in manufacturing lines, communication links and service systems break down, are taken offline for maintenance, or go on vacation. When the interruptions are rare but long, they dominate congestion. A single down period can build a backlog that takes a long time to clear, and in a network that backlog propagates downstream. Standard heavy-traffic diffusion approximations, which describe queue lengths by reflected Brownian motion, do not capture this effect.

Chen and Whitt (Queueing Systems 13, 1993) identify a regime in which the effect survives in the limit. Up times are of order nnn and down times of order n\sqrt nn​, while the load is within 1/n1/\sqrt n1/n​ of capacity. Under the diffusion scaling each down period then becomes a jump, and the limit of the queue-length process is a reflected jump-diffusion. The paper generalises the single-station result of Kella and Whitt (Adv. Appl. Probab. 22, 1990; reference [22] of the paper) to open networks.

Timeline:

  • 1981: Harrison and Reiman define the multidimensional reflection map on continuous paths (Ann. Probab. 9). Reiman (Math. Oper. Res. 9, 1984) extends it to paths with jumps.
  • 1990: Kella and Whitt prove the one-station jump-diffusion limit for long up and down times.
  • 1991: Chen and Mandelbaum give fluid and diffusion limits of open networks without interruptions (Math. Oper. Res. 16 and Ann. Probab. 19; references [5], [6] of the paper).
  • 1993: Chen and Whitt prove the network case with interruptions (this mission), in Skorohod's M1M_1M1​ topology.

Setting

A network has JJJ single-server stations. Customers arrive from outside station jjj according to a counting process AjA_jAj​. Station jjj completes Sj(t)S_j(t)Sj​(t) services in its first ttt units of busy time. The lllth departure from station kkk is routed to station jjj when the indicator χkj(l)=1\chi_{kj}(l)=1χkj​(l)=1, and Rkj(m)=∑l≤mχkj(l)R_{kj}(m)=\sum_{l\le m}\chi_{kj}(l)Rkj​(m)=∑l≤m​χkj​(l) counts such departures. Station jjj alternates up periods u1j,u2j,…u^j_1,u^j_2,\dotsu1j​,u2j​,… and down periods d1j,d2j,…d^j_1,d^j_2,\dotsd1j​,d2j​,…, starting up, and Dj(t)D_j(t)Dj​(t) is its cumulative down time in [0,t][0,t][0,t]. With a work-conserving discipline, the queue length ZZZ and the busy time BBB satisfy

Zj(t)=Zj(0)+Aj(t)+∑kRkj(Sk(Bk(t)))−Sj(Bj(t)),Bj(t)=∫0t1[Zj(s)>0, j up at s] ds,Z_j(t)=Z_j(0)+A_j(t)+\sum_{k}R_{kj}\big(S_k(B_k(t))\big)-S_j(B_j(t)),\qquad B_j(t)=\int_0^t 1[Z_j(s)>0,\ j\text{ up at }s]\,ds ,Zj​(t)=Zj​(0)+Aj​(t)+k∑​Rkj​(Sk​(Bk​(t)))−Sj​(Bj​(t)),Bj​(t)=∫0t​1[Zj​(s)>0, j up at s]ds,

and the idle time is Yj(t)=t−Dj(t)−Bj(t)Y_j(t)=t-D_j(t)-B_j(t)Yj​(t)=t−Dj​(t)−Bj​(t).

The reflection map (ψ,ϕ)(\psi,\phi)(ψ,ϕ) associated with a matrix QQQ takes a path xxx to the pair (y,z)(y,z)(y,z) with z=x+(I−Q)y≥0z=x+(I-Q)y\ge 0z=x+(I−Q)y≥0, yyy nondecreasing, and yjy_jyj​ increasing only when zj=0z_j=0zj​=0.

A sequence of networks is indexed by nnn. The arrival, service and routing processes satisfy functional central limit theorems with rates λn→λ\lambda^n\to\lambdaλn→λ and μn→μ\mu^n\to\muμn→μ at speed 1/n1/\sqrt n1/n​. Up and down times scale as (ukj,n/n, dkj,n/n)⇒(ukj,dkj)(u^{j,n}_k/n,\ d^{j,n}_k/\sqrt n)\Rightarrow(u^j_k,d^j_k)(ukj,n​/n, dkj,n​/n​)⇒(ukj​,dkj​). The network is balanced, λ=[I−Pt]μ\lambda=[I-P^{\mathsf t}]\muλ=[I−Pt]μ, with PPP the routing matrix. The limit down time D^j(t)\hat D_j(t)D^j​(t) is the sum of dkjd^j_kdkj​ over the up periods completed by time ttt, which is a pure-jump process.

The M1M_1M1​ topology on paths with jumps compares completed graphs, in which each jump is filled in by the straight segment from x(t−)x(t-)x(t−) to x(t)x(t)x(t), through their monotone parametrisations.

Formalization targets

Goal: Theorem 4.1, case J=1J=1J=1

For a single station with feedback probability p∈[0,1)p\in[0,1)p∈[0,1), with Z^n(t)=n−1/2Zn(nt)\hat Z^n(t)=n^{-1/2}Z^n(nt)Z^n(t)=n−1/2Zn(nt), B^n(t)=n−1/2[Bn(nt)−nt]\hat B^n(t)=n^{-1/2}[B^n(nt)-nt]B^n(t)=n−1/2[Bn(nt)−nt], Y^n(t)=n−1/2Yn(nt)\hat Y^n(t)=n^{-1/2}Y^n(nt)Y^n(t)=n−1/2Yn(nt) and D^n(t)=n−1/2Dn(nt)\hat D^n(t)=n^{-1/2}D^n(nt)D^n(t)=n−1/2Dn(nt),

(Z^n,B^n,Y^n,D^n)⇒(Z^,B^,Y^,D^)in D((0,∞),R4,M1).(\hat Z^n,\hat B^n,\hat Y^n,\hat D^n)\Rightarrow(\hat Z,\hat B,\hat Y,\hat D)\quad\text{in }D((0,\infty),\mathbb R^{4},M_1).(Z^n,B^n,Y^n,D^n)⇒(Z^,B^,Y^,D^)in D((0,∞),R4,M1​).

Here Z^=ϕ(X^)\hat Z=\phi(\hat X)Z^=ϕ(X^), Y^=μ−1ψ(X^)\hat Y=\mu^{-1}\psi(\hat X)Y^=μ−1ψ(X^) and B^=−D^−Y^\hat B=-\hat D-\hat YB^=−D^−Y^, with Q=pQ=pQ=p and

X^(t)=Z^(0)+ξ^(t)+(cλ−(1−p)cμ)t+(1−p)μD^(t).\hat X(t)=\hat Z(0)+\hat\xi(t)+\big(c_\lambda-(1-p)c_\mu\big)t+(1-p)\mu\hat D(t).X^(t)=Z^(0)+ξ^​(t)+(cλ​−(1−p)cμ​)t+(1−p)μD^(t).

The paper states Theorem 4.1 for JJJ stations, with the analogous formulas and Q=PtQ=P^{\mathsf t}Q=Pt. The mission's goal is its case J=1J=1J=1 (see Formalization scope).

Milestones

  1. Lemma 4.1: D^n⇒D^\hat D^n\Rightarrow\hat DD^n⇒D^ in D((0,∞),RJ,M1)D((0,\infty),\mathbb R^J,M_1)D((0,∞),RJ,M1​).
  2. Lemma 4.2: n−1Bjn(nt)→tn^{-1}B^n_j(nt)\to tn−1Bjn​(nt)→t u.o.c.
  3. Eq. (4.24): n−1/2ξn(nt)→ξ^(t)n^{-1/2}\xi^n(nt)\to\hat\xi(t)n−1/2ξn(nt)→ξ^​(t) u.o.c.
  4. Eqs. (4.28)–(4.29): (n−1/2Xn(nt), n−1/2Dn(nt))→(X^,D^)\big(n^{-1/2}X^n(nt),\,n^{-1/2}D^n(nt)\big)\to(\hat X,\hat D)(n−1/2Xn(nt),n−1/2Dn(nt))→(X^,D^) jointly in M1M_1M1​.
  5. The almost-sure form of Theorem 4.1 on a Skorohod representation space, case J=1J=1J=1.

Significance

The theorem yields a tractable approximation for networks with rare long interruptions: a reflected Lévy-type process driven by a Brownian part and a compound jump part. Its distribution can be studied through the reflection map. The jump directions [I−Pt]diag⁡(μ)ej[I-P^{\mathsf t}]\operatorname{diag}(\mu)e_j[I−Pt]diag(μ)ej​ make explicit how an outage at one station drains its downstream stations while its own queue builds up. Remark (4.3) of the paper derives a diffusion analogue of Little's law from the same limit.

The theorem is proved in the paper, and no part of it has been formalized. A formalization would produce the first machine-checked M1M_1M1​ topology on paths with jumps, a heavy-traffic limit theorem for a queueing network, and the random-time-change argument for counting processes.

Difficulty

The obvious argument chains three facts: the primitive processes converge, hence so does the scaled free process XXX, and the reflection map is continuous. Two steps break. First, subtraction is not continuous in M1M_1M1​ when the two paths jump at the same time in opposite directions, so the joint convergence of D^n\hat D^nD^n across stations needs (4.11) and one common parametrisation. Second, the reflection map is Lipschitz in the uniform topology, but the uniform topology cannot see jumps that occur at nearby times. Carrying the convergence through the reflection map in the M1M_1M1​ topology requires controlling how the regulator and the regulated process move along each jump segment of X^\hat XX^, jointly for all coordinates.

Formalization scope

Stations are Fin J; the network index is n : ℕ, and only n→∞n\to\inftyn→∞ enters. Durations are indexed from 000 in Lean. The queue length is integer valued, (3.2) is computed in Z\mathbb ZZ, and a solution satisfies Z≥0Z\ge 0Z≥0.

  • Solutions, not constructions. Every statement quantifies over all solutions (Zn,Bn)(Z^n,B^n)(Zn,Bn) of (3.2)–(3.3) and all reflection pairs of X^\hat XX^. Existence and uniqueness are asserted in the paper by citation and are not assumed or proved here.
  • M1M_1M1​. Parametric representations are monotone in the order of the completed graph, which is the standard definition. The page states only that the time component is nondecreasing. Convergence on (0,∞)(0,\infty)(0,∞) means convergence on every [a,b][a,b][a,b] with 0<a<b0<a<b0<a<b continuity points of the limit. Jump segments are segments in Rd\mathbb R^dRd (strong M1M_1M1​). Convergence in D((0,∞),⋅,M1)D((0,\infty),\cdot,M_1)D((0,∞),⋅,M1​) includes the requirement that every path be càdlàg on (0,∞)(0,\infty)(0,∞), so a copy of the limit that is continuous nowhere cannot satisfy the continuity-point condition vacuously.
  • Weak convergence is in coupling form: one probability space carries copies with the right laws that converge almost surely. The limits in (4.1)–(4.4) are continuous, so there the mode is u.o.c.
  • Corrected printed errors. Lemma 4.2 is stated with n−1n^{-1}n−1 in place of the printed n−1/2n^{-1/2}n−1/2, as in its proof. The map on p. 346 is read as ϕ(X)=Z\phi(X)=Zϕ(X)=Z, ψ(X)=diag⁡(μ)Y\psi(X)=\operatorname{diag}(\mu)Yψ(X)=diag(μ)Y, following (4.13). The reflection map allows y(0)≥0y(0)\ge 0y(0)≥0, because X^(0)\hat X(0)X^(0) may leave the orthant when D^(0)>0\hat D(0)>0D^(0)>0; when x(0)≥0x(0)\ge 0x(0)≥0 this agrees with (2.2).
  • Added hypotheses. The processes Zn,Bn,Z^,Y^Z^n,B^n,\hat Z,\hat YZn,Bn,Z^,Y^ are assumed to be stochastic processes (measurable at each time). All networks share one probability space, so that the routing is literally common. No independence is assumed.
  • The goal is the case J=1J=1J=1 of Theorem 4.1. The printed theorem claims strong M1M_1M1​ convergence, with one parametric representation for all 4J4J4J coordinates, for every JJJ. For J≥2J\ge 2J≥2 that claim fails: during an upstream outage, a downstream queue that empties part-way through the jump bends the prelimit graph of (D^j,Y^k)(\hat D_j,\hat Y_k)(D^j​,Y^k​), while the limit's completed graph is a straight segment. For J=1J=1J=1 every coordinate moves linearly through each jump. The milestones Lemma 4.1, Lemma 4.2, (4.24) and (4.28)–(4.29) are stated for general JJJ, and the almost-sure core of the proof for J=1J=1J=1.

A trivializing formalization is excluded. The hypotheses are satisfiable (for example by deterministic arrival and service processes), N^\hat NN^ is used only when ∑kukj=∞\sum_ku^j_k=\infty∑k​ukj​=∞, and laws are compared only for measurable path maps.

Needed infrastructure: the Skorohod space with the M1M_1M1​ topology and its characterization on (0,∞)(0,\infty)(0,∞), continuity of addition and of composition with continuous time changes, the multidimensional reflection map on paths with jumps, and a Skorohod representation argument. Proofs of Lemma 4.1 and Lemma 4.2 are welcome independently.

Selected references

  • H. Chen, W. Whitt, Diffusion approximations for open queueing networks with service interruptions, Queueing Systems 13 (1993) 335–359. https://doi.org/10.1007/BF01149260
  • O. Kella, W. Whitt, Diffusion approximations for queues with server vacations, Adv. Appl. Probab. 22 (1990) 706–729 (reference [22] of the paper).
  • J. M. Harrison, M. I. Reiman, Reflected Brownian motion on an orthant, Ann. Probab. 9 (1981) 302–308. https://doi.org/10.1214/aop/1176994472
  • H. Chen, A. Mandelbaum, Discrete flow networks: diffusion approximations and bottlenecks, Ann. Probab. 19 (1991) 1463–1519 (reference [6] of the paper).
  • M. I. Reiman, Open queueing networks in heavy traffic, Math. Oper. Res. 9 (1984) 441–458 (reference [25] of the paper).
  • W. Whitt, Some useful functions for functional limit theorems, Math. Oper. Res. 5 (1980) 67–85. https://doi.org/10.1287/moor.5.1.67
  • A. V. Skorohod, Limit theorems for stochastic processes, Theory Probab. Appl. 1 (1956) 261–290. https://doi.org/10.1137/1101022
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Control TheoryDynamical SystemsOperations Research+1·Captain: mikedeng1

Stabilization of Hybrid Systems by Feedback Control Based on Discrete-Time State Observations II: Mean-Square and Almost Sure Exponential StabilityResearch Paper

Motivation

Many engineered systems switch between a finite number of operating modes at random times: a power grid after a line failure, a networked controller whose links drop, a manufacturing plant whose machines break down and are repaired. A standard model for such systems is a hybrid stochastic differential equation, also called an SDE with Markovian switching: the state follows an Itô equation whose coefficients depend on a mode that evolves as a continuous-time Markov chain. The monograph of Mao and Yuan (Stochastic Differential Equations with Markovian Switching, 2006) develops the stability theory of these equations.

A controller that stabilizes such a system usually needs the current state. In practice the state is sampled: it is observed at times 0,τ,2τ,…0,\tau,2\tau,\dots0,τ,2τ,… and the control is held between observations. Mao (Automatica 49, 2013) showed that, under a global Lipschitz condition on the drift and diffusion, a feedback control based on discrete-time observations makes a hybrid SDE mean-square exponentially stable when τ\tauτ is small enough. You, Liu, Lu, Mao and Qiu (SIAM J. Control Optim. 53(2), 2015) replaced that condition by local Lipschitz continuity plus linear growth, gave an explicit bound (3.5) on the admissible observation interval, and proved H∞H_\inftyH∞​-stability, asymptotic stability, and, in Section 4, exponential stability in mean square and almost surely with an explicit rate. This mission formalizes that exponential stability result, Theorem 4.2, and the steps of its proof.

Setting

Let (Ω,F,{Ft}t≥0,P)(\Omega,\mathcal F,\{\mathcal F_t\}_{t\ge0},\mathbb P)(Ω,F,{Ft​}t≥0​,P) be a probability space with a filtration satisfying the usual conditions (increasing, right-continuous, F0\mathcal F_0F0​ contains the null sets). On it live an mmm-dimensional {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion www and a right-continuous {Ft}\{\mathcal F_t\}{Ft​}-Markov chain rrr on S={1,…,N}S=\{1,\dots,N\}S={1,…,N} with generator Γ=(γij)\Gamma=(\gamma_{ij})Γ=(γij​) (γij≥0\gamma_{ij}\ge0γij​≥0 for i≠ji\ne ji=j, zero row sums), independent of www. Fix τ>0\tau>0τ>0 and the sampling time δt=[t/τ]τ\delta_t=[t/\tau]\tauδt​=[t/τ]τ. The controlled system is

dx(t)=(f(x(t),r(t),t)+u(x(δt),r(t),t))dt+g(x(t),r(t),t) dw(t),x(0)=x0, r(0)=r0,(2.1)dx(t)=\big(f(x(t),r(t),t)+u(x(\delta_t),r(t),t)\big)dt+g(x(t),r(t),t)\,dw(t),\qquad x(0)=x_0,\ r(0)=r_0,\tag{2.1}dx(t)=(f(x(t),r(t),t)+u(x(δt​),r(t),t))dt+g(x(t),r(t),t)dw(t),x(0)=x0​, r(0)=r0​,(2.1)

with f,u:Rn×S×R+→Rnf,u:\mathbb R^n\times S\times\mathbb R_+\to\mathbb R^nf,u:Rn×S×R+​→Rn and g:Rn×S×R+→Rn×mg:\mathbb R^n\times S\times\mathbb R_+\to\mathbb R^{n\times m}g:Rn×S×R+​→Rn×m.

The hypotheses are:

  • Assumption 2.1: f,gf,gf,g locally Lipschitz in xxx, and ∣f(x,i,t)∣≤K1∣x∣|f(x,i,t)|\le K_1|x|∣f(x,i,t)∣≤K1​∣x∣, ∣g(x,i,t)∣≤K2∣x∣|g(x,i,t)|\le K_2|x|∣g(x,i,t)∣≤K2​∣x∣ (∣g∣|g|∣g∣ the trace norm).
  • Assumption 2.2: ∣u(x,i,t)−u(y,i,t)∣≤K3∣x−y∣|u(x,i,t)-u(y,i,t)|\le K_3|x-y|∣u(x,i,t)−u(y,i,t)∣≤K3​∣x−y∣ and u(0,i,t)=0u(0,i,t)=0u(0,i,t)=0.
  • Assumption 3.1: there are U∈C2,1(Rn×S×R+;R+)U\in C^{2,1}(\mathbb R^n\times S\times\mathbb R_+;\mathbb R_+)U∈C2,1(Rn×S×R+​;R+​) and λ1,λ2>0\lambda_1,\lambda_2>0λ1​,λ2​>0 with LU(x,i,t)+λ1∣Ux(x,i,t)∣2≤−λ2∣x∣2\mathcal LU(x,i,t)+\lambda_1|U_x(x,i,t)|^2\le-\lambda_2|x|^2LU(x,i,t)+λ1​∣Ux​(x,i,t)∣2≤−λ2​∣x∣2, where
LU=Ut+Ux[f+u]+12trace⁡[gTUxxg]+∑jγijU(x,j,t).\mathcal LU=U_t+U_x[f+u]+\tfrac12\operatorname{trace}[g^TU_{xx}g]+\sum_j\gamma_{ij}U(x,j,t).LU=Ut​+Ux​[f+u]+21​trace[gTUxx​g]+j∑​γij​U(x,j,t).
  • Assumption 4.1: c1∣x∣2≤U(x,i,t)≤c2∣x∣2c_1|x|^2\le U(x,i,t)\le c_2|x|^2c1​∣x∣2≤U(x,i,t)≤c2​∣x∣2 with c1,c2>0c_1,c_2>0c1​,c2​>0.
  • Condition (3.5): λ2>τK32λ1[2τ(K12+2K32)+K22]\lambda_2>\frac{\tau K_3^2}{\lambda_1}\big[2\tau(K_1^2+2K_3^2)+K_2^2\big]λ2​>λ1​τK32​​[2τ(K12​+2K32​)+K22​] and τ≤14K3\tau\le\frac1{4K_3}τ≤4K3​1​.

Put θ=K32/λ1\theta=K_3^2/\lambda_1θ=K32​/λ1​, λ=λ2−θτ[2τ(K12+2K32)+K22]\lambda=\lambda_2-\theta\tau[2\tau(K_1^2+2K_3^2)+K_2^2]λ=λ2​−θτ[2τ(K12​+2K32​)+K22​] (positive by (3.5)), and

H1=θτ(2τ(K12+2K32)+K22)+24θτ4K341−6τ2K32,H2=12θτ2K32(τK12+K22)1−6τ2K32.H_1=\theta\tau\big(2\tau(K_1^2+2K_3^2)+K_2^2\big)+\frac{24\theta\tau^4K_3^4}{1-6\tau^2K_3^2},\qquad H_2=\frac{12\theta\tau^2K_3^2(\tau K_1^2+K_2^2)}{1-6\tau^2K_3^2}.H1​=θτ(2τ(K12​+2K32​)+K22​)+1−6τ2K32​24θτ4K34​​,H2​=1−6τ2K32​12θτ2K32​(τK12​+K22​)​.

In Lean these are Assumption21, Assumption22, C21, LU, Assumption31, Assumption41, Condition35, theta, lam, H1, H2, rateEquationLHS; the basis is HybridSetup, the Itô integral IsItoIntegral, the sampling time delta, solutions SolvesSampledHybridSDE, and the functional (4.7) Vbar, all in the namespace You2015.Expo.

Formalization targets

Goal: Theorem 4.2 (exponential stability)

Under the hypotheses above, the equation

2τγe2τγ(H1+τH2)+γc2=λ(4.4)2\tau\gamma e^{2\tau\gamma}(H_1+\tau H_2)+\gamma c_2=\lambda\tag{4.4}2τγe2τγ(H1​+τH2​)+γc2​=λ(4.4)

has a unique root γ>0\gamma>0γ>0, and every solution of (2.1) satisfies

lim sup⁡t→∞1tlog⁡(E∣x(t)∣2)≤−γ,lim sup⁡t→∞1tlog⁡∣x(t)∣≤−γ2a.s.\limsup_{t\to\infty}\frac1t\log\big(\mathbb E|x(t)|^2\big)\le-\gamma,\qquad\limsup_{t\to\infty}\frac1t\log|x(t)|\le-\frac\gamma2\quad\text{a.s.}t→∞limsup​t1​log(E∣x(t)∣2)≤−γ,t→∞limsup​t1​log∣x(t)∣≤−2γ​a.s.

for all x0∈Rnx_0\in\mathbb R^nx0​∈Rn, r0∈Sr_0\in Sr0​∈S.

Milestones, in the order the proof uses them

  1. (3.15) E∣x(t)−x(δt)∣2≤2E∫δtt[τ∣f+u(x(δs),⋅)∣2+∣g∣2]ds\mathbb E|x(t)-x(\delta_t)|^2\le2\mathbb E\int_{\delta_t}^t[\tau|f+u(x(\delta_s),\cdot)|^2+|g|^2]dsE∣x(t)−x(δt​)∣2≤2E∫δt​t​[τ∣f+u(x(δs​),⋅)∣2+∣g∣2]ds.
  2. Theorem 3.2 (H∞H_\inftyH∞​-stability): ∫0∞E∣x(s)∣2ds<∞\int_0^\infty\mathbb E|x(s)|^2ds<\infty∫0∞​E∣x(s)∣2ds<∞.
  3. (3.21) E∣x(s)−x(δs)∣2≤3(τK12+K22)1−6τ2K32∫δssE∣x(z)∣2dz+6τ2K321−6τ2K32E∣x(s)∣2\mathbb E|x(s)-x(\delta_s)|^2\le\frac{3(\tau K_1^2+K_2^2)}{1-6\tau^2K_3^2}\int_{\delta_s}^s\mathbb E|x(z)|^2dz+\frac{6\tau^2K_3^2}{1-6\tau^2K_3^2}\mathbb E|x(s)|^2E∣x(s)−x(δs​)∣2≤1−6τ2K32​3(τK12​+K22​)​∫δs​s​E∣x(z)∣2dz+1−6τ2K32​6τ2K32​​E∣x(s)∣2.
  4. (4.11) EVˉ(x^z,r^z,z)≤(H1+τH2)∫z−2τzE∣x(y)∣2dy\mathbb E\bar V(\hat x_z,\hat r_z,z)\le(H_1+\tau H_2)\int_{z-2\tau}^z\mathbb E|x(y)|^2dyEVˉ(x^z​,r^z​,z)≤(H1​+τH2​)∫z−2τz​E∣x(y)∣2dy for z≥2τz\ge2\tauz≥2τ.
  5. (4.14) c1eγtE∣x(t)∣2≤Cc_1e^{\gamma t}\mathbb E|x(t)|^2\le Cc1​eγtE∣x(t)∣2≤C for t≥2τt\ge2\taut≥2τ.
  6. (4.14) ⇒\Rightarrow⇒ (4.3), the mean-square-to-almost-sure transfer cited from Mao–Yuan [23, Theorem 8.8].

Significance

The result. Theorem 4.2 gives a quantitative guarantee: a controller that samples the state every τ\tauτ units makes the switching system decay exponentially, with a rate γ\gammaγ computable from the constants of the assumptions. Asymptotic stability (Section 3 of the paper) says nothing about how fast trajectories settle; the rate is what a designer trades against the sampling cost when choosing τ\tauτ. The almost sure statement concerns individual trajectories, which is what an operator observes.

Formalizing it. The results are proved in the paper; none of them is machine-checked. Mathlib has real Brownian motion but no Itô integral, no stochastic differential equations and no continuous-time Markov chains. The mission therefore also produces a definition layer: a filtration under the usual conditions, a multidimensional {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion, an {Ft}\{\mathcal F_t\}{Ft​}-Markov chain with a given generator, the L2L^2L2 Itô integral of vector-valued integrands, and the solution notion of an SDE with Markovian switching and a sampled-state delay. A related but different layer exists on Prove2Me for Ethier–Kurtz (EthierKurtz_IsStandardBrownian, EthierKurtz_HasBrownianItoIntegral, EthierKurtz_SolvesBrownianSDE); it has no mode switching and no sampled state, so it cannot express (2.1). Formalization also checks the constants: it found that the printed H1H_1H1​ in (4.5) disagrees with the paper's own derivation (see below).

Difficulty

Equation (2.1) is a stochastic differential delay equation whose delay t−δtt-\delta_tt−δt​ is bounded but jumps at every observation time, so the delay-equation stability theorems that require a differentiable delay with derivative below one (Mao–Yuan, p. 285) do not apply. A Lyapunov function of the current state alone leaves the term Ux[u(x(t))−u(x(δt))]U_x[u(x(t))-u(x(\delta_t))]Ux​[u(x(t))−u(x(δt​))], which has no sign and depends on the path over a whole observation interval. An exponential rate requires controlling this delay term with an exponential weight, and the weight inflates the delay contribution by a factor e2τγe^{2\tau\gamma}e2τγ; the rate equation (4.4) records exactly this balance. The almost sure part does not follow from the mean-square part by Chebyshev's inequality at fixed times alone: a pathwise bound needs control of the supremum of ∣x∣|x|∣x∣ over each unit interval, which involves the martingale part of the solution.

Formalization scope

Conventions committed to in Lean:

  • The state space is EuclideanSpace ℝ (Fin n), so ∣x∣|x|∣x∣ is the Euclidean norm; the explicit constants in (3.5), (3.21), (4.5) depend on it. The diffusion ggg is given by its mmm columns and ∣g∣2=∑k∣gk∣2|g|^2=\sum_k|g_k|^2∣g∣2=∑k​∣gk​∣2 (trace norm). Modes are Fin N (0-based). Time is ℝ≥0; time integrals are over subsets of R\mathbb RR at s.toNNReal.
  • Every expectation of a nonnegative quantity (E∣x∣2\mathbb E|x|^2E∣x∣2, EVˉ\mathbb E\bar VEVˉ) and every time integral of one is a lower Lebesgue integral in [0,∞][0,\infty][0,∞], so a non-integrable process cannot produce a junk value 000.
  • Logarithms. The paper's log⁡\loglog takes the value −∞-\infty−∞ at 000. For a finite a(t)≥0a(t)\ge0a(t)≥0, lim sup⁡t→∞1tlog⁡a(t)≤−γ\limsup_{t\to\infty}\frac1t\log a(t)\le-\gammalimsupt→∞​t1​loga(t)≤−γ is stated in the equivalent form "for every γ′<γ\gamma'<\gammaγ′<γ, eventually a(t)≤e−γ′ta(t)\le e^{-\gamma't}a(t)≤e−γ′t". Lean's Real.log 0 = 0 never enters. In (4.3) the almost-sure quantifier is outside the quantifier over γ′\gamma'γ′.
  • Correction of (4.5). The page prints the last term of H1H_1H1​ as 24τ3K34/(1−6τ2K32)24\tau^3K_3^4/(1-6\tau^2K_3^2)24τ3K34​/(1−6τ2K32​). Substituting (3.21) into (4.9), as the proof does, gives 24θτ4K34/(1−6τ2K32)24\theta\tau^4K_3^4/(1-6\tau^2K_3^2)24θτ4K34​/(1−6τ2K32​) (the same computation reproduces the printed H2H_2H2​). The mission uses the corrected H1H_1H1​ in the goal, (4.11) and (4.14). With the printed value the claimed rate could exceed what the proof yields whenever θτ>1\theta\tau>1θτ>1.
  • "The unique root" is a conjunct of the goal (∃! γ>0\exists!\,\gamma>0∃!γ>0); the stability conclusions are stated for every positive root. "(so λ>0\lambda>0λ>0)" is a consequence of (3.5), not a hypothesis. (4.4) is kept as an equality.
  • "The solution of (2.1)" is read as every process satisfying the solution definition: progressively measurable, almost surely continuous paths, E∣x(t)∣2<∞\mathbb E|x(t)|^2<\inftyE∣x(t)∣2<∞ for each ttt, and for each ttt, almost surely, the integral equation with Itô integrals in the L2L^2L2 sense. Existence and uniqueness (cited from Mao–Yuan on p. 908) are not asserted.
  • "An mmm-dimensional Brownian motion" and "a Markov chain with generator Γ\GammaΓ" are read in the Mao–Yuan framework the paper cites: an {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion with independent coordinates and increments independent of the past, and an {Ft}\{\mathcal F_t\}{Ft​}-Markov chain with transition matrix etΓe^{t\Gamma}etΓ. The usual conditions are kept as hypotheses.
  • "Locally Lipschitz" is uniform in the mode and time on each ball. C2,1C^{2,1}C2,1 carries its derivatives Ut,Ux,UxxU_t,U_x,U_{xx}Ut​,Ux​,Uxx​ as witnesses tied to UUU by derivative relations and joint continuity.
  • "τ>0\tau>0τ>0 sufficiently small for (3.5)" means every τ>0\tau>0τ>0 satisfying both inequalities of (3.5). U,λ1,λ2,c1,c2,τU,\lambda_1,\lambda_2,c_1,c_2,\tauU,λ1​,λ2​,c1​,c2​,τ are data. The constant CCC of (4.14) is chosen after x0x_0x0​, r0r_0r0​, the solution and γ\gammaγ, and before ttt.
  • (3.15), (3.21) and the transfer (4.14) ⇒\Rightarrow⇒ (4.3) are stated under fewer hypotheses than the surrounding proof has (Assumptions 2.1, 2.2, τ>0\tau>0τ>0, and for (3.21) τ≤1/(4K3)\tau\le1/(4K_3)τ≤1/(4K3​)), because their derivations use no more. Vˉ\bar VVˉ of (4.7) is used only for z≥2τz\ge2\tauz≥2τ, where no extension of the solution to negative times is needed. Other misprints on the page (g(x,i,s)=f(x,i,0)g(x,i,s)=f(x,i,0)g(x,i,s)=f(x,i,0) on p. 909, V(x^0,r^0,t)V(\hat x_0,\hat r_0,t)V(x^0​,r^0​,t) for V(x^0,r^0,0)V(\hat x_0,\hat r_0,0)V(x^0​,r^0​,0) on p. 918, the swapped ∨,∧\vee,\wedge∨,∧ on p. 907) are not formalized.

A trivializing formalization is ruled out: the expectations are not Bochner integrals, log⁡0\log 0log0 is never evaluated, the goal asserts that the rate equation has exactly one positive root (so the stability clauses are not vacuous), the solution notion admits the true solution and requires path continuity, and the derivative witnesses of UUU are tied to UUU. A sorry-free local check confirms that Assumptions 2.1, 2.2, 4.1, condition (3.5) and λ>0\lambda>0λ>0 hold for n=m=N=1n=m=N=1n=m=N=1, f=g=0f=g=0f=g=0, u(x)=−xu(x)=-xu(x)=−x, U=∣x∣2U=|x|^2U=∣x∣2, K1=K2=K3=1K_1=K_2=K_3=1K1​=K2​=K3​=1, λ1=1/4\lambda_1=1/4λ1​=1/4, λ2=1\lambda_2=1λ2​=1, c1=c2=1c_1=c_2=1c1​=c2​=1, τ=1/10\tau=1/10τ=1/10; for these data LU+λ1∣Ux∣2=−∣x∣2\mathcal LU+\lambda_1|U_x|^2=-|x|^2LU+λ1​∣Ux​∣2=−∣x∣2 by hand.

Welcome contributions: the Itô isometry and Itô's formula for the L2L^2L2 integral defined here, a generalized Itô formula for functions of a Markov-modulated Itô process, the Burkholder–Davis–Gundy inequality, and the Borel–Cantelli argument that turns mean-square exponential decay into almost sure decay. These are reusable far beyond this mission. Section 3 of the paper (asymptotic stability) is a separate mission of the same series.

Selected references

  • S. You, W. Liu, J. Lu, X. Mao, Q. Qiu, Stabilization of Hybrid Systems by Feedback Control Based on Discrete-Time State Observations, SIAM J. Control Optim. 53(2), 905–925, 2015. https://doi.org/10.1137/140985779
  • X. Mao, C. Yuan, Stochastic Differential Equations with Markovian Switching, Imperial College Press, 2006. https://doi.org/10.1142/p473
  • X. Mao, Stabilization of continuous-time hybrid stochastic differential equations by discrete-time feedback control, Automatica 49(12), 3677–3681, 2013. https://doi.org/10.1016/j.automatica.2013.09.005
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Dynamic ProgrammingOperations ResearchProbability·Captain: mikedeng1

Exit Problems for Spectrally Negative Lévy Processes and Applications to (Canadized) Russian Options II: Optimal Stopping for the Perpetual Russian OptionResearch Paper

Motivation

A Russian option is a perpetual American-type claim that pays, when the holder exercises at time τ\tauτ, the maximum of the asset price seen so far, discounted by e−ατe^{-\alpha\tau}e−ατ. It was introduced by Shepp and Shiryaev for the Black–Scholes market (Shepp–Shiryaev 1993), where the underlying log-price is a Brownian motion with drift. Empirical work on asset returns (skewness, heavy tails, downward jumps) motivates replacing the Brownian motion by a Lévy process with negative jumps only. Avram, Kyprianou and Pistorius (2004) solve the Russian optimal stopping problem in that model in closed form, in terms of the scale functions of the process.

Timeline. 1993: Shepp and Shiryaev solve the Russian problem for geometric Brownian motion; Duffie and Harrison give its no-arbitrage price. Graversen and Peskir, and Kyprianou and Pistorius, treat further variants within the Black–Scholes market (the works the paper cites in §6). 2004: Avram, Kyprianou and Pistorius solve it for every spectrally negative Lévy process, covering both unbounded and bounded variation, using the exit problem of the reflected process Y=X‾−XY=\overline X-XY=X−X (their Theorem 1, the subject of the first mission of this series).

Setting

Let (Ω,F,F={Ft}t≥0,P)(\Omega,\mathcal F,\mathbf F=\{\mathcal F_t\}_{t\ge0},\mathbb P)(Ω,F,F={Ft​}t≥0​,P) be a filtered probability space with a right-continuous filtration, and X={Xt, t≥0}X=\{X_t,\ t\ge0\}X={Xt​, t≥0} a spectrally negative Lévy process for F\mathbf FF: X0=0X_0=0X0​=0, càdlàg paths with no positive jumps, independent and stationary increments with Xs+t−XsX_{s+t}-X_sXs+t​−Xs​ independent of Fs\mathcal F_sFs​, and paths that are not monotone. The standing assumption of the paper is that XXX has unbounded variation, or bounded variation and a Lévy measure absolutely continuous with respect to Lebesgue measure.

The Laplace exponent is ψ(θ)=log⁡E[eθX1]\psi(\theta)=\log\mathbb E[e^{\theta X_1}]ψ(θ)=logE[eθX1​], and Φ(q)\Phi(q)Φ(q) is the largest root of ψ(θ)=q\psi(\theta)=qψ(θ)=q. For q≥0q\ge0q≥0 the qqq-scale function W(q):R→[0,∞)W^{(q)}:\mathbb R\to[0,\infty)W(q):R→[0,∞) is the unique function that vanishes on (−∞,0](-\infty,0](−∞,0], is continuous on (0,∞)(0,\infty)(0,∞), and satisfies ∫0∞e−θxW(q)(x) dx=(ψ(θ)−q)−1\int_0^\infty e^{-\theta x}W^{(q)}(x)\,dx=(\psi(\theta)-q)^{-1}∫0∞​e−θxW(q)(x)dx=(ψ(θ)−q)−1 for θ>Φ(q)\theta>\Phi(q)θ>Φ(q). Then Z(q)(x)=1+q∫−∞xW(q)(z) dzZ^{(q)}(x)=1+q\int_{-\infty}^xW^{(q)}(z)\,dzZ(q)(x)=1+q∫−∞x​W(q)(z)dz. The tilted scale functions Wv(p)W_v^{(p)}Wv(p)​ are those of the exponent ψv(θ)=ψ(θ+v)−ψ(v)\psi_v(\theta)=\psi(\theta+v)-\psi(v)ψv​(θ)=ψ(θ+v)−ψ(v).

Fix r≥0r\ge0r≥0 with ψ(1)=r\psi(1)=rψ(1)=r (the risk-neutral condition), and let P1\mathbb P^1P1 be the Esscher measure, dP1/dP∣Ft=eXt−rtd\mathbb P^1/d\mathbb P|_{\mathcal F_t}=e^{X_t-rt}dP1/dP∣Ft​​=eXt​−rt. For z≥0z\ge0z≥0, under P−z1\mathbb P^1_{-z}P−z1​ the process starts at −z-z−z with running maximum X‾t=max⁡{0,sup⁡u≤tXu}\overline X_t=\max\{0,\sup_{u\le t}X_u\}Xt​=max{0,supu≤t​Xu​}, and the reflected process Y=X‾−XY=\overline X-XY=X−X starts at Y0=zY_0=zY0​=z. The passage time is τk=inf⁡{t≥0:Yt∉[0,k)}\tau_k=\inf\{t\ge0:Y_t\notin[0,k)\}τk​=inf{t≥0:Yt​∈/[0,k)}. Fix α>0\alpha>0α>0 and put q=α+rq=\alpha+rq=α+r.

The Russian optimal stopping problem (28) is

wR(z)=sup⁡τ E−z1[e−ατ+Yτ],w^R(z)=\sup_\tau\ \mathbb E^1_{-z}\big[e^{-\alpha\tau+Y_\tau}\big],wR(z)=τsup​ E−z1​[e−ατ+Yτ​],

the supremum over all P1\mathbb P^1P1-almost surely finite F\mathbf FF-stopping times. The option price is Vr(M0,S0)=S0 wR(log⁡(M0/S0))V_r(M_0,S_0)=S_0\,w^R(\log(M_0/S_0))Vr​(M0​,S0​)=S0​wR(log(M0​/S0​)).

Formalization targets

Goal: Theorem 2

With the optimal level (30) and the candidate value

κ∗=inf⁡{x: Z(q)(x)≤qW(q)(x)},u(z)=ezZ(q)(κ∗−z),\kappa^*=\inf\{x:\ Z^{(q)}(x)\le qW^{(q)}(x)\},\qquad u(z)=e^zZ^{(q)}(\kappa^*-z),κ∗=inf{x: Z(q)(x)≤qW(q)(x)},u(z)=ezZ(q)(κ∗−z),

for every z≥0z\ge0z≥0,

wR(z)=u(z)=E−z1[e−ατκ∗+Yτκ∗],w^R(z)=u(z)=\mathbb E^1_{-z}\big[e^{-\alpha\tau_{\kappa^*}+Y_{\tau_{\kappa^*}}}\big],wR(z)=u(z)=E−z1​[e−ατκ∗​+Yτκ∗​​],

and τκ∗\tau_{\kappa^*}τκ∗​ is a P1\mathbb P^1P1-a.s. finite F\mathbf FF-stopping time.

Milestones

  1. Remark 4: W(u)(x)=evxWv(u−ψ(v))(x)W^{(u)}(x)=e^{vx}W_v^{(u-\psi(v))}(x)W(u)(x)=evxWv(u−ψ(v))​(x).
  2. Lemma 1: Z(q)(x)/W(q)(x)→q/Φ(q)Z^{(q)}(x)/W^{(q)}(x)\to q/\Phi(q)Z(q)(x)/W(q)(x)→q/Φ(q) as x→∞x\to\inftyx→∞ (for q≥0q\ge0q≥0, with the paper's convention for 0/Φ(0)0/\Phi(0)0/Φ(0)).
  3. Remark 3: Wv(0+)=0W_v(0+)=0Wv​(0+)=0 if and only if XXX has unbounded variation.
  4. Corollary 1, (29): the value of stopping at τk\tau_kτk​,
E−z1(e−ατk+Yτk)=ez(Z(q)(k−z)+Z(q)(k)−qW(q)(k)W(q)′(k)−W(q)(k)W(q)(k−z)).\mathbb E^1_{-z}\big(e^{-\alpha\tau_k+Y_{\tau_k}}\big)=e^z\Big(Z^{(q)}(k-z)+\frac{Z^{(q)}(k)-qW^{(q)}(k)}{W^{(q)\prime}(k)-W^{(q)}(k)}W^{(q)}(k-z)\Big).E−z1​(e−ατk​+Yτk​​)=ez(Z(q)(k−z)+W(q)′(k)−W(q)(k)Z(q)(k)−qW(q)(k)​W(q)(k−z)).
  1. Lemma 2 (i): for q>rq>rq>r, f=Z(q)−qW(q)f=Z^{(q)}-qW^{(q)}f=Z(q)−qW(q) decreases on [0,∞)[0,\infty)[0,∞) to −∞-\infty−∞.
  2. Lemma 2 (ii): κ∗=0\kappa^*=0κ∗=0 if W(q)(0+)≥q−1W^{(q)}(0+)\ge q^{-1}W(q)(0+)≥q−1; otherwise κ∗>0\kappa^*>0κ∗>0 is the unique root of fff.
  3. The stopped process e−α(t∧τκ∗)u(Yt∧τκ∗)e^{-\alpha(t\wedge\tau_{\kappa^*})}u(Y_{t\wedge\tau_{\kappa^*}})e−α(t∧τκ∗​)u(Yt∧τκ∗​​) is a P1\mathbb P^1P1-martingale.
  4. E−z1[e−αt+YtZ(q)(κ∗−Yt)]≤ezZ(q)(κ∗−z)\mathbb E^1_{-z}[e^{-\alpha t+Y_t}Z^{(q)}(\kappa^*-Y_t)]\le e^zZ^{(q)}(\kappa^*-z)E−z1​[e−αt+Yt​Z(q)(κ∗−Yt​)]≤ezZ(q)(κ∗−z).
  5. e−αtu(Yt)e^{-\alpha t}u(Y_t)e−αtu(Yt​) is a P1\mathbb P^1P1-supermartingale.

Significance

The result. Theorem 2 gives the price of the perpetual Russian option and its optimal exercise rule for every exponential spectrally negative Lévy market. The rule is to exercise when the ratio of the running maximum to the current price first reaches eκ∗e^{\kappa^*}eκ∗. The level is explicit through scale functions, and it separates the regimes: for bounded variation with W(q)(0+)≥q−1W^{(q)}(0+)\ge q^{-1}W(q)(0+)≥q−1, immediate exercise is optimal. The theorem is the model case of a general method: an optimal stopping problem for a functional of (X,X‾)(X,\overline X)(X,X) is reduced, by a change of measure, to one for the reflected process, and solved by verification. The same method underlies the Canadized Russian option (third mission of the series).

Formalizing it. The result is proved in the paper; it has no machine-checked proof. This mission produces a Lean statement of the full verification theorem, including admissibility of τκ∗\tau_{\kappa^*}τκ∗​. It also states the analytic facts about scale functions that the proof relies on (Lemmas 1, 2 and Remarks 3, 4), which apply to any problem phrased in scale functions.

Difficulty

The obvious route is the classical verification: show that e−αtu(Yt)e^{-\alpha t}u(Y_t)e−αtu(Yt​) is a supermartingale, apply optional stopping, and check equality at τκ∗\tau_{\kappa^*}τκ∗​. The first step fails as a direct Itô computation. In the unbounded-variation case uuu is only C1C^1C1 at κ∗\kappa^*κ∗, and in the bounded-variation case only continuous there. The generator of YYY is nonlocal, so smoothness away from κ∗\kappa^*κ∗ does not control the jump part of the process across the boundary. The equality case needs the exact value of stopping at τk\tau_kτk​ (Corollary 1). That value requires the overshoot of YYY over kkk, which is caused by a downward jump of XXX, and the exit problem of the reflected process. Finally, P1\mathbb P^1P1 is not equivalent to P\mathbb PP on F∞\mathcal F_\inftyF∞​, so passing from P\mathbb PP-facts to P1\mathbb P^1P1-facts is valid only on each Ft\mathcal F_tFt​.

Formalization scope

Conventions committed to in Lean:

  • Time is [0,∞)[0,\infty)[0,∞) (ℝ≥0) and values are real. Random times take values in [0,∞][0,\infty][0,∞] (WithTop ℝ≥0), and the payoff is set to 000 on {τ=∞}\{\tau=\infty\}{τ=∞}, a P1\mathbb P^1P1-null event for admissible τ\tauτ.
  • The spectrally negative Lévy process is a structure: measurable marginals, X0=0X_0=0X0​=0, independent increments, stationary increments, càdlàg paths, no positive jumps, not almost surely monotone. Paths start at 000, are càdlàg, and have no positive jumps for every ω\omegaω, not merely almost surely. Adaptedness, independence of increments from the past, and right-continuity of F\mathbf FF are added for the filtered version.
  • "The usual conditions" are read as right-continuity only; completeness is not imposed. P1\mathbb P^1P1 is typically singular to P\mathbb PP on F∞\mathcal F_\inftyF∞​, so a complete F0\mathcal F_0F0​ would contradict (3).
  • "Unbounded variation" means "not almost surely of bounded variation on compacts". Condition (AC) is stated through jumps: no jump lands in a Lebesgue-null set, almost surely. The standing assumption is "bounded variation implies (AC)".
  • ψ\psiψ is Mathlib's cumulant generating function; "ψ(v)<∞\psi(v)<\inftyψ(v)<∞" is integrability of evX1e^{vX_1}evX1​.
  • W(q)W^{(q)}W(q) is a definite description (choice among functions with the properties of Definition 2) for q≥0q\ge0q≥0, and the series (5) for q<0q<0q<0. Z(q)Z^{(q)}Z(q) integrates over (−∞,x](-\infty,x](−∞,x].
  • P1\mathbb P^1P1 is data (a probability measure Q\mathbb QQ) with Q∣Ft=eXt−rt⋅P∣Ft\mathbb Q|_{\mathcal F_t}=e^{X_t-rt}\cdot\mathbb P|_{\mathcal F_t}Q∣Ft​​=eXt​−rt⋅P∣Ft​​ for all ttt. P−z1\mathbb P^1_{-z}P−z1​ is encoded by the reflected process with prior maximum 000 and starting point −z-z−z.
  • The value function is a supremum in [0,∞][0,\infty][0,∞] of lower Lebesgue integrals. Expectation identities (Corollary 1, the display on p. 230) are stated in [0,∞][0,\infty][0,∞] and thereby assert finiteness.
  • W(q)(0+)W^{(q)}(0+)W(q)(0+) is Function.rightLim, and κ∗\kappa^*κ∗ is the real infimum (30); its nonemptiness is Lemma 2, not a hypothesis. τ0=0\tau_0=0τ0​=0 extends the paper's τk\tau_kτk​, k>0k>0k>0.
  • Readings of informal words: "decreases monotonically" is strict decrease on [0,∞)[0,\infty)[0,∞); "the unique root" is on [0,∞)[0,\infty)[0,∞); Lemma 1 is formalized for q≥0q\ge0q≥0, with 0/Φ(0)0/\Phi(0)0/Φ(0) read as lim⁡θ↓0θ/Φ(θ)\lim_{\theta\downarrow0}\theta/\Phi(\theta)limθ↓0​θ/Φ(θ) as the paper stipulates; Remarks 3 and 4 for real qqq, uuu only. The p. 230 martingale, bound and supermartingale claims are stated under the standing assumption, covering all three cases of the proof.

A trivializing formalization is ruled out: the supremum ranges over every P1\mathbb P^1P1-a.s. finite stopping time of the given filtration (not only passage times, not a smaller filtration), and it is taken in [0,∞][0,\infty][0,∞], where no junk value of an unbounded real supremum can occur.

Infrastructure a complete development needs: Lévy processes on path space, their Laplace exponents and Esscher transforms, scale functions (existence, uniqueness, smoothness under the standing assumption), the reflected process and the exit identity of Theorem 1, optional stopping for continuous-time supermartingales, and Itô/change-of-variables formulas for semimartingales with jumps. The scale-function and Esscher layers are reusable for the other missions of this series and for any fluctuation-theory problem. Contributions to any of these layers, or to the milestones separately, are welcome.

Selected references

  • F. Avram, A. E. Kyprianou, M. R. Pistorius, Exit problems for spectrally negative Lévy processes and applications to (Canadized) Russian options, Ann. Appl. Probab. 14(1), 215–238, 2004. https://doi.org/10.1214/aoap/1075828052
  • L. Shepp, A. N. Shiryaev, The Russian option: reduced regret, Ann. Appl. Probab. 3(3), 631–640, 1993. https://doi.org/10.1214/aoap/1177005715
  • J. Bertoin, Lévy Processes, Cambridge Tracts in Mathematics 121, Cambridge University Press, 1996. ISBN 0-521-56243-0
  • A. E. Kyprianou, Fluctuations of Lévy Processes with Applications, 2nd ed., Springer, 2014. https://doi.org/10.1007/978-3-642-37632-0
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Dynamical SystemsProbabilityReinforcement Learning·Captain: mikedeng1

The O.D.E. Method for Convergence of Stochastic Approximation and Reinforcement Learning II: Mean-Square Error under Bounded StepsizesResearch Paper

Motivation

Stochastic approximation is the family of recursive algorithms that locate a zero of a vector field hhh from noisy evaluations of it. Temporal-difference learning, Q-learning, actor–critic methods and stochastic gradient descent are all instances. In practice these algorithms are often run with a constant or bounded, non-vanishing stepsize: the iterate keeps adapting to new data and never freezes, at the price of never converging exactly. The natural question for such a scheme is quantitative: how far from the target does the iterate stay in the long run, and how does that distance scale with the stepsize?

Borkar and Meyn (SIAM J. Control Optim. 38(2), 2000) answer both halves of the question under one set of hypotheses. First, stability of a "fluid" ODE obtained by scaling hhh at infinity implies that the iterates have bounded second moments, with no a priori boundedness or projection assumption. Second, if the ODE x˙=h(x)\dot x = h(x)x˙=h(x) has a globally exponentially stable equilibrium x∗x^*x∗, the asymptotic mean-square error is of the order of the largest stepsize. The first result replaced the usual stochastic-Lyapunov-function verification in reinforcement-learning applications (Section 3 of the paper). This mission formalizes the bounded-stepsize branch of the paper. A companion mission (… I: Stability and Almost-Sure Convergence under Tapering Stepsizes) covers the vanishing-stepsize branch.

Setting

Fix d≥1d \ge 1d≥1 and a Lipschitz vector field h:Rd→Rdh : \mathbb{R}^d \to \mathbb{R}^dh:Rd→Rd. The stochastic approximation recursion (1.1) is

X(n+1)=X(n)+a(n)[h(X(n))+M(n+1)],n≥0,X(n+1) = X(n) + a(n)\big[h(X(n)) + M(n+1)\big], \qquad n \ge 0,X(n+1)=X(n)+a(n)[h(X(n))+M(n+1)],n≥0,

with a deterministic step sequence {a(n)}\{a(n)\}{a(n)} and a noise sequence {M(n)}\{M(n)\}{M(n)} on a probability space (Ω,F,P)(\Omega, \mathcal F, \mathsf P)(Ω,F,P). The associated ODE (1.2) is x˙=h(x)\dot x = h(x)x˙=h(x).

  • The scaled fields are hr(x)=r−1h(rx)h_r(x) = r^{-1} h(rx)hr​(x)=r−1h(rx). Assumption (A1) asks that hhh be Lipschitz, that hr(x)→h∞(x)h_r(x) \to h_\infty(x)hr​(x)→h∞​(x) for every xxx as r→∞r \to \inftyr→∞, and that the origin be an asymptotically stable equilibrium of the fluid ODE x˙=h∞(x)\dot x = h_\infty(x)x˙=h∞​(x).
  • Let Fn=σ(X(0),…,X(n))\mathcal F_n = \sigma(X(0), \dots, X(n))Fn​=σ(X(0),…,X(n)). Assumption (A2) asks that {M(n)}\{M(n)\}{M(n)} be a martingale difference sequence, E[M(n+1)∣Fn]=0\mathsf E[M(n+1) \mid \mathcal F_n] = 0E[M(n+1)∣Fn​]=0, with conditional second moments E[∥M(n+1)∥2∣Fn]≤C0(1+∥X(n)∥2)\mathsf E[\|M(n+1)\|^2 \mid \mathcal F_n] \le C_0(1 + \|X(n)\|^2)E[∥M(n+1)∥2∣Fn​]≤C0​(1+∥X(n)∥2) for a constant C0C_0C0​.
  • Assumption (BS), bounded stepsizes: 0<α‾≤a(n)≤αˉ<10 < \underline\alpha \le a(n) \le \bar\alpha < 10<α​≤a(n)≤αˉ<1 for all nnn, with α‾<αˉ\underline\alpha < \bar\alphaα​<αˉ.
  • The error (2.2) is e(n)=∥X(n)−x∗∥e(n) = \|X(n) - x^*\|e(n)=∥X(n)−x∗∥.

An equilibrium x∗x^*x∗ of (1.2) is globally asymptotically stable if it is Lyapunov stable and attracts every solution. It is globally exponentially asymptotically stable if there are bbb and δ>0\delta > 0δ>0 with ∥x(t)−x∗∥≤b e−δt∥x(0)−x∗∥\|x(t) - x^*\| \le b\,e^{-\delta t}\|x(0) - x^*\|∥x(t)−x∗∥≤be−δt∥x(0)−x∗∥ for every solution.

The proofs compare the iterates with ODE solutions on a time grid: t(n)=∑i<na(i)t(n) = \sum_{i<n} a(i)t(n)=∑i<n​a(i), blocks T(j)=t(m(j))T(j) = t(m(j))T(j)=t(m(j)) of length about TTT, the interpolated path ψ\psiψ of the iterates, its rescaled version ϕj=ψ/r(j)\phi_j = \psi/r(j)ϕj​=ψ/r(j) with r(j)=max⁡(1,∥X(m(j))∥)r(j) = \max(1, \|X(m(j))\|)r(j)=max(1,∥X(m(j))∥), and the ODE solutions ψ^\hat\psiψ^​, ϕ^j\hat\phi_jϕ^​j​ restarted at each block.

Formalization targets

Goal: Theorem 2.3(ii)

Under (A1), (A2) and (BS), if x∗x^*x∗ is a globally asymptotically and globally exponentially asymptotically stable equilibrium of (1.2), there are α∗>0\alpha^* > 0α∗>0 and b2<∞b_2 < \inftyb2​<∞ such that for all 0<αˉ≤α∗0 < \bar\alpha \le \alpha^*0<αˉ≤α∗ and every initial condition X(0)X(0)X(0),

lim sup⁡n→∞E[e(n)2]≤b2 αˉ.\limsup_{n \to \infty} \mathsf E\big[e(n)^2\big] \le b_2\, \bar\alpha .n→∞limsup​E[e(n)2]≤b2​αˉ.

The constant b2b_2b2​ is uniform in the stepsizes and in X(0)X(0)X(0). No rate constant is fixed: only the linear dependence on αˉ\bar\alphaαˉ is asserted.

Milestones

  1. Lemma 4.7. For fixed T>0T > 0T>0 there is C2C_2C2​, independent of the stepsizes, with E[∥ϕj(t)−ϕ^j(t)∥2∣Fm(j)]≤C2αˉ\mathsf E[\|\phi_j(t) - \hat\phi_j(t)\|^2 \mid \mathcal F_{m(j)}] \le C_2\bar\alphaE[∥ϕj​(t)−ϕ^​j​(t)∥2∣Fm(j)​]≤C2​αˉ and E[∥ϕj(t)∥2∣Fm(j)]≤C2\mathsf E[\|\phi_j(t)\|^2 \mid \mathcal F_{m(j)}] \le C_2E[∥ϕj​(t)∥2∣Fm(j)​]≤C2​ on every block.
  2. Theorem 2.1(ii). There are α∗>0\alpha^* > 0α∗>0 and C1C_1C1​ with lim sup⁡nE∥X(n)∥2≤C1\limsup_n \mathsf E\|X(n)\|^2 \le C_1limsupn​E∥X(n)∥2≤C1​ whenever αˉ<α∗\bar\alpha < \alpha^*αˉ<α∗.
  3. Lemma 4.8. For αˉ≤α∗\bar\alpha \le \alpha^*αˉ≤α∗, sup⁡t≥0E∥ψ^(t)−ψ(t)∥2≤C3αˉ\sup_{t \ge 0} \mathsf E\|\hat\psi(t) - \psi(t)\|^2 \le C_3 \bar\alphasupt≥0​E∥ψ^​(t)−ψ(t)∥2≤C3​αˉ.

Significance

The result. Theorem 2.1(ii) says that a stability property of a deterministic ODE at infinity controls a stochastic recursion in mean square, uniformly over initial conditions. Theorem 2.3(ii) turns this into an error bound: with a non-vanishing stepsize the iterate does not converge, but its mean-square distance from x∗x^*x∗ is eventually O(αˉ)O(\bar\alpha)O(αˉ). This is the quantitative justification for constant-stepsize stochastic approximation in reinforcement learning and adaptive control, and it is the starting point of the trade-off between bias (small stepsize) and speed (large stepsize) discussed in Section 2.2 of the paper.

Formalizing it. The results are proved in the paper, partly by sketch: Lemma 4.8's proof refers to "familiar arguments using the Bellman–Gronwall lemma", and the paper writes several bounds as O(αˉ)O(\bar\alpha)O(αˉ). A formal proof makes every constant and its dependence explicit, which the paper's quantifier order leaves partly implicit (see the scope section). No machine-checked proof of these results, or of any stochastic-approximation stability theorem in this generality, is known to exist.

Difficulty

The natural first argument, that the iterates track the ODE and the ODE converges, needs the iterates to be bounded. Bounded iterates are exactly what is being proved, so the argument is circular. The paper breaks the circularity by rescaling: on each block the iterate is divided by r(j)r(j)r(j), so that on large scales it tracks the fluid ODE, whose stability contracts the norm by a fixed factor per block. Making this work in mean square requires conditional second-moment estimates that are uniform in the stepsize and the scale (Lemma 4.7). A second difficulty is that the stepsize does not vanish: the tracking error per block does not go to zero, and the goal's content is precisely that it is of order αˉ\bar\alphaαˉ with a constant that does not depend on αˉ\bar\alphaαˉ.

Formalization scope

  • The state space is EuclideanSpace ℝ (Fin d). ODE solutions are forward solutions: continuous on [0,∞)[0,\infty)[0,∞) with right derivatives. Stability notions are the standard ones, with exponential stability in the form the proof of Theorem 2.3(ii) uses.
  • The filtration is the natural filtration of the iterates. (A2) includes integrability of M(n+1)M(n+1)M(n+1) and ∥M(n+1)∥2\|M(n+1)\|^2∥M(n+1)∥2 so that the conditional expectations are meaningful. Each theorem quantifies over every probability space, every measurable process satisfying (1.1) and (A2), and every deterministic X(0)X(0)X(0).
  • Second moments, suprema and lim sup⁡\limsuplimsup are computed in [0,∞][0,\infty][0,∞], so a bound is a genuine finiteness claim.
  • Constant placement. α∗\alpha^*α∗, C1C_1C1​ and b2b_2b2​ depend only on hhh, h∞h_\inftyh∞​, C0C_0C0​ (and x∗x^*x∗). C2C_2C2​ depends in addition on TTT, and C3C_3C3​ on TTT and X(0)X(0)X(0). None depends on the stepsizes. Theorem 2.3's page text puts b2b_2b2​ after α\alphaα. Read literally, that would allow b2=C1/αˉb_2 = C_1/\bar\alphab2​=C1​/αˉ and make the goal a restatement of Theorem 2.1(ii). The formal goal fixes b2b_2b2​ before the stepsizes and the initial condition, as the proof (16C3αˉ16C_3\bar\alpha16C3​αˉ) gives. α∗\alpha^*α∗ is existential in Theorem 2.3(ii) and Lemma 4.8 rather than tied to Theorem 2.1(ii)'s witness.
  • The proof objects ψ^\hat\psiψ^​, ϕ^j\hat\phi_jϕ^​j​ are characterized by predicates (initial value, continuity, ODE on the block). Lemmas 4.7 and 4.8 hold for every function satisfying them.
  • Not included: Theorem 2.3(i) (its proof chooses a radius depending on αˉ\bar\alphaαˉ), Theorem 2.4 and the Markov-chain results of Section 4.3, and the asynchronous extension (Theorem 2.5). The deterministic ODE lemmas 4.1–4.4 belong to the companion mission.

Useful infrastructure, reusable beyond this mission: Bellman–Gronwall inequalities in discrete time (Lemma 4.3 of the paper), stability of scaled ODEs, and conditional second-moment estimates for martingale-difference-driven recursions. Contributions of any of these as separate lemmas are welcome.

Selected references

  • V. S. Borkar and S. P. Meyn, The O.D.E. Method for Convergence of Stochastic Approximation and Reinforcement Learning, SIAM J. Control Optim. 38(2):447–469, 2000. https://doi.org/10.1137/S0363012997331639
  • M. Benaïm, Dynamics of stochastic approximation algorithms, Séminaire de Probabilités XXXIII, Lecture Notes in Math. 1709, Springer, 1999. https://doi.org/10.1007/BFb0096509
  • H. J. Kushner and G. G. Yin, Stochastic Approximation and Recursive Algorithms and Applications, 2nd ed., Springer, 2003. https://doi.org/10.1007/b97441
7 thms1 active userReviewed
Dynamic ProgrammingOperations ResearchProbability·Captain: mikedeng1

On the Optimal Dividend Problem for a Spectrally Negative Lévy Process II: Optimality of the Double-Barrier Strategy at d* with Bail-Out LoansResearch Paper

Dividends, ruin and bail-out loans

An insurance company's surplus in the Cramér–Lundberg model grows linearly with premiums and falls by claims arriving as a compound Poisson process. When premium income exceeds the expected claims, the surplus drifts to infinity. De Finetti (1957) proposed that the surplus above a barrier should instead be paid to shareholders as dividends, and the resulting optimal dividend problem — maximize the expected discounted dividends — is a central problem of risk theory. A barrier policy, however, drives the surplus below zero with probability one. Harrison and Taylor (1978) and Løkka and Zervos studied, for Brownian motion, a variant with bail-out loans: ruin is forbidden, and the shareholders must inject capital whenever the surplus would become negative, at a cost φ>1\varphi>1φ>1 per unit.

Avram, Palmowski and Pistorius (Ann. Appl. Probab. 17 (2007)) solved the bail-out problem when the surplus is a general spectrally negative Lévy process, which includes the Cramér–Lundberg model, Brownian motion with drift and their sums. They showed that the optimal policy is a double barrier policy for every initial capital. This mission formalizes that result, Theorem 3 of the paper.

Timeline:

  • 1957 — de Finetti introduces dividend barriers.
  • 1978 — Harrison and Taylor: optimal control of a Brownian storage system with two reflecting barriers.
  • 1995 — Jeanblanc and Shiryaev: optimal dividends for Brownian motion with drift.
  • 2004 — Avram, Kyprianou and Pistorius: exit problems for spectrally negative Lévy processes reflected at their infimum and supremum, in terms of scale functions.
  • 2007 — Avram, Palmowski and Pistorius: Theorems 1 and 3 of the present paper; Pistorius' pathwise construction of the doubly reflected process is used.

Setting

A spectrally negative Lévy process X={Xt}t≥0X=\{X_t\}_{t\ge0}X={Xt​}t≥0​ on a filtered probability space (Ω,F,F,P)(\Omega,\mathcal F,\mathbb F,P)(Ω,F,F,P) starts at X0=0X_0=0X0​=0, has càdlàg paths, is F\mathbb FF-adapted, and has stationary increments with Xt−XsX_t-X_sXt​−Xs​ independent of Fs\mathcal F_sFs​. Its jumps are all negative, and E[eθXt]=etψ(θ)E[e^{\theta X_t}]=e^{t\psi(\theta)}E[eθXt​]=etψ(θ) for θ≥0\theta\ge0θ≥0, where the Laplace exponent is

ψ(θ)=cθ+σ22θ2+∫(−∞,0)(eθy−1−θy1{∣y∣<1}) ν(dy).\psi(\theta)=c\theta+\tfrac{\sigma^2}{2}\theta^2+\int_{(-\infty,0)}(e^{\theta y}-1-\theta y\mathbf 1_{\{|y|<1\}})\,\nu(dy).ψ(θ)=cθ+2σ2​θ2+∫(−∞,0)​(eθy−1−θy1{∣y∣<1}​)ν(dy).

With initial capital x≥0x\ge0x≥0 the surplus is x+Xx+Xx+X. The standing assumptions are: XXX does not have monotone paths; E[X1]>−∞E[X_1]>-\inftyE[X1​]>−∞ (so ψ′(0+)=E[X1]\psi'(0+)=E[X_1]ψ′(0+)=E[X1​] is finite); σ>0\sigma>0σ>0, or ∫(−1,0)∣y∣ν(dy)=∞\int_{(-1,0)}|y|\nu(dy)=\infty∫(−1,0)​∣y∣ν(dy)=∞, or ν\nuν has a density (condition (3.3)).

A policy πˉ=(L,R)\bar\pi=(L,R)πˉ=(L,R) consists of nondecreasing adapted processes with L0=R0=0L_0=R_0=0L0​=R0​=0: cumulative dividends LLL (left-continuous) and cumulative injected capital RRR (right-continuous). The controlled surplus is Vt=x+Xt−Lt+RtV_t=x+X_t-L_t+R_tVt​=x+Xt​−Lt​+Rt​. The policy is admissible if Vt≥0V_t\ge0Vt​≥0 for t>0t>0t>0 and ∫0∞e−qtdRt<∞\int_0^\infty e^{-qt}dR_t<\infty∫0∞​e−qtdRt​<∞ almost surely. Its value and the value function are

vˉπˉ(x)=E[∫0∞e−qtdLt−φ∫0∞e−qtdRt],vˉ∗(x)=sup⁡πˉ admissiblevˉπˉ(x),\bar v_{\bar\pi}(x)=E\Bigl[\int_0^\infty e^{-qt}dL_t-\varphi\int_0^\infty e^{-qt}dR_t\Bigr],\qquad \bar v_*(x)=\sup_{\bar\pi\ \text{admissible}}\bar v_{\bar\pi}(x),vˉπˉ​(x)=E[∫0∞​e−qtdLt​−φ∫0∞​e−qtdRt​],vˉ∗​(x)=πˉ admissiblesup​vˉπˉ​(x),

with discount rate q>0q>0q>0 and cost φ>1\varphi>1φ>1. The double-barrier strategy πˉ0,a\bar\pi_{0,a}πˉ0,a​ pays out (x−a)+(x-a)^+(x−a)+ at once and then the minimal dividends and injections that keep VVV in [0,a][0,a][0,a]: dLdLdL is carried by {V=a}\{V=a\}{V=a} and dRdRdR by {V=0}\{V=0\}{V=0}.

The qqq-scale function W=W(q)W=W^{(q)}W=W(q) vanishes on (−∞,0)(-\infty,0)(−∞,0), is continuous and nondecreasing on [0,∞)[0,\infty)[0,∞), and satisfies ∫0∞e−θyW(y)dy=1/(ψ(θ)−q)\int_0^\infty e^{-\theta y}W(y)dy=1/(\psi(\theta)-q)∫0∞​e−θyW(y)dy=1/(ψ(θ)−q) for θ>Φ(q)\theta>\Phi(q)θ>Φ(q), the largest root of ψ=q\psi=qψ=q. Set W‾(y)=∫0yW\overline W(y)=\int_0^yWW(y)=∫0y​W, Z=1+qW‾Z=1+q\overline WZ=1+qW, Z‾(y)=∫0yZ\overline Z(y)=\int_0^yZZ(y)=∫0y​Z. The candidate value of πˉ0,a\bar\pi_{0,a}πˉ0,a​ is

vˉa(x)=φ(Z‾(x)+ψ′(0+)/q)+Z(x)1−φZ(a)qW(a)(0≤x≤a),vˉa(x)=x−a+vˉa(a)(x>a),\bar v_a(x)=\varphi\bigl(\overline Z(x)+\psi'(0+)/q\bigr)+Z(x)\frac{1-\varphi Z(a)}{qW(a)}\quad(0\le x\le a),\qquad \bar v_a(x)=x-a+\bar v_a(a)\quad(x>a),vˉa​(x)=φ(Z(x)+ψ′(0+)/q)+Z(x)qW(a)1−φZ(a)​(0≤x≤a),vˉa​(x)=x−a+vˉa​(a)(x>a),

and the barrier level is d∗=inf⁡{a>0:[φZ(a)−1]W′(a)−φqW(a)2≤0}d^*=\inf\{a>0:[\varphi Z(a)-1]W'(a)-\varphi qW(a)^2\le0\}d∗=inf{a>0:[φZ(a)−1]W′(a)−φqW(a)2≤0}, with inf⁡∅=∞\inf\emptyset=\inftyinf∅=∞.

Formalization targets

Goal: Theorem 3

d∗<∞,vˉ∗(x)=vˉd∗(x)  (x≥0),πˉ0,d∗ exists, is admissible and attains vˉ∗(x).d^*<\infty,\qquad \bar v_*(x)=\bar v_{d^*}(x)\ \ (x\ge0),\qquad \bar\pi_{0,d^*}\ \text{exists, is admissible and attains }\bar v_*(x).d∗<∞,vˉ∗​(x)=vˉd∗​(x)  (x≥0),πˉ0,d∗​ exists, is admissible and attains vˉ∗​(x).

Milestones

  • Lemma 1: W‾(y)/W‾(a)≤W(y)/W(a)\overline W(y)/\overline W(a)\le W(y)/W(a)W(y)/W(a)≤W(y)/W(a) for 0≤y≤a0\le y\le a0≤y≤a.
  • Proposition 2, (3.17): the expected discounted undershoot Ex[e−qT0−XT0−]E_x[e^{-qT_0^-}X_{T_0^-}]Ex​[e−qT0−​XT0−​​] in closed form.
  • Theorem 1: the expected discounted dividends and injections of πˉ0,a\bar\pi_{0,a}πˉ0,a​, a>0a>0a>0, in closed form; hence vˉπˉ0,a=vˉa\bar v_{\bar\pi_{0,a}}=\bar v_avˉπˉ0,a​​=vˉa​.
  • Lemma 2(ii): d∗=0d^*=0d∗=0 if and only if σ=0\sigma=0σ=0 and ν(−∞,0)≤q/(φ−1)\nu(-\infty,0)\le q/(\varphi-1)ν(−∞,0)≤q/(φ−1).
  • Proposition 3(ii): d∗<∞d^*<\inftyd∗<∞ and vˉa≤vˉd∗\bar v_a\le\bar v_{d^*}vˉa​≤vˉd∗​ for all levels aaa.
  • Lemma 3(ii)–(iv): 1≤vˉd∗′≤φ1\le\bar v_{d^*}'\le\varphi1≤vˉd∗′​≤φ with boundary slopes; a↦vˉa(x)a\mapsto\bar v_a(x)a↦vˉa​(x) nonincreasing for a>d∗a>d^*a>d∗; vˉd∗\bar v_{d^*}vˉd∗​ concave.
  • Lemma 5: (Γvˉd∗−qvˉd∗)≤0(\Gamma\bar v_{d^*}-q\bar v_{d^*})\le0(Γvˉd∗​−qvˉd∗​)≤0 on (0,∞)(0,\infty)(0,∞), with equality on (0,d∗)(0,d^*)(0,d∗).
  • Proposition 4(ii): any C2C^2C2 solution of the variational inequality (5.9) dominates vˉ∗\bar v_*vˉ∗​.

Significance

Theorem 3 answers the bail-out problem completely: for every initial capital and every spectrally negative Lévy surplus, the optimal policy is a double barrier with an explicit level and an explicit value in terms of scale functions. In the classical problem without injections (Theorem 2 of the same paper) the analogous conclusion needs an extra generator condition, and Azcue and Muler exhibited Cramér–Lundberg models where barrier policies are not optimal. The result is the basis of later work on dividends with capital injection, transaction costs and Parisian ruin.

The result has a published proof. What this mission adds is a machine-checked version. As far as is known, no part of the theory used — Lévy processes, scale functions, doubly reflected processes, the generator of a Lévy process, singular stochastic control — has been formalized in Lean's Mathlib.

Difficulty

The value function is a supremum over all adapted singular controls. Its upper bound requires a verification argument: Itô's formula for e−qtw(Vt)e^{-qt}w(V_t)e−qtw(Vt​) with a semimartingale VVV that has jumps, a controlled bounded-variation part and a possibly nonzero continuous martingale part, followed by localization and limits. A function that satisfies the variational inequality only in the viscosity sense is not enough, so the candidate vˉd∗\bar v_{d^*}vˉd∗​ must be shown to be regular enough and to satisfy Γvˉd∗−qvˉd∗≤0\Gamma\bar v_{d^*}-q\bar v_{d^*}\le0Γvˉd∗​−qvˉd∗​≤0 everywhere on (0,∞)(0,\infty)(0,∞). Above the barrier this inequality does not follow from a martingale property: the paper derives it from concavity and a comparison with higher barriers, through the resolvent of the doubly reflected process. The lower bound requires the existence and value of the doubly reflected process, and computing that value needs fluctuation identities (two-sided exit, overshoot) that are themselves theorems about scale functions.

Formalization scope

Time is indexed by R≥0\mathbb R_{\ge0}R≥0​. The process is a structure carrying the triplet (c,σ,ν)(c,\sigma,\nu)(c,σ,ν), the paths, adaptedness, independence of future increments from Fs\mathcal F_sFs​, stationarity, the Laplace-exponent identity, and the usual conditions on the filtration. PxP_xPx​ is the law of x+Xx+Xx+X. Policy values are computed as E[∫e−qtdL]−φE[∫e−qtdR]E[\int e^{-qt}dL]-\varphi E[\int e^{-qt}dR]E[∫e−qtdL]−φE[∫e−qtdR] in the extended reals from two [0,∞][0,\infty][0,∞]-valued expectations, and the value function is a supremum in the extended reals; a policy with both expectations infinite gets −∞-\infty−∞. Stieltjes integrals include the jump at time 000. The scale function is a hypothesis IsScaleFunction (it is unique), and d∗d^*d∗ lives in [0,∞][0,\infty][0,∞], so an empty defining set gives ∞\infty∞. The double-barrier strategy is characterized by the two-sided Skorokhod conditions plus mutual singularity of dLdLdL and dRdRdR, which pins the level-000 policy of bounded-variation processes. These conditions hold almost surely, and they are stated on the post-decision surplus Vt+=x+Xt−Lt++RtV_{t+}=x+X_t-L_{t+}+R_tVt+​=x+Xt​−Lt+​+Rt​: dLdLdL is carried by {Vt+=a}\{V_{t+}=a\}{Vt+​=a} and dRdRdR by {Vt+=0}\{V_{t+}=0\}{Vt+​=0}. This is the paper's "minimal amount" (p. 4) and matches its construction on pp. 10–11. The closure-of-support wording of (4.2) on its own would also admit non-minimal lump dividends. Admissibility, Vt≥0V_t\ge0Vt​≥0 for t>0t>0t>0 together with (2.3), is likewise required almost surely.

Printed slips corrected (milestone texts are verbatim):

  • Theorem 3 and Proposition 3(ii) print "ψ′(0+)<∞\psi'(0+)<\inftyψ′(0+)<∞", which always holds; the intended ψ′(0+)>−∞\psi'(0+)>-\inftyψ′(0+)>−∞ is used.
  • (3.3) prints ∫−10x ν(dx)=∞\int_{-1}^0x\,\nu(dx)=\infty∫−10​xν(dx)=∞ for ∫(−1,0)∣x∣ ν(dx)=∞\int_{(-1,0)}|x|\,\nu(dx)=\infty∫(−1,0)​∣x∣ν(dx)=∞.
  • (3.4) prints e−θxe^{-\theta x}e−θx in a dydydy-integral.
  • p. 20 prints the extension vˉd∗(x)+φx\bar v_{d^*}(x)+\varphi xvˉd∗​(x)+φx for vˉd∗(0)+φx\bar v_{d^*}(0)+\varphi xvˉd∗​(0)+φx.
  • Lemma 3(iv) is printed for every a>0a>0a>0 but proved and used only for a=d∗a=d^*a=d∗, and is stated for a=d∗a=d^*a=d∗.
  • Proposition 3(ii) at a=0a=0a=0 is stated only for bounded variation, where vˉ0\bar v_0vˉ0​ is defined.

The goal cannot be satisfied trivially. It asserts equality of the value function with vˉd∗\bar v_{d^*}vˉd∗​, not only an inequality. Existence of the optimal policy is part of the conclusion. Generator statements carry integrability of the jump integrand, so a non-integrable integrand cannot make them true with the junk value 000.

A complete development needs Lévy processes and their Laplace exponents, scale functions, first-passage and two-sided exit identities, reflected and doubly reflected processes, Itô's formula for semimartingales with jumps, and a verification theorem for singular control. All of these are reusable well beyond this mission. Contributions of any of these foundations are welcome, as are proofs of the analytic milestones (Lemma 3, Proposition 3(ii)) from the scale-function properties.

Selected references

  • F. Avram, Z. Palmowski, M. R. Pistorius, On the optimal dividend problem for a spectrally negative Lévy process, Ann. Appl. Probab. 17 (2007) 156–180. https://arxiv.org/abs/math/0702893
  • F. Avram, A. E. Kyprianou, M. R. Pistorius, Exit problems for spectrally negative Lévy processes and applications to (Canadized) Russian options, Ann. Appl. Probab. 14 (2004) 215–238. https://doi.org/10.1214/aoap/1075828052
  • M. R. Pistorius, On doubly reflected completely asymmetric Lévy processes, Stochastic Process. Appl. 107 (2003) 131–143. https://doi.org/10.1016/S0304-4149(03)00065-9
  • J. M. Harrison, A. J. Taylor, Optimal control of a Brownian storage system, Stochastic Process. Appl. 6 (1978) 179–194. https://doi.org/10.1016/0304-4149(78)90059-5
  • A. E. Kyprianou, Introductory Lectures on Fluctuations of Lévy Processes with Applications, Springer, 2006. https://doi.org/10.1007/978-3-540-31343-4
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Operations ResearchProbability·Captain: Shuze Chen

Processing Networks IV: Fluid Equations for Non-Idling, Priority and FCFS ControlTextbook

Motivation

Mission III's Theorem 6.2 — "fluid limit stability implies SPN stability" — converts a probabilistic stability question into a real-analysis question, but it only supplies the generic fluid equations (6.1)-(6.6), which hold under any control policy and therefore say nothing policy-specific: (6.1)-(6.6) alone never force a fluid path to reach zero. To actually prove a concrete queueing network stable, one must first identify the extra fluid equation a specific policy forces on every fluid limit path, and prove that this extra equation genuinely holds — a task the book calls "justifying" the equation "through the same fluid limit procedure used in the proof of Theorem 6.5." J. G. Dai and J. Michael Harrison's Processing Networks: Fluid Models and Stability (Cambridge University Press, forthcoming; cited here from the authors' pre-publication draft, 2020-4-2, http://spnbook.org) carries out this derivation for four control-policy families in Chapter 7, laying the groundwork every later stability chapter of the book (feedforward networks, the Rybko–Stolyar boundary, back-pressure, proportional fairness, task allocation) builds on.

The first-come-first-served (FCFS) analysis traces to Rybko and Stolyar's 1992 fluid-scaling argument and was first stated in closed form as Eq. (2.6) of M. Bramson's 1996 paper on FCFS queueing networks; Bramson also showed by example (1994) that FCFS networks can be unstable even under the standard load condition, motivating the need for a precise fluid-equation characterization rather than an informal one.

Setting

A queueing network (Section 2.6) is an SPN with one activity per buffer: buffer/class iii is served by a unique pool p(i)p(i)p(i), and on completion a class-iii job becomes class jjj with probability PijP_{ij}Pij​ (the routing matrix). I(k)I(k)I(k) denotes the set of classes served by pool kkk. The fluid equations (6.1)-(6.6) specialize accordingly: consumption is the identity (D^=F^\hat D = \hat FD^=F^) and the output matrix is Γij=Pji\Gamma_{ij} = P_{ji}Γij​=Pji​.

Three control-policy families are studied. A policy is non-idling if no server sits idle while a job waits in one of its buffers. A static buffer priority (SBP) policy is non-idling and additionally orders same-pool classes by a fixed priority permutation σ\sigmaσ, always serving the highest-priority non-empty class first; it is non-preemptive if a job's service, once begun, is never interrupted by a later higher-priority arrival. Under FCFS, jobs at a pool are served strictly in arrival order — the workload-based analysis of Section 7.3. Section 7.4 studies a fourth, more general family: a unitary network (one service type per class) under a relaxed control policy β=h(z^)\beta = h(\hat z)β=h(z^), where z^\hat zz^ is the updated job-count vector and hhh is any capacity-respecting, degree-zero-homogeneous function (Assumption 7.6) — a family general enough to include non-idling and SBP policies as special cases, and to anticipate the proportionally fair allocation studied in Chapters 9-10.

Formalization targets

Goal: Theorem 7.5 — the FCFS fluid equation

For a queueing network under FCFS control, every fluid limit path (D^,F^,T^,Z^)(\hat D, \hat F, \hat T, \hat Z)(D^,F^,T^,Z^) satisfies (6.1)-(6.6) and

D^i(t+W^k(t))=G^i(t),t≥0, i∈I(k), k∈K,\hat D_i\big(t + \hat W_k(t)\big) = \hat G_i(t), \qquad t \ge 0,\ i \in I(k),\ k \in K,D^i​(t+W^k​(t))=G^i​(t),t≥0, i∈I(k), k∈K,

where G^i(t)=λit+∑jPjiD^j(t)\hat G_i(t) = \lambda_i t + \sum_j P_{ji}\hat D_j(t)G^i​(t)=λi​t+∑j​Pji​D^j​(t) is the fluid arrival rate into class iii and W^k(t)=∑i∈I(k)miZ^i(t)\hat W_k(t) = \sum_{i \in I(k)} m_i \hat Z_i(t)W^k​(t)=∑i∈I(k)​mi​Z^i​(t) is pool kkk's fluid-scaled immediate workload. This is the weakest natural target: an identity that pins down exactly the time-shift FCFS imposes, without asserting anything about how quickly or whether the fluid model reaches zero (that is left to the Lyapunov arguments of later chapters, once this equation is in hand).

Supporting milestones

Theorem 7.2 (non-idling): ∑i∈I(k)Z^i(t)>0\sum_{i\in I(k)} \hat Z_i(t) > 0∑i∈I(k)​Z^i​(t)>0 forces pool kkk's aggregate service rate to run at full capacity bkb_kbk​. Theorem 7.3 (non-preemptive SBP): the same conclusion with I(k)I(k)I(k) sharpened to the priority set H(j)H(j)H(j) (Eq. 7.5), for every buffer jjj. Theorem 7.8 (general relaxed control): under Assumption 7.6, Z^i(t)>0\hat Z_i(t) > 0Z^i​(t)>0 forces T^i\hat T_iT^i​'s derivative to equal hi(Z^(t))h_i(\hat Z(t))hi​(Z^(t)) exactly — the common generalization from which the non-idling and SBP fluid equations both follow as special cases of a suitable hhh.

Significance

The result itself. Theorem 7.5 is the precise bridge that lets FCFS-specific stability questions be attacked by the Lyapunov-function method Theorem 6.2 licenses: without a closed-form fluid equation, "does an FCFS network satisfy the standard load condition stably?" has no tractable deterministic reformulation. Bramson's 1994 example (an FCFS network unstable despite satisfying the standard load condition) shows the equation's content is not vacuous — FCFS fluid limits genuinely can misbehave, and this equation is precisely what any subsequent stability or instability argument for FCFS networks must reason about.

Formalizing it. No result about FCFS, non-idling, static-buffer-priority, or general relaxed control policies exists on Prove2Me (q=first-come-first-served, q=FCFS, q=priority policy all return zero hits, consistent with triage.json's record that none of this book's Chapters 6-14 machinery is on the platform). This mission is a from-scratch formalization of queueing networks, their three named control-policy families, and the four policy-specific fluid equations Chapter 7 derives for them.

Difficulty

The obvious shortcut for Theorem 7.3 — reuse Theorem 7.2's hypothesis and conclusion verbatim with I(k)I(k)I(k) replaced by H(j)H(j)H(j) — conflates the preemptive and non-preemptive SBP policies: Remark 7.4 explicitly notes the underlying pathwise identity (7.4) (used directly by Theorem 7.2) holds unconditionally under preemption but only asymptotically, via a vanishing-remainder argument bounding the leftover processing time of interrupted-but-continuing jobs, under non-preemption — the theorem actually being formalized is about the harder, non-preemptive case. For Theorem 7.5, the central difficulty is that FCFS's defining property is a genuinely time-shifted identity (departures at t+W^k(t)t + \hat W_k(t)t+W^k​(t) match arrivals at ttt), not a same-instant conditional statement like the non-idling and SBP equations — an approach that tried to state FCFS as a same-instant condition on T^\hat TT^ or D^\hat DD^ alone, without introducing the auxiliary workload process W^\hat WW^, could not express the theorem's actual content. A further subtlety Theorem 7.8's proof flags directly (Remark 7.9) is that the tempting converse — "Z^i(t)=0\hat Z_i(t) = 0Z^i​(t)=0 implies zero service rate" — is false in general (a corrected version appears only later, as Lemma 8.9); this mission's goal and milestone statements are careful to assert only the one-directional implication the book actually proves.

Formalization scope

Mission III's fluid-limit-path apparatus (Definition 6.6, u.o.c. convergence) is restated locally in this chapter's own namespace rather than imported, since drafts in this series do not import one another; the restatement is trimmed to the four raw processes (Dx,Fx,Tx,Zx)(D^x,F^x,T^x,Z^x)(Dx,Fx,Tx,Zx) this chapter's proofs need, omitting mission III's "delayed random walk" machinery. The non-idling and non-preemptive-SBP hypotheses are both formalized via one shared predicate, FullyUtilized, applied to different index sets (I(k)I(k)I(k) vs. H(j)H(j)H(j)) — the pathwise full-utilization identity (7.4) that each policy's proof establishes for its own priority classes, taken as a hypothesis rather than re-derived from a lower-level model of server scheduling (Chapter 2's construction of the service-starting mechanism is out of scope for this chapter, exactly as it was for mission III's SPNProcessFamily). Likewise, the FCFS goal theorem hypothesizes the raw identity (7.12) (rewritten via the material-balance equation to avoid needing the raw arrival process) and the fluid-scaled limit of the raw workload process (7.17), rather than re-deriving either from the "delayed random walk" VVV of Eq. (6.47). A formalization that dropped the workload shift W^k(t)\hat W_k(t)W^k​(t) from Theorem 7.5's conclusion, or that stated Theorem 7.8's converse implication (which Remark 7.9 explicitly disclaims), would each be an unfaithful trivialization or overstatement ruled out here. QueueingNetworkData, ProcessFamily, FullyUtilized, and SatisfiesAssumption76 are the primary reusable contributions of this mission; contributions completing the four by sorry proofs — each of which needs the u.o.c.-convergence and dominated-convergence arguments mission III's own proofs still lack — are welcome.

Selected references

  • J. G. Dai and J. Michael Harrison, Processing Networks: Fluid Models and Stability, Cambridge University Press (forthcoming), pre-publication draft 2020-4-2. http://spnbook.org
  • M. Bramson, "Convergence to equilibria for fluid models of FIFO queueing networks," Queueing Systems 22 (1996), 5–45.
  • M. Bramson, "Instability of FIFO queueing networks," Annals of Applied Probability 4 (1994), 414–431.
  • A. N. Rybko and A. L. Stolyar, "Ergodicity of stochastic processes describing the operation of open queueing networks," Problemy Peredachi Informatsii 28 (1992), 3–26.
9 thms1 active userReviewed
Control TheoryDynamical SystemsOperations Research+1·Captain: mikedeng1

Stabilization of Hybrid Systems by Feedback Control Based on Discrete-Time State Observations I: Almost Sure Asymptotic StabilityResearch Paper

Motivation

Many engineered systems switch between a finite number of operating modes at random times: a power grid after a line failure, a networked controller whose links drop, a manufacturing plant whose machines break down and are repaired. A standard model for such systems is a hybrid stochastic differential equation, also called an SDE with Markovian switching: the state follows an Itô equation whose coefficients depend on a mode that evolves as a continuous-time Markov chain. The monograph of Mao and Yuan (Stochastic Differential Equations with Markovian Switching, 2006) develops the stability theory of these equations.

A controller that stabilizes such a system usually needs the current state. In practice the state is sampled: it is observed at times 0,τ,2τ,…0,\tau,2\tau,\dots0,τ,2τ,… and the control is held between observations. Mao (Automatica 49, 2013) showed that, under a global Lipschitz condition on the drift and diffusion, a feedback control based on discrete-time observations stabilizes a hybrid SDE in the sense of mean-square exponential stability when τ\tauτ is small enough. You, Liu, Lu, Mao and Qiu (SIAM J. Control Optim. 53(2), 2015) replaced that condition by local Lipschitz continuity plus linear growth, gave an explicit bound (3.5) on the admissible observation interval τ\tauτ, and proved H∞H_\inftyH∞​-stability, mean-square asymptotic stability, almost sure asymptotic stability and exponential stability of the controlled system. This mission formalizes the almost sure asymptotic stability result, Theorem 3.4, and the results it is built on.

Setting

Let (Ω,F,{Ft}t≥0,P)(\Omega,\mathcal F,\{\mathcal F_t\}_{t\ge0},\mathbb P)(Ω,F,{Ft​}t≥0​,P) be a probability space with a filtration satisfying the usual conditions (increasing, right-continuous, F0\mathcal F_0F0​ contains the null sets). On it live an mmm-dimensional {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion www and a right-continuous {Ft}\{\mathcal F_t\}{Ft​}-Markov chain rrr on S={1,…,N}S=\{1,\dots,N\}S={1,…,N} with generator Γ=(γij)\Gamma=(\gamma_{ij})Γ=(γij​) (γij≥0\gamma_{ij}\ge0γij​≥0 for i≠ji\ne ji=j, zero row sums), independent of www. Fix τ>0\tau>0τ>0 and the sampling time δt=[t/τ]τ\delta_t=[t/\tau]\tauδt​=[t/τ]τ, the last observation time up to ttt. The controlled system is

dx(t)=(f(x(t),r(t),t)+u(x(δt),r(t),t))dt+g(x(t),r(t),t) dw(t),x(0)=x0, r(0)=r0,(2.1)dx(t)=\big(f(x(t),r(t),t)+u(x(\delta_t),r(t),t)\big)dt+g(x(t),r(t),t)\,dw(t),\qquad x(0)=x_0,\ r(0)=r_0,\tag{2.1}dx(t)=(f(x(t),r(t),t)+u(x(δt​),r(t),t))dt+g(x(t),r(t),t)dw(t),x(0)=x0​, r(0)=r0​,(2.1)

with f,u:Rn×S×R+→Rnf,u:\mathbb R^n\times S\times\mathbb R_+\to\mathbb R^nf,u:Rn×S×R+​→Rn and g:Rn×S×R+→Rn×mg:\mathbb R^n\times S\times\mathbb R_+\to\mathbb R^{n\times m}g:Rn×S×R+​→Rn×m. The feedback uuu sees the state only at the observation times.

The hypotheses are:

  • Assumption 2.1: f,gf,gf,g locally Lipschitz in xxx, and ∣f(x,i,t)∣≤K1∣x∣|f(x,i,t)|\le K_1|x|∣f(x,i,t)∣≤K1​∣x∣, ∣g(x,i,t)∣≤K2∣x∣|g(x,i,t)|\le K_2|x|∣g(x,i,t)∣≤K2​∣x∣ (∣g∣|g|∣g∣ the trace norm).
  • Assumption 2.2: ∣u(x,i,t)−u(y,i,t)∣≤K3∣x−y∣|u(x,i,t)-u(y,i,t)|\le K_3|x-y|∣u(x,i,t)−u(y,i,t)∣≤K3​∣x−y∣ and u(0,i,t)=0u(0,i,t)=0u(0,i,t)=0.
  • Assumption 3.1: there are U∈C2,1(Rn×S×R+;R+)U\in C^{2,1}(\mathbb R^n\times S\times\mathbb R_+;\mathbb R_+)U∈C2,1(Rn×S×R+​;R+​) and λ1,λ2>0\lambda_1,\lambda_2>0λ1​,λ2​>0 with LU(x,i,t)+λ1∣Ux(x,i,t)∣2≤−λ2∣x∣2\mathcal LU(x,i,t)+\lambda_1|U_x(x,i,t)|^2\le-\lambda_2|x|^2LU(x,i,t)+λ1​∣Ux​(x,i,t)∣2≤−λ2​∣x∣2, where
LU=Ut+Ux[f+u]+12trace⁡[gTUxxg]+∑jγijU(x,j,t).\mathcal LU=U_t+U_x[f+u]+\tfrac12\operatorname{trace}[g^TU_{xx}g]+\sum_j\gamma_{ij}U(x,j,t).LU=Ut​+Ux​[f+u]+21​trace[gTUxx​g]+j∑​γij​U(x,j,t).
  • Condition (3.5): λ2>τK32λ1[2τ(K12+2K32)+K22]\lambda_2>\frac{\tau K_3^2}{\lambda_1}\big[2\tau(K_1^2+2K_3^2)+K_2^2\big]λ2​>λ1​τK32​​[2τ(K12​+2K32​)+K22​] and τ≤14K3\tau\le\frac1{4K_3}τ≤4K3​1​.

In Lean these are Assumption21, Assumption22, C21, LU, Assumption31, Condition35, in the namespace You2015.Asymp; the basis is HybridSetup, the Itô integral IsItoIntegral, the sampling time delta, and solutions SolvesSampledHybridSDE, in the namespace You2015.Shared shared with the companion mission.

Formalization targets

Goal: Theorem 3.4 (almost sure asymptotic stability)

Under the hypotheses above, every solution of (2.1) satisfies

lim⁡t→∞x(t)=0a.s.\lim_{t\to\infty}x(t)=0\quad\text{a.s.}t→∞lim​x(t)=0a.s.

for all x0∈Rnx_0\in\mathbb R^nx0​∈Rn and r0∈Sr_0\in Sr0​∈S. No rate is claimed; the statement is the qualitative convergence of almost every path.

Milestones, in the order the proof uses them

  1. (3.15) E∣x(t)−x(δt)∣2≤2E∫δtt[τ∣f+u(x(δs),⋅)∣2+∣g∣2]ds\mathbb E|x(t)-x(\delta_t)|^2\le2\mathbb E\int_{\delta_t}^t[\tau|f+u(x(\delta_s),\cdot)|^2+|g|^2]dsE∣x(t)−x(δt​)∣2≤2E∫δt​t​[τ∣f+u(x(δs​),⋅)∣2+∣g∣2]ds.
  2. Theorem 3.2 (H∞H_\inftyH∞​-stability): ∫0∞E∣x(s)∣2ds<∞\int_0^\infty\mathbb E|x(s)|^2ds<\infty∫0∞​E∣x(s)∣2ds<∞.
  3. (3.21) E∣x(s)−x(δs)∣2≤3(τK12+K22)1−6τ2K32∫δssE∣x(z)∣2dz+6τ2K321−6τ2K32E∣x(s)∣2\mathbb E|x(s)-x(\delta_s)|^2\le\frac{3(\tau K_1^2+K_2^2)}{1-6\tau^2K_3^2}\int_{\delta_s}^s\mathbb E|x(z)|^2dz+\frac{6\tau^2K_3^2}{1-6\tau^2K_3^2}\mathbb E|x(s)|^2E∣x(s)−x(δs​)∣2≤1−6τ2K32​3(τK12​+K22​)​∫δs​s​E∣x(z)∣2dz+1−6τ2K32​6τ2K32​​E∣x(s)∣2.
  4. (3.23) sup⁡t≥0E∣x(t)∣2<∞\sup_{t\ge0}\mathbb E|x(t)|^2<\inftysupt≥0​E∣x(t)∣2<∞.
  5. ∣E∣x(t2)∣2−E∣x(t1)∣2∣≤C(t2−t1)|\mathbb E|x(t_2)|^2-\mathbb E|x(t_1)|^2|\le C(t_2-t_1)∣E∣x(t2​)∣2−E∣x(t1​)∣2∣≤C(t2​−t1​).
  6. Theorem 3.3: lim⁡t→∞E∣x(t)∣2=0\lim_{t\to\infty}\mathbb E|x(t)|^2=0limt→∞​E∣x(t)∣2=0.
  7. (3.24)–(3.25): E∫0∞∣x(t)∣2dt<∞\mathbb E\int_0^\infty|x(t)|^2dt<\inftyE∫0∞​∣x(t)∣2dt<∞ and lim inf⁡t→∞∣x(t)∣=0\liminf_{t\to\infty}|x(t)|=0liminft→∞​∣x(t)∣=0 a.s.
  8. (3.28): P(∃t:∣x(t)∣≥h)≤C/h2\mathbb P(\exists t:|x(t)|\ge h)\le C/h^2P(∃t:∣x(t)∣≥h)≤C/h2 for h>∣x0∣h>|x_0|h>∣x0​∣.

Significance

The result. Theorem 3.4 says that a controller sampling the state at rate 1/τ1/\tau1/τ makes almost every trajectory of the switching system converge to the equilibrium, with an explicit, checkable bound (3.5) on τ\tauτ. Mean-square convergence (Theorem 3.3) does not imply almost sure convergence in general, and a single trajectory is what an operator observes, so the pathwise statement is the one relevant to a deployed system. Condition (3.5) is stated in terms of the constants of Assumptions 2.1, 2.2 and 3.1, so for a concrete system (Section 6 of the paper) it gives a numerical bound on the observation interval.

Formalizing it. The results are proved in the paper; none of them is machine-checked. Mathlib has real Brownian motion but no Itô integral, no stochastic differential equations and no continuous-time Markov chains. The mission therefore also produces a reusable definition layer: a filtration under the usual conditions, a multidimensional {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion, an {Ft}\{\mathcal F_t\}{Ft​}-Markov chain with a given generator, the L2L^2L2 Itô integral of vector-valued integrands, and the solution notion of an SDE with Markovian switching and a sampled-state delay. A related but different layer exists on Prove2Me for Ethier–Kurtz (EthierKurtz_IsStandardBrownian, EthierKurtz_HasBrownianItoIntegral, EthierKurtz_SolvesBrownianSDE); it has no mode switching and no sampled state, so it cannot express (2.1).

Difficulty

Equation (2.1) is a stochastic differential delay equation with the delay t−δtt-\delta_tt−δt​, which is bounded but jumps at every observation time and has derivative 111 in between. The stability theorems for hybrid delay equations in the literature require a differentiable delay with derivative less than one (Mao–Yuan, p. 285), so they do not apply. Applying LU\mathcal LULU directly to U(x(t),r(t),t)U(x(t),r(t),t)U(x(t),r(t),t) leaves the term Ux[u(x(t))−u(x(δt))]U_x[u(x(t))-u(x(\delta_t))]Ux​[u(x(t))−u(x(δt​))], which has no sign and depends on the path over a whole observation interval, so a Lyapunov function of the current state alone does not close the argument.

For the goal, the natural first idea, deducing almost sure convergence from E∣x(t)∣2→0\mathbb E|x(t)|^2\to0E∣x(t)∣2→0 or from ∫0∞∣x(t)∣2dt<∞\int_0^\infty|x(t)|^2dt<\infty∫0∞​∣x(t)∣2dt<∞ a.s., fails: both are compatible with paths that make ever shorter excursions away from 000. The obstacle is to exclude infinitely many excursions of a fixed size, which neither moment statement controls.

Formalization scope

Conventions committed to in Lean:

  • The state space is EuclideanSpace ℝ (Fin n), so ∣x∣|x|∣x∣ is the Euclidean norm; the explicit constants in (3.5) and (3.21) depend on it. The diffusion ggg is given by its mmm columns and ∣g∣2=∑k∣gk∣2|g|^2=\sum_k|g_k|^2∣g∣2=∑k​∣gk​∣2 (trace norm). Modes are Fin N (0-based). Time is ℝ≥0; time integrals are over subsets of R\mathbb RR at s.toNNReal.
  • Every expectation E∣⋅∣2\mathbb E|\cdot|^2E∣⋅∣2 and every time integral of a nonnegative quantity is a lower Lebesgue integral in [0,∞][0,\infty][0,∞], so a non-integrable process cannot produce a junk value 000.
  • "The solution of (2.1)" is read as every process satisfying the solution definition: progressively measurable, almost surely continuous paths, E∣x(t)∣2<∞\mathbb E|x(t)|^2<\inftyE∣x(t)∣2<∞ for each ttt, and for each ttt, almost surely, the integral equation with Itô integrals in the L2L^2L2 sense. Existence and uniqueness (cited from Mao–Yuan on p. 908) are not asserted.
  • "An mmm-dimensional Brownian motion" and "a Markov chain with generator Γ\GammaΓ" are read in the Mao–Yuan framework the paper cites: an {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion with independent coordinates and increments independent of the past, and an {Ft}\{\mathcal F_t\}{Ft​}-Markov chain with transition matrix etΓe^{t\Gamma}etΓ. The usual conditions are kept as hypotheses.
  • "Locally Lipschitz" is uniform in the mode and time on each ball. C2,1C^{2,1}C2,1 carries its derivatives Ut,Ux,UxxU_t,U_x,U_{xx}Ut​,Ux​,Uxx​ as witnesses tied to UUU by derivative relations and joint continuity.
  • "τ>0\tau>0τ>0 sufficiently small for (3.5)" means every τ>0\tau>0τ>0 satisfying both inequalities of (3.5). U,λ1,λ2,τU,\lambda_1,\lambda_2,\tauU,λ1​,λ2​,τ are data of each statement. The paper's "CCC denotes a positive constant" is an existential chosen after x0x_0x0​, r0r_0r0​ and the solution, and before the time variables and hhh.
  • (3.15) and (3.21) are stated under fewer hypotheses than the surrounding proof has (Assumptions 2.1, 2.2, τ>0\tau>0τ>0, and for (3.21) τ≤1/(4K3)\tau\le1/(4K_3)τ≤1/(4K3​)), because their derivations use no more. Misprints on the page (for example g(x,i,s)=f(x,i,0)g(x,i,s)=f(x,i,0)g(x,i,s)=f(x,i,0) on p. 909 and the swapped definitions of ∨,∧\vee,\wedge∨,∧ on p. 907) are not formalized.

A trivializing formalization is ruled out: the expectations are not Bochner integrals (which vanish for non-integrable integrands), the solution notion admits the true solution and requires path continuity, the derivative witnesses of UUU are tied to UUU, and a sorry-free check shows that the data hypotheses (Assumptions 2.1, 2.2, 3.1, C2,1C^{2,1}C2,1, (3.5)) are satisfiable, for example by n=m=N=1n=m=N=1n=m=N=1, f=g=0f=g=0f=g=0, u(x)=−xu(x)=-xu(x)=−x, U=∣x∣2U=|x|^2U=∣x∣2, λ1=1/4\lambda_1=1/4λ1​=1/4, λ2=1\lambda_2=1λ2​=1, τ=1/10\tau=1/10τ=1/10.

Welcome contributions: the Itô isometry and Itô's formula for the L2L^2L2 integral defined here, a generalized Itô formula for functions of a Markov-modulated Itô process, and Doob's maximal inequality in continuous time. These are reusable far beyond this mission. Section 4 of the paper (exponential stability) is a separate mission of the same series.

Selected references

  • S. You, W. Liu, J. Lu, X. Mao, Q. Qiu, Stabilization of Hybrid Systems by Feedback Control Based on Discrete-Time State Observations, SIAM J. Control Optim. 53(2), 905–925, 2015. https://doi.org/10.1137/140985779
  • X. Mao, C. Yuan, Stochastic Differential Equations with Markovian Switching, Imperial College Press, 2006. https://doi.org/10.1142/p473
  • X. Mao, Stabilization of continuous-time hybrid stochastic differential equations by discrete-time feedback control, Automatica 49(12), 3677–3681, 2013. https://doi.org/10.1016/j.automatica.2013.09.005
13 thms1 active userReviewed
Control TheoryOperations ResearchOptimization+1·Captain: mikedeng1

A General Stochastic Maximum Principle for Optimal Control Problems: The Maximum Principle with First- and Second-Order Adjoint ProcessesResearch Paper

Motivation

Pontryagin's maximum principle gives necessary conditions for optimality in deterministic optimal control: along an optimal trajectory, the optimal control maximizes (or minimizes) a Hamiltonian built from an adjoint process. For a system driven by Brownian noise the analogous statement was open in full generality for two decades. The difficulty appears exactly when the diffusion coefficient depends on the control and the control domain is not convex, the situation of controlled volatility in finance, of controlled noise intensity in engineering, and of any problem whose admissible actions form a discrete or otherwise nonconvex set.

Shige Peng's 1990 paper (SIAM J. Control Optim. 28(4)) closed that case. It introduced the second-order adjoint process and a second-order variational inequality, and it is the starting point of the modern theory of stochastic Hamiltonian systems and of backward stochastic differential equations as a tool in control.

Timeline.

  • 1972: Kushner obtains necessary conditions for diffusions whose diffusion coefficient does not depend on the control (SIAM J. Control 10).
  • 1973–1978: Bismut introduces the adjoint equation as a linear backward stochastic differential equation and develops duality methods (SIAM Review 20).
  • Early 1980s: Bensoussan and Haussmann prove maximum principles for convex control domains or control-independent diffusion, using the first-order adjoint equation only.
  • 1990: Peng proves the general principle, with control-dependent diffusion and an arbitrary nonempty control domain (this mission). In the same year Pardoux and Peng prove existence and uniqueness for nonlinear backward SDEs (Systems Control Lett. 14).
  • 1999: Yong and Zhou give a textbook account of the theory (Springer).

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space carrying a standard ddd-dimensional Wiener process B=(B1,…,Bd)B=(B^1,\dots,B^d)B=(B1,…,Bd), and let Ft=σ{B(s);0≤s≤t}\mathcal F^t=\sigma\{B(s);0\le s\le t\}Ft=σ{B(s);0≤s≤t} be its natural filtration. Fix a horizon T>0T>0T>0, an initial state x0∈Rnx_0\in\mathbb R^nx0​∈Rn and a nonempty control domain U⊆RkU\subseteq\mathbb R^kU⊆Rk. The data are

g:Rn×Rk→Rn,σ=(σ1,…,σd), σj:Rn×Rk→Rn,l:Rn×Rk→R,h:Rn→R.g:\mathbb R^n\times\mathbb R^k\to\mathbb R^n,\quad \sigma=(\sigma^1,\dots,\sigma^d),\ \sigma^j:\mathbb R^n\times\mathbb R^k\to\mathbb R^n,\quad l:\mathbb R^n\times\mathbb R^k\to\mathbb R,\quad h:\mathbb R^n\to\mathbb R .g:Rn×Rk→Rn,σ=(σ1,…,σd), σj:Rn×Rk→Rn,l:Rn×Rk→R,h:Rn→R.

An admissible control vvv is a progressively measurable UUU-valued process with sup⁡t≤TE∣v(t)∣m<∞\sup_{t\le T}E|v(t)|^m<\inftysupt≤T​E∣v(t)∣m<∞ for every m≥1m\ge1m≥1. Its trajectory solves the state equation

dx(t)=g(x(t),v(t)) dt+∑j=1dσj(x(t),v(t)) dBj(t),x(0)=x0,dx(t)=g(x(t),v(t))\,dt+\sum_{j=1}^d\sigma^j(x(t),v(t))\,dB^j(t),\qquad x(0)=x_0,dx(t)=g(x(t),v(t))dt+j=1∑d​σj(x(t),v(t))dBj(t),x(0)=x0​,

and its cost is J(v)=E∫0Tl(x(t),v(t)) dt+E h(x(T))J(v)=E\int_0^Tl(x(t),v(t))\,dt+E\,h(x(T))J(v)=E∫0T​l(x(t),v(t))dt+Eh(x(T)). A pair (y,u)(y,u)(y,u) is optimal when J(u)≤J(v)J(u)\le J(v)J(u)≤J(v) for every admissible vvv.

Assumption (3): g,σ,l,hg,\sigma,l,hg,σ,l,h are C2C^2C2 in xxx, jointly continuous in (x,v)(x,v)(x,v) together with their first and second xxx-derivatives; gx,gxx,σx,σxx,lxx,hxxg_x,g_{xx},\sigma_x,\sigma_{xx},l_{xx},h_{xx}gx​,gxx​,σx​,σxx​,lxx​,hxx​ are bounded; and g,σ,lx,hxg,\sigma,l_x,h_xg,σ,lx​,hx​ grow at most like C(1+∣x∣+∣v∣)C(1+|x|+|v|)C(1+∣x∣+∣v∣).

The Hamiltonian is H(x,v,p,K)=l(x,v)+(p,g(x,v))+∑j(Kj,σj(x,v))H(x,v,p,K)=l(x,v)+(p,g(x,v))+\sum_j(K_j,\sigma^j(x,v))H(x,v,p,K)=l(x,v)+(p,g(x,v))+∑j​(Kj​,σj(x,v)). The first-order adjoint process (p,K)(p,K)(p,K) solves the backward equation

−dp=[gx∗p+∑jσxj∗Kj+lx]dt−∑jKj dBj,p(T)=hx(y(T)),-dp=\Big[g_x^*p+\sum_j\sigma_x^{j*}K_j+l_x\Big]dt-\sum_jK_j\,dB^j,\qquad p(T)=h_x(y(T)),−dp=[gx∗​p+j∑​σxj∗​Kj​+lx​]dt−j∑​Kj​dBj,p(T)=hx​(y(T)),

and the second-order adjoint process (P,Q)(P,Q)(P,Q), symmetric-matrix valued, solves

−dP=[gx∗P+Pgx+∑jσxj∗Pσxj+∑jσxj∗Qj+∑jQjσxj+Hxx]dt−∑jQj dBj,P(T)=hxx(y(T)),-dP=\Big[g_x^*P+Pg_x+\sum_j\sigma_x^{j*}P\sigma_x^j+\sum_j\sigma_x^{j*}Q_j+\sum_jQ_j\sigma_x^j+H_{xx}\Big]dt-\sum_jQ_j\,dB^j,\qquad P(T)=h_{xx}(y(T)),−dP=[gx∗​P+Pgx​+j∑​σxj∗​Pσxj​+j∑​σxj∗​Qj​+j∑​Qj​σxj​+Hxx​]dt−j∑​Qj​dBj,P(T)=hxx​(y(T)),

with all coefficients evaluated along (y(t),u(t))(y(t),u(t))(y(t),u(t)) and both solutions adapted to Ft\mathcal F^tFt.

Formalization targets

Goal: Theorem 3 (p. 975)

If (y,u)(y,u)(y,u) is optimal, then adjoint processes (p,K)(p,K)(p,K) and (P,Q)(P,Q)(P,Q) exist in LF2L^2_{\mathcal F}LF2​, solving the two equations above, such that for every v∈Uv\in Uv∈U, for almost every τ∈[0,T]\tau\in[0,T]τ∈[0,T], almost surely,

H(y,v,p,K−Pσ(y,u))+12tr⁡(σσ∗(y,v)P) ≥ H(y,u,p,K−Pσ(y,u))+12tr⁡(σσ∗(y,u)P),H\big(y,v,p,K-P\sigma(y,u)\big)+\tfrac12\operatorname{tr}\big(\sigma\sigma^*(y,v)P\big)\ \ge\ H\big(y,u,p,K-P\sigma(y,u)\big)+\tfrac12\operatorname{tr}\big(\sigma\sigma^*(y,u)P\big),H(y,v,p,K−Pσ(y,u))+21​tr(σσ∗(y,v)P) ≥ H(y,u,p,K−Pσ(y,u))+21​tr(σσ∗(y,u)P),

all evaluated at time τ\tauτ.

Milestones

  1. Lemma 1: the spike-perturbed state equals y+y1+y2y+y_1+y_2y+y1​+y2​ up to o(ε2)o(\varepsilon^2)o(ε2) in mean square, where y1,y2y_1,y_2y1​,y2​ solve the first- and second-order variational equations (5), (6).
  2. Lemma 2: the cost expansion (11) is ≥o(ε)\ge o(\varepsilon)≥o(ε) at an optimal control.
  3. Eq. (13): existence and uniqueness of (p,K)(p,K)(p,K) as a Riesz representer.
  4. Eq. (14): the cost expansion in Hamiltonian form is ≥o(ε)\ge o(\varepsilon)≥o(ε).
  5. Eq. (17): existence and uniqueness of (P,Q)(P,Q)(P,Q) as a Riesz representer.
  6. Eq. (18): the variational inequality for these representers.
  7. Eq. (19): (p,K)(p,K)(p,K) is the unique solution of the first-order adjoint equation.
  8. Eq. (20): (P,Q)(P,Q)(P,Q) solves the second-order adjoint equation.

Significance

The result. Theorem 3 is the necessary condition for optimal control of diffusions in its general form. When σ\sigmaσ does not depend on the control the trace terms cancel and it reduces to the classical first-order principle. When the control enters the diffusion, the first-order condition is false in general, and the second-order adjoint PPP is the correction. The theorem underlies stochastic linear-quadratic theory, the verification of optimal portfolio and volatility-control policies, and the relation between the maximum principle and the Hamilton–Jacobi–Bellman equation.

Formalizing it. The theorem is classical and proved; none of it is machine-checked. Mathlib has real Brownian motion but no stochastic integral, no SDE and no backward SDE. This mission produces the first formal statements on the platform of a controlled SDE, of a backward SDE and of the maximum principle, together with a precise definition layer (Itô integral, Itô process, BSDE solution) that later missions can reuse, e.g. for Peng's endpoint-constrained principle (§6 of the paper) or for the existence theory of BSDEs. A formal proof would also pin down the approximation arguments the paper leaves to the reader.

Difficulty

The obvious route perturbs the optimal control convexly, u+ε(v−u)u+\varepsilon(v-u)u+ε(v−u), and differentiates the cost. That needs UUU convex. For nonconvex UUU one uses a spike variation on a time interval of length ε\varepsilonε. For deterministic systems the state then moves by O(ε)O(\varepsilon)O(ε) and a first-order expansion suffices. With control-dependent diffusion the stochastic integral over the spike interval moves the state by order ε\sqrt\varepsilonε​ in L2L^2L2, so the first-order variational equation leaves an error of the same order as the effect being measured. Second-order terms in the state enter the cost at order ε\varepsilonε, and they are quadratic, so they cannot be handled by a single linear adjoint. The second-order expansion, the matrix-valued adjoint that represents the quadratic term, and the identification of both adjoints with backward SDEs are where the work lies. On the formal side, none of the stochastic calculus exists in Mathlib: the Itô isometry, Itô's formula for matrix-valued processes, moment estimates for linear SDEs and the martingale representation behind the backward equations all have to be built.

Formalization scope

Conventions committed to in Lean:

  • States, controls and noise are Fin n → ℝ, Fin k → ℝ, Fin d → ℝ with the sup norm; matrices are Matrix (Fin n) (Fin n) ℝ. Time is ℝ≥0, and time integrals are over [0, t] ⊂ ℝ.
  • The Wiener process is Rd\mathbb R^dRd-valued: the paper's "RnR^nRn-valued standard Wiener process" (p. 967) is a misprint, since σ(x,v)∈L(Rd,Rn)\sigma(x,v)\in\mathcal L(R^d,R^n)σ(x,v)∈L(Rd,Rn). Coordinates are independent real Brownian motions (Mathlib's IsBrownianReal).
  • The filtration is the natural filtration of BBB, not completed, as on p. 967.
  • "Adapted", for processes integrated in dtdtdt, is read as progressively measurable.
  • The Itô integral is a relation (an L2L^2L2 limit of elementary integrals, as in Ikeda–Watanabe), not an operator. SDE and BSDE solutions hold "for every ttt, almost surely", with sup⁡tE∣x(t)∣2<∞\sup_tE|x(t)|^2<\inftysupt​E∣x(t)∣2<∞ for forward solutions and LF2L^2_{\mathcal F}LF2​ membership for backward ones.
  • Optimality is among admissible controls of finite cost, and the optimal cost is finite; the paper never states finiteness, and a cost can be +∞+\infty+∞ under (3).
  • Lemma 1 is stated with o(ε2)o(\varepsilon^2)o(ε2) where the page prints "≤Cε2\le C\varepsilon^2≤Cε2" in (4). The proof (via (10)) establishes o(ε2)o(\varepsilon^2)o(ε2), and Lemma 2 needs it. Lemma 1, (13), (17), (19) and (20) are stated for any admissible pair, since their proofs do not use optimality.
  • "≥o(ε)\ge o(\varepsilon)≥o(ε)" means: some r(ε)=o(ε)r(\varepsilon)=o(\varepsilon)r(ε)=o(ε) as ε→0+\varepsilon\to0^+ε→0+ bounds the left side from below for small ε\varepsilonε. "∀v∈U\forall v\in U∀v∈U, a.e., a.s." quantifies vvv first, then τ\tauτ, then ω\omegaω.
  • PPP and QjQ_jQj​ are symmetric-valued (Rn,nR^{n,n}Rn,n is the space of symmetric matrices, p. 973). Stochastic integrals against the matrix σ\sigmaσ or QQQ are sums over the columns, ∑j(⋅)j dBj\sum_j(\cdot)_j\,dB^j∑j​(⋅)j​dBj.

Trivializing formalizations ruled out. Without adaptedness the backward equations have pathwise solutions with K=0K=0K=0 and the goal would be free; every adjoint and every solution is required to be progressive for the natural filtration of BBB. The hypotheses are satisfiable: a sorry-free check shows that the zero problem has an optimal pair and that the Itô relation holds for the zero integrand.

Infrastructure needed, and reusable. The Itô integral and isometry, Itô's formula (vector and matrix forms), existence, uniqueness and moment estimates for linear SDEs with bounded coefficients, Riesz representation in LF2L^2_{\mathcal F}LF2​, and existence and uniqueness for linear BSDEs (via martingale representation for the Brownian filtration). All of these are reusable well beyond this mission; contributions of any of them, as separate theorems, are welcome. Related platform definitions: the Ethier–Kurtz series (EthierKurtz_HasBrownianItoIntegral, EthierKurtz_SolvesBrownianSDE) formalizes an Itô integral by dyadic step approximation and uncontrolled SDEs over a completed filtration. The deterministic Pontryagin principle appears in Vector Space Methods XII and Dynamic Programming and Optimal Control III.

Selected references

  • S. Peng, A General Stochastic Maximum Principle for Optimal Control Problems, SIAM J. Control Optim. 28(4), 966–979, 1990. https://doi.org/10.1137/0328054
  • H. J. Kushner, Necessary Conditions for Continuous Parameter Stochastic Optimization Problems, SIAM J. Control 10(3), 550–565, 1972. https://doi.org/10.1137/0310041
  • J.-M. Bismut, An Introductory Approach to Duality in Optimal Stochastic Control, SIAM Review 20(1), 62–78, 1978. https://doi.org/10.1137/1020004
  • E. Pardoux and S. Peng, Adapted Solution of a Backward Stochastic Differential Equation, Systems & Control Letters 14(1), 55–61, 1990. https://doi.org/10.1016/0167-6911(90)90082-6
  • J. Yong and X. Y. Zhou, Stochastic Controls: Hamiltonian Systems and HJB Equations, Springer, 1999. https://doi.org/10.1007/978-1-4612-1466-3
12 thms1 active userReviewed
Markov ChainOperations ResearchProbability·Captain: mikedeng1

Open, Closed, and Mixed Networks of Queues with Different Classes of Customers: The Product-Form Equilibrium DistributionResearch Paper

Motivation

Networks of queues model computer systems, communication networks and manufacturing lines: customers (jobs, packets, parts) move between service centers, wait, receive service and move on. Their equilibrium behaviour determines throughputs, utilizations and response times, and for most networks it can only be computed by solving the full balance equations of a continuous-time Markov chain whose state space grows combinatorially with the number of centers and customers. A product-form network is one whose equilibrium distribution factorizes over the centers; for such networks performance measures can be computed exactly by efficient algorithms (convolution, mean value analysis), and this is the basis of much of classical computer-performance modelling.

Timeline of the main product-form results:

  • 1957–1963, Jackson (Oper. Res. 5, 1957; Manag. Sci. 10, 1963): open networks of exponential FCFS queues, one customer class, Poisson arrivals.
  • 1967, Gordon and Newell (Oper. Res. 15): the closed single-class exponential case.
  • 1975, Baskett, Chandy, Muntz and Palacios (J. ACM 22): several customer classes with class switching, four service disciplines (FCFS, processor sharing, infinite server, preemptive-resume LCFS), service times with rational Laplace transforms at the last three, and open, closed or mixed networks with state-dependent Poisson arrivals. This is the BCMP theorem, the subject of this mission.
  • 1975–1979, Kelly (J. Appl. Prob. 12, 1975; Reversibility and Stochastic Networks, Wiley 1979): symmetric queues and quasi-reversibility, a general framework containing the BCMP disciplines.

Setting

A network has NNN service centers and RRR customer classes. A class-rrr customer finishing service at center iii next requires center jjj in class sss with probability pi,r;j,sp_{i,r;j,s}pi,r;j,s​ and leaves the network with probability 1−∑j,spi,r;j,s1-\sum_{j,s}p_{i,r;j,s}1−∑j,s​pi,r;j,s​. The pairs (i,r)(i,r)(i,r) are partitioned into subchains E1,…,EmE_1,\dots,E_mE1​,…,Em​ that routing never leaves. Each center has one of four types:

  1. FCFS, with an exponential service time of rate μi\mu_iμi​ common to all classes;
  2. a single processor-sharing server (each of nnn customers is served at rate 1/n1/n1/n);
  3. an infinite-server center;
  4. a single preemptive-resume LCFS server.

At types 2–4 the class-rrr service time is Coxian: uir≥1u_{ir}\ge1uir​≥1 exponential stages of rates μirl\mu_{irl}μirl​, and after stage lll the customer continues with probability airla_{irl}airl​ or finishes with probability birl=1−airlb_{irl}=1-a_{irl}birl​=1−airl​. The state S=(x1,…,xN)S=(x_1,\dots,x_N)S=(x1​,…,xN​) records the FCFS order of classes at type 1, the number mirlm_{irl}mirl​ of class-rrr customers in stage lll at types 2 and 3, and the LCFS order of (class, stage) pairs at type 4. External arrivals are Poisson, either with rate λ(M(S))\lambda(M(S))λ(M(S)) depending on the total population M(S)M(S)M(S) (process A) or with one stream per subchain of rate λk(M(S/Ek))\lambda_k(M(S/E_k))λk​(M(S/Ek​)) (process B); an arrival joins center jjj in class sss with probability qjsq_{js}qjs​. A subchain with q≡0q\equiv0q≡0 is closed and keeps a fixed population KkK_kKk​.

With relative arrival rates eir≥0e_{ir}\ge0eir​≥0 solving the traffic equations ∑(i,r)eirpi,r;j,s+qjs=ejs\sum_{(i,r)}e_{ir}p_{i,r;j,s}+q_{js}=e_{js}∑(i,r)​eir​pi,r;j,s​+qjs​=ejs​ and Airl=∏j<lairjA_{irl}=\prod_{j<l}a_{irj}Airl​=∏j<l​airj​ (the probability of reaching stage lll, stages numbered from 0), the paper defines fi(xi)f_i(x_i)fi​(xi​) per center type and a factor d(S)d(S)d(S) from the arrival rates.

Formalization targets

Goal: the BCMP theorem (§3.2, pp. 253–254)

π(S)=d(S) f1(x1) f2(x2)⋯fN(xN)\pi(S)=d(S)\,f_1(x_1)\,f_2(x_2)\cdots f_N(x_N)π(S)=d(S)f1​(x1​)f2​(x2​)⋯fN​(xN​)

satisfies the global balance equations of the network, and, under the paper's assumption that the equilibrium distribution is unique, every equilibrium distribution equals π/Z\pi/Zπ/Z whenever Z=∑Sπ(S)Z=\sum_S\pi(S)Z=∑S​π(S) is finite and positive. The goal covers all four center types, open, closed and mixed networks, and both arrival processes.

Milestones

  • §3.1 (p. 252): independent balance implies global balance.
  • §3.2 (p. 254): the product form satisfies the independent balance equations.
  • §4.1 (p. 254): the aggregate-state probabilities are C d(S) g1(y1)⋯gN(yN)C\,d(S)\,g_1(y_1)\cdots g_N(y_N)Cd(S)g1​(y1​)⋯gN​(yN​).

A further supporting item, also from §4.1 (p. 254), states that summing fif_ifi​ over local states with fixed class counts gives gig_igi​. So gig_igi​ depends on the service times only through their means 1/μir=∑lAirl/μirl1/\mu_{ir}=\sum_lA_{irl}/\mu_{irl}1/μir​=∑l​Airl​/μirl​.

Significance

The theorem places the four disciplines, class switching and mixed open/closed populations under one formula. Its corollary in §4.1, that aggregate probabilities depend on service time distributions only through their means (insensitivity), is what makes the model usable with measured mean service times, and it underlies the convolution and mean value analysis algorithms for normalizing constants.

The result is classical and proved on paper. As far as the platform's catalogue shows, it is not formalized: the platform has Kelly's single-class migration process with exponential service, a special case. A machine-checked BCMP theorem would provide a verified multiclass queueing-network model (states, event-driven transition rates, balance equations) on which later results can build: mean value analysis, the state-dependent rates of §5, and the open-network marginals of §4.2.

The printed statement contains an error. The paper defines Airl=∏j=1lairjA_{irl}=\prod_{j=1}^{l}a_{irj}Airl​=∏j=1l​airj​ (p. 253). With the branching of its Figs. 1 and 3, this product includes the branch out of stage lll. For exponential service (uir=1u_{ir}=1uir​=1) it gives Air1=air1=0A_{ir1}=a_{ir1}=0Air1​=air1​=0, so every fif_ifi​ of a type 2–4 center with a customer present vanishes, and a closed network of such centers would have no normalizable solution. The mission states the corrected theorem with Airl=∏j<lairjA_{irl}=\prod_{j<l}a_{irj}Airl​=∏j<l​airj​, which the mean-service-time identity of §4.1 also requires. The type-2 factor 1/mikl!1/m_{ikl}!1/mikl​! is read as 1/mirl!1/m_{irl}!1/mirl​!.

Difficulty

The algebra of the paper's proof is local: each independent balance equation reduces to the traffic equations. The difficulty is in making that statement precise for a real state space. The independent balance equations need a consistent labelling of each moving customer by the "stage" it leaves and enters. That labelling has to cover FCFS centers, where per-class labels are inconsistent (p. 253), the outside world of each open subchain, and LCFS preemption. Every in-flow into a state is a sum over predecessor states, and those states differ by list operations (appending at an FCFS tail, pushing on an LCFS head) or by stage-count updates. The factorials in the processor-sharing and infinite-server factors, and the telescoping identity ∑lAirlbirl=1\sum_lA_{irl}b_{irl}=1∑l​Airl​birl​=1 for departures, must line up exactly with the rates. The obvious shortcut is to check global balance directly for a single class with exponential service. That covers neither class switching, nor Coxian stages, nor mixed networks.

Formalization scope

Centers are Fin N, classes Fin R and subchains Fin m. The class-rrr stages at center iii are Fin (u i r) with u i r : ℕ+, numbered from 0. A local state is an inductive type with three shapes (FCFS list, stage-count array, LCFS list of (class, stage) pairs). The state space is the subtype of configurations whose shapes match the center types and whose closed subchains hold their fixed populations. Transition rates are the sums of the rates of explicit events (arrivals, FCFS completions, stage moves and completions, LCFS moves and completions). Global balance uses tsum; every state has finitely many successors and predecessors with nonzero rate, so these sums are finite. The standing assumptions (substochastic routing closed on subchains, closed subchains with no arrivals and no departures, positive rates, continuation probabilities in [0,1][0,1][0,1] vanishing at the last stage) are collected in Network.IsValid. Irreducibility of subchains is not assumed, and any nonnegative solution of the traffic equations is allowed. Under process B the product in d(S)d(S)d(S) runs over open subchains only. Uniqueness of the equilibrium is a hypothesis, as in the paper. The type-1 rate is constant, and the state-dependent rates of Condition 1 and §5 are not covered.

The following formalizations would trivialize the mission and are ruled out: stating only global balance of π\piπ (satisfied by π≡0\pi\equiv0π≡0), quantifying over arbitrary rate functions instead of the rates built from the network data, and restricting the goal to exponential service or to a single class.

Needed infrastructure: finite-support tsum manipulations, multinomial identities for the §4.1 sums over orderings and stage assignments, and bookkeeping for list and array updates. The model and the balance-equation layer can be reused for later queueing missions. Contributions are welcome on each milestone, on the per-center-type pieces of the independent balance check, and on helper lemmas about the event system.

Selected references

  • F. Baskett, K. M. Chandy, R. R. Muntz, F. G. Palacios, Open, Closed, and Mixed Networks of Queues with Different Classes of Customers, J. ACM 22(2):248–260, 1975. https://doi.org/10.1145/321879.321887
  • J. R. Jackson, Networks of Waiting Lines, Operations Research 5(4):518–521, 1957. https://doi.org/10.1287/opre.5.4.518
  • J. R. Jackson, Jobshop-like Queueing Systems, Management Science 10(1):131–142, 1963. https://doi.org/10.1287/mnsc.10.1.131
  • W. J. Gordon, G. F. Newell, Closed Queuing Systems with Exponential Servers, Operations Research 15(2):254–265, 1967. https://doi.org/10.1287/opre.15.2.254
  • F. P. Kelly, Reversibility and Stochastic Networks, Wiley, 1979. http://www.statslab.cam.ac.uk/~frank/rsn.html
  • D. R. Cox, A Use of Complex Probabilities in the Theory of Stochastic Processes, Proc. Cambridge Phil. Soc. 51:313–319, 1955. https://doi.org/10.1017/S0305004100030231
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Markov Processes: Characterization and Convergence IV: Martingale characterization of Markov processesTextbook

From local evolution to a Markov process

A stochastic process can be described through the way functions of its state change over time. For a suitable pair of functions f and g, the difference between f evaluated along the process and the accumulated integral of g has zero conditional drift. A martingale problem specifies a collection of such pairs. The question is whether these local conditions determine the evolution of the process, including the dependence of its future on its past. Ethier and Kurtz's Chapter 4, Theorem 4.1 answers this question under analytic hypotheses on the collection of pairs and a separation condition on the functions being observed.

State space, functions, and histories

Let E be a separable metric space, with its Borel sigma algebra. Write B(E) for the bounded real Borel functions, equipped with the uniform norm. A linear relation A is a linear subspace of B(E) × B(E). A pair (f,g) in A prescribes g as the drift associated with f; the relation is allowed to be multivalued. It is dissipative when

a∥f∥≤∥af−g∥((f,g)∈A, a>0).a\|f\|\leq\|af-g\|\qquad ((f,g)\in A,\ a>0).a∥f∥≤∥af−g∥((f,g)∈A, a>0).

Let μ be a probability measure on E. A solution X of the martingale problem for (A,μ) is a jointly measurable process on a probability space with initial law μ, satisfying the compensated moment identities of Chapter 4, equation (3.4). Those identities test each compensated increment against products of bounded Borel functions of finitely many earlier states. The natural past at time s is the sigma algebra generated by all coordinates X(r) with r≤s.

A subspace L of B(E) is separating if two Borel probability measures that have the same integral against every function in L must be equal. This is a condition on measures, stronger in purpose than merely distinguishing individual states.

Characterization target

Suppose A′ is a linear subrelation of A and, for some λ>0,

R(λ−A′)‾=D(A′)‾=L,\overline{\mathcal R(\lambda-A')}=\overline{\mathcal D(A')}=L,R(λ−A′)​=D(A′)​=L,

where both closures use the uniform norm and L is separating. Given a solution X of (A,μ), the target is the existence of a strongly continuous contraction semigroup T on L generated by the closed relation A′‾\overline{A'}A′, together with

E[f(X(s+t))∣FsX]=(T(t)f)(X(s))(s,t≥0, f∈L).\mathbb E[f(X(s+t))\mid\mathcal F_s^X]=(T(t)f)(X(s))\quad(s,t\geq0,\ f\in L).E[f(X(s+t))∣FsX​]=(T(t)f)(X(s))(s,t≥0, f∈L).

The process is Markov: for every bounded Borel observable, conditioning a future observation on the entire past agrees almost surely with conditioning on the present state. In addition, any other solution with initial law μ has exactly the same finite-dimensional distributions as X. The competing solution may live on a different probability space. Existence of X is an assumption; the existence conclusion concerns its corresponding semigroup.

What the characterization establishes

The theorem joins an analytic description of evolution with a probabilistic one. The closed generator relation determines a semigroup, while the martingale identities identify the conditional evolution of the supplied process. Separation allows observables in L to determine probability laws. Uniqueness concerns every finite list of observation times, which is the source's convention for this martingale problem.

This is a known theorem of Ethier and Kurtz. The formalization target is its complete statement and eventually a machine-checked proof. The present theorem remains a proof obligation. Its expression infrastructure consists of bounded functions, the natural past, and the finite-history definition of a solution.

Mathematical difficulty

The observed functions initially lie in a subspace L, whereas the Markov conclusion ranges over all bounded Borel observations. Identifying only individual expectations does not by itself establish conditional evolution or equality of joint laws. The analytic part must also identify the entire generator graph: agreement on the original relation alone is weaker than the asserted equality with its closure. Both closure hypotheses and probability-measure separation are therefore part of the target.

Formalization scope

Bounded functions are actual pointwise real functions with the uniform norm. Borel measurability is imposed on the relation, and uniform limits preserve it. The construction does not use functions modulo almost-everywhere equality. The state space is separable and metric; completeness and local compactness are not additional hypotheses. Processes need no right-continuous or cadlag paths.

Histories may be empty, repeated, or unordered, with every history time at most the start of the increment. Products combine repeated observations. Boundedness and finite time intervals ensure the required integrability. Nonnegative real times index the processes. The semigroup is represented by a real-indexed family whose axioms concern nonnegative times; negative-time values have no mathematical role. Generator equality is a biconditional for the derivative limit from positive times. The target retains semigroup correspondence, the ordinary Markov property, and unrestricted finite-dimensional uniqueness as one theorem.

Selected references

Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 4, Theorem 4.1, printed p.182 (PDF p.191); equations (3.4) and (4.2), printed pp.174 and 183. Separation conventions: Chapter 3, printed pp.112 and 116. Chapter 4.

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