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Control Theory

156 missions · 36 completed

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Dynamical SystemsOperations Research·Captain: mikedeng1

Dynamic Instabilities and Stabilization Methods in Distributed Real-Time Scheduling of Manufacturing Systems 4: A Run-Truncating Priority-Queue Supervisor Keeps Every Buffer Bounded When ρₘ < 1Research Paper

Motivation

A flexible manufacturing system routes several part types through a set of machines; a machine that switches from one kind of part to another must spend a set-up time first. Each machine has to decide, in real time and from local information only, which of its waiting buffers to work on and for how long. Long runs waste little time on set-ups but starve other buffers; short runs do the opposite.

Kumar and Seidman (IEEE TAC 35(3), 1990) showed in §III of the paper that natural distributed rules (clearing policies, which keep processing a buffer until it is empty) can be unstable when parts revisit machines, even though every machine has enough capacity. Their §IV gives a sufficient condition for a subclass of such rules to be stable, which is stricter than the capacity condition. §V, the subject of this mission, asks for something stronger: a simple, distributed mechanism that a supervisor can add to any scheduling policy and that makes the system stable whenever the capacity condition alone holds.

Timeline. Perkins and Kumar (1989) proved that the capacity condition is sufficient for the existence of some stabilizing policy, and that every clear-a-fraction policy is stable on acyclic systems. Kumar and Seidman (1990) gave the instability examples for nonacyclic systems and the universal supervisor formalized here.

Setting

There are PPP part types and MMM machines. Part type ppp arrives at rate dp>0d_p>0dp​>0 and follows a route of npn_pnp​ operations; operation iii is done by machine μp,i\mu_{p,i}μp,i​ and takes τp,i>0\tau_{p,i}>0τp,i​>0 per part. Parts awaiting operation iii wait in buffer bp,ib_{p,i}bp,i​, with level xp,i(t)≥0x_{p,i}(t)\ge 0xp,i​(t)≥0. Machine mmm serves Bm={bp,i:μp,i=m}B_m=\{b_{p,i}:\mu_{p,i}=m\}Bm​={bp,i​:μp,i​=m}, and switching from bbb to b′b'b′ costs δb,b′≥0\delta_{b,b'}\ge 0δb,b′​≥0. Flows are continuous: a machine processing a nonempty buffer bp,ib_{p,i}bp,i​ drains it at rate 1/τp,i1/\tau_{p,i}1/τp,i​, the output feeds bp,i+1b_{p,i+1}bp,i+1​ instantly, and a machine on an empty buffer passes its inflow through. Each machine works in runs: a set-up, then a processing phase on one buffer.

The load of machine mmm and the capacity condition are

ρm:=∑(p,i): μp,i=mdpτp,i<1(1≤m≤M).(1)\rho_m:=\sum_{(p,i):\,\mu_{p,i}=m}d_p\tau_{p,i}<1\qquad(1\le m\le M). \tag{1}ρm​:=(p,i):μp,i​=m∑​dp​τp,i​<1(1≤m≤M).(1)

The system is stable if sup⁡0≤t<∞xp,i(t)<∞\sup_{0\le t<\infty}x_{p,i}(t)<\inftysup0≤t<∞​xp,i​(t)<∞ for every buffer.

The supervisor picks γm\gamma_mγm​ with

γm(1−ρm)>∑b∈Bmmax⁡b′∈Bmδb′,b(24)\gamma_m(1-\rho_m)>\sum_{b\in B_m}\max_{b'\in B_m}\delta_{b',b} \tag{24}γm​(1−ρm​)>b∈Bm​∑​b′∈Bm​max​δb′,b​(24)

and thresholds zp,i≥0z_{p,i}\ge0zp,i​≥0. It truncates every processing run of bp,ib_{p,i}bp,i​ at γmdpτp,i\gamma_m d_p\tau_{p,i}γm​dp​τp,i​; it keeps a first-come first-served queue QmQ_mQm​ of the buffers that are not being processed and whose level exceeds zp,iz_{p,i}zp,i​; when a run ends and Qm≠∅Q_m\ne\emptysetQm​=∅, the head of QmQ_mQm​ is processed next, for exactly γmdpτp,i\gamma_m d_p\tau_{p,i}γm​dp​τp,i​ unless it clears earlier. When QmQ_mQm​ is empty the underlying policy is free. Write ζm:=γm(1−ρm)−∑b∈Bmmax⁡b′∈Bmδb′,b>0\zeta_m:=\gamma_m(1-\rho_m)-\sum_{b\in B_m}\max_{b'\in B_m}\delta_{b',b}>0ζm​:=γm​(1−ρm​)−∑b∈Bm​​maxb′∈Bm​​δb′,b​>0 (26) and βp,i(t):=∑j≤iτp,ixp,j(t)\beta_{p,i}(t):=\sum_{j\le i}\tau_{p,i}x_{p,j}(t)βp,i​(t):=∑j≤i​τp,i​xp,j​(t), the backlog of part type ppp for machine μp,i\mu_{p,i}μp,i​.

Formalization targets

Goal: Theorem 2

Under (1), (24) and z≥0z\ge 0z≥0, every supervised trajectory, from every initial state, satisfies

sup⁡0≤t<∞xp,i(t)<+∞for all p,i.\sup_{0\le t<\infty}x_{p,i}(t)<+\infty\qquad\text{for all }p,i.0≤t<∞sup​xp,i​(t)<+∞for all p,i.

The bound is allowed to depend on the trajectory; no uniformity in the initial state is claimed.

Milestones: Lemma 1

  1. A buffer that enters QmQ_mQm​ at tint_{\rm in}tin​ completes its next run by tin+γm−ζmt_{\rm in}+\gamma_m-\zeta_mtin​+γm​−ζm​ (25).
  2. If it enters QmQ_mQm​ with xp,i(tin)≥γmdpx_{p,i}(t_{\rm in})\ge\gamma_m d_pxp,i​(tin​)≥γm​dp​, that run lowers the backlog: βp,i(tcomplete)≤βp,i(tin)−ζmdpτp,i\beta_{p,i}(t_{\rm complete})\le\beta_{p,i}(t_{\rm in})-\zeta_m d_p\tau_{p,i}βp,i​(tcomplete​)≤βp,i​(tin​)−ζm​dp​τp,i​.
  3. A buffer that enters QmQ_mQm​ at tint_{\rm in}tin​ and stays above max⁡(γmdp,zp,i)\max(\gamma_md_p,z_{p,i})max(γm​dp​,zp,i​) (strictly above zp,iz_{p,i}zp,i​ after tint_{\rm in}tin​) up to t′t't′ has t′−tin≤(1+βp,i(tin)/(ζmdpτp,i))(γm−ζm)t'-t_{\rm in}\le(1+\beta_{p,i}(t_{\rm in})/(\zeta_md_p\tau_{p,i}))(\gamma_m-\zeta_m)t′−tin​≤(1+βp,i​(tin​)/(ζm​dp​τp,i​))(γm​−ζm​).
  4. Any interval on which xp,i≥gp,i:=max⁡(γmdp,zp,i)+γmdpx_{p,i}\ge g_{p,i}:=\max(\gamma_md_p,z_{p,i})+\gamma_md_pxp,i​≥gp,i​:=max(γm​dp​,zp,i​)+γm​dp​ has length at most ap,i+cp,iβp,i(t)a_{p,i}+c_{p,i}\beta_{p,i}(t)ap,i​+cp,i​βp,i​(t).

Significance

The theorem separates two concerns of real-time scheduling. The underlying policy can be tuned for performance (low set-up overhead, short buffers) without any stability analysis; the supervisor guarantees stability under exactly the condition that is necessary for it. The mechanism is distributed: each machine uses only its own buffer levels. With z=0z=0z=0 it enforces FCFS with truncated runs; with large zzz and γ\gammaγ it never intervenes on a policy that is already stable, so the degree of intervention is tunable. Combined with the §III instability examples, it shows that instability of clearing policies is a design defect that a local safeguard removes.

The result is proved in the paper; to our knowledge it has no machine-checked proof. This mission produces a formal model of continuous-flow manufacturing systems with set-up times and runs, a formal definition of the supervisor, and the four parts of Lemma 1 as reusable statements about it. Part 3) is stated with a corrected hypothesis (see Formalization scope).

Difficulty

The underlying policy is arbitrary, so no structure of the trajectory between interventions can be used: the policy may idle on empty buffers, switch at will, and re-select a buffer as soon as its run is truncated. The natural approach of bounding the total work at a machine fails, because work arrives at machine mmm from upstream machines whose behaviour depends on mmm itself through re-entrant routes, so a machine-by-machine argument is circular. A further difficulty is that the supervisor acts only on buffers above their thresholds, so a buffer can be ignored for as long as it sits at or below zp,iz_{p,i}zp,i​; any bound has to account for the time spent below the threshold and for repeated re-entries into QmQ_mQm​, with a set-up paid at each.

Formalization scope

  • Model. Part types Fin P, machines Fin M, buffers Σ p, Fin (n p); paper index iii is Lean index i−1i-1i−1. Time is real with t≥0t\ge0t≥0. Set-up times satisfy δb,b=0\delta_{b,b}=0δb,b​=0: a set-up is paid only on a switch. No transport delays or assembly, as in the paper.
  • Runs. Each machine is always in a run (no idling outside runs); a run is never cut during its set-up; run starts do not accumulate; zero-length runs are allowed. Processing is at rate at most 1/τb1/\tau_b1/τb​ and only in a processing phase of bbb, and at exactly 1/τb1/\tau_b1/τb​ while bbb is nonempty.
  • Queue. Membership of QmQ_mQm​ is determined by the trajectory: not on the current run and level strictly above zbz_bzb​. The FCFS key is the start of the current sojourn; ties, including the initial queue at time 000, are broken arbitrarily, so every initial queue order is covered. A buffer whose run just ended is in QmQ_mQm​ at that instant if its level exceeds zbz_bzb​.
  • Lemma 1. Parts 1)–3) assume, as the page does, that the buffer enters QmQ_mQm​ at tint_{\rm in}tin​. Part 3) adds xp,i>zp,ix_{p,i}>z_{p,i}xp,i​>zp,i​ on (tin,t′](t_{\rm in},t'](tin​,t′]: with the printed non-strict hypothesis the buffer can sit at exactly zp,iz_{p,i}zp,i​, never be re-queued, and wait arbitrarily long. In 4), cp,ic_{p,i}cp,i​ is (γm−ζm)/(ζmdpτp,i)(\gamma_m-\zeta_m)/(\zeta_md_p\tau_{p,i})(γm​−ζm​)/(ζm​dp​τp,i​).
  • Ruled out. The base policy is not restricted to clearing, CAF or any fixed rule, the system is not restricted to few machines or acyclic routes, and the hypothesis of the goal is (24), not ζm>0\zeta_m>0ζm​>0. A non-vacuity witness (one machine, one buffer) shows the class of supervised trajectories is nonempty.
  • Reusable. The trajectory model (runs, set-ups, processing law) is the same as in the other missions of this series and applies to any distributed scheduling policy with set-ups.

Contributions welcome: proofs of the Lemma 1 parts, and lemmas on the model (Lipschitz continuity of levels, monotonicity of a buffer's level while it is not processed).

Selected references

  • P. R. Kumar and T. I. Seidman, Dynamic instabilities and stabilization methods in distributed real-time scheduling of manufacturing systems, IEEE Trans. Automat. Control 35(3), 289–298, 1990. https://doi.org/10.1109/9.50339
  • J. R. Perkins and P. R. Kumar, Stable, distributed, real-time scheduling of flexible manufacturing/assembly/disassembly systems, IEEE Trans. Automat. Control 34(2), 139–148, 1989. https://doi.org/10.1109/9.21085
8 thms1 active userReviewed
Convex OptimizationProbability·Captain: mikedeng1

Convex Duality in Constrained Portfolio Optimization II: The Dual Problem Attains Its Infimum, So an Optimal Constrained Portfolio–Consumption Pair Exists for Every Initial CapitalResearch Paper

Motivation

Portfolio decisions in continuous time must respect both market uncertainty and investment restrictions. A ban on short sales, for example, restricts the vector of wealth fractions a trader may hold at every instant. The corresponding optimal consumption and investment problem is harder than its unrestricted counterpart because a candidate portfolio obtained from the usual pricing equations may violate the constraint. Cvitanić and Karatzas introduced auxiliary markets indexed by a process and used a dual optimization problem to establish existence of an optimal constrained policy in their 1992 paper. This mission formalizes the paper's existence theorem, Theorem 13.1, together with the results in Sections 12–13 that specify its dual target.

Setting

Fix a finite horizon T>0T>0T>0 and a complete probability space carrying a standard ddd-dimensional Brownian motion WWW. Information at time ttt is the probability augmentation of the filtration generated by WWW up to ttt. A bond earns short rate rtr_trt​; ddd stocks have appreciation vector btb_tbt​ and volatility matrix σt\sigma_tσt​. The market assumptions require progressively measurable coefficients, a uniform lower bound on rrr, uniform nondegeneracy of σσT\sigma\sigma^{\mathsf T}σσT, finite expected interest-rate integral, and finite energy of the market price of risk θ=σ−1(b−r1)\theta=\sigma^{-1}(b-r\mathbf1)θ=σ−1(b−r1) §2.

A portfolio πt\pi_tπt​ specifies fractions of wealth held in the stocks, while ct≥0c_t\geq0ct​≥0 is consumption and XtX_tXt​ is wealth. The feasible portfolios lie in a fixed nonempty closed convex set K⊆RdK\subseteq\mathbb R^dK⊆Rd. Its support function is δK(v)=sup⁡π∈K(−π⋅v)\delta_K(v)=\sup_{\pi\in K}(-\pi\cdot v)δK​(v)=supπ∈K​(−π⋅v), which may equal +∞+\infty+∞. The process ν\nuν indexing an auxiliary market belongs to D\mathcal DD when it has finite expected quadratic energy and finite expected integrated support value. Its deflator HνH_\nuHν​ combines an interest-rate discount with a Brownian exponential. The class D′\mathcal D'D′ consists of those ν∈D\nu\in\mathcal Dν∈D for which the budget map Xν(y)\mathcal X_\nu(y)Xν​(y) is finite for every y>0y>0y>0 §§4, 8.

The running utility U1(t,c)U_1(t,c)U1​(t,c) and terminal utility U2(XT)U_2(X_T)U2​(XT​) are strictly increasing and strictly concave for positive arguments. An admissible constrained policy has nonnegative wealth, finite expected negative utility, and πt∈K\pi_t\in Kπt​∈K for Lebesgue-time times probability almost every (t,ω)(t,\omega)(t,ω). The primal value V(x)V(x)V(x) is the supremum of its expected utility over all such policies with initial capital x>0x>0x>0. The dual value V~(y)\widetilde V(y)V(y) is the infimum, over ν∈D\nu\in\mathcal Dν∈D, of expected conjugate utility evaluated at yHνyH_\nuyHν​ §§5–6, 12.

Formalization targets

Dual attainment

The first conclusion of Theorem 13.1 is the paper's condition (12.9):

∀y>0∃λy∈D′V~(y)=J~(y;λy).\forall y>0\quad\exists\lambda_y\in\mathcal D'\quad\widetilde V(y)=\widetilde J(y;\lambda_y).∀y>0∃λy​∈D′V(y)=J(y;λy​).

Thus the infimum is attained by a drift with a finite budget map. It is a conclusion of this mission, even though earlier Section 12 results assume it. The milestones include weak duality (12.8), the dual representation of Proposition 12.1, the capital-matching result of Proposition 12.2, and the analytic properties of the extended dual functional in Proposition 13.2 pp. 792–795.

An optimal constrained policy for every capital

The theorem's second conclusion is

∀x>0∃(π^,c^,X^)∈A′(x)∀(π,c,X)∈A′(x),J(π,c,X)≤J(π^,c^,X^).\forall x>0\quad\exists (\widehat\pi,\widehat c,\widehat X)\in\mathcal A'(x)\quad\forall(\pi,c,X)\in\mathcal A'(x),\quad J(\pi,c,X)\leq J(\widehat\pi,\widehat c,\widehat X).∀x>0∃(π,c,X)∈A′(x)∀(π,c,X)∈A′(x),J(π,c,X)≤J(π,c,X).

Here A′(x)\mathcal A'(x)A′(x) is the constrained admissible class. Theorem 12.4 establishes this conclusion when dual attainment is assumed; Theorem 13.1 provides that assumption under the paper's stated utility and dual-finiteness conditions p. 794.

Significance

The result supplies an optimizer, rather than only a bound on the best attainable utility. It also identifies a minimizing auxiliary market for every positive dual parameter, making the dual description usable at a specified initial capital. The dual representation links the primal value to a convex function that can be studied without choosing a constrained policy first §§12–13.

The theorem is proved in the paper; the remaining work here is a machine-checked development of its definitions, hypotheses, and existence argument. The mission also produces reusable definitions of an almost-surely square-integrable Brownian integral relation, extended-real utility expectations, an extended support function, and constrained wealth classes. The Brownian state space and predictable step-sum substrate credit the published Ethier–Kurtz formalizations. The paper refers some analytic steps to earlier works instead of reproducing full proofs, including Lemma 12.3 and a final finiteness argument pp. 793–796.

Difficulty

Weak duality alone only bounds the constrained value from above. It does not supply a minimizer of J~(y;ν)\widetilde J(y;\nu)J(y;ν), and an arbitrary minimizing auxiliary process need not belong to D′\mathcal D'D′. The dual functional must retain meaningful infinite values on the full finite-energy process space H\mathcal HH; replacing them with total-operation defaults can turn the needed coercivity and lower-semicontinuity statements into different claims. Even after dual attainment, the minimizing parameter for a prescribed capital must match the budget map Xλy(y)\mathcal X_{\lambda_y}(y)Xλy​​(y) §§12–13. These are the precise gaps between a numerical bound and the asserted optimal policy.

Formalization scope

Lean uses Rd\mathbb R^dRd with its Euclidean norm, a finite positive horizon, a complete probability measure, and the augmented Brownian filtration. Processes are functions of time and sample point; ℓ⊗P\ell\otimes Pℓ⊗P almost-everywhere restrictions on portfolios and auxiliary drifts are distinct from pathwise PPP-almost-sure statements. A policy is represented by a triple (π,c,X)(\pi,c,X)(π,c,X) whose wealth process satisfies the integral equation, matching the paper's pair together with its unique wealth solution. The integral operator is bound to the local Itô construction by predictable step approximations; it is not a free function. Integrands must be in its almost-sure square-integrable domain.

Support values, utility at zero, expected utility, and value functions use extended reals. The extension U(0)U(0)U(0) is the right limit U(0+)U(0+)U(0+); an extended-real supremum defines conjugate utility where zero arguments arise. The inverse marginal is a positive-argument inverse of U′U'U′. The minimization in V~\widetilde VV ranges over D\mathcal DD, while (12.9) asks for a minimizer in D′\mathcal D'D′. Its witnesses λy\lambda_yλy​ remain explicit choices in statements involving Xλy\mathcal X_{\lambda_y}Xλy​​; no default-valued inverse Yν\mathcal Y_\nuYν​ is introduced. The functional J~y\widetilde J_yJy​ of (13.3) is defined on H\mathcal HH, uses the paper's formula on G\mathcal GG, and is +∞+\infty+∞ off G\mathcal GG. On D\mathcal DD it agrees almost everywhere with the original dual objective, an equality requiring a formal lemma. Assumption 6.2 and conditions (5.8), (8.25), (12.2), (12.3), and (12.11) are explicit. Their quantifiers cover both utilities and every time in [0,T][0,T][0,T] where stated. The mission rules out a vacuous dual-attainment hypothesis, a zero default for an unbounded support supremum, and an unconstrained stochastic-integral operator. Contributions proving the source milestones and the analytic lemmas they need are in scope.

Selected references

  • Jakša Cvitanić and Ioannis Karatzas, Convex Duality in Constrained Portfolio Optimization, The Annals of Applied Probability 2(4), 1992, 767–818. DOI: 10.1214/aoap/1177005576.
15 thms1 active userReviewed
Dynamical SystemsOperations ResearchOptimization·Captain: mikedeng1

Homogeneous Approximation, Recursive Observer Design, and Output Feedback: Global Asymptotic Stabilization of a Chain of Integrators by a Homogeneous-in-the-Bi-Limit Output FeedbackResearch Paper

Motivation

Many nonlinear control systems behave like a chain of integrators, x˙1=x2,…,x˙n=u\dot x_1=x_2,\dots,\dot x_n=ux˙1​=x2​,…,x˙n​=u, with additional terms that are small either near the origin or far from it. Designs based on weighted homogeneity handle such systems by making the closed loop invariant under a dilation, which gives robustness to perturbations that are dominated by the homogeneous part (Rosier, Homogeneous Lyapunov function for homogeneous continuous vector field, Systems & Control Letters, 1992, doi:10.1016/0167-6911(92)90078-7). A single homogeneous approximation, however, describes the system only at one scale. A perturbation that is negligible near the origin may dominate at infinity, and a design tuned to the origin can then fail globally.

Andrieu, Praly and Astolfi (arXiv:0903.0298v1; SIAM J. Control Optim., 2008, doi:10.1137/060675861) introduce homogeneity in the bi-limit: a function or vector field has one homogeneous approximation near the origin and another, possibly with different weights and degree, at infinity. They develop the basic calculus of this notion, a converse Lyapunov theorem for it, a recursive observer and a recursive state feedback for the chain of integrators, and combine them into a global output feedback. This mission formalizes that output-feedback result and the chain of results it rests on.

Setting

For a weight r=(r1,…,rn)r=(r_1,\dots,r_n)r=(r1​,…,rn​) with all ri>0r_i>0ri​>0 and λ>0\lambda>0λ>0, the dilation is λr⋄x=(λr1x1,…,λrnxn)\lambda^r\diamond x=(\lambda^{r_1}x_1,\dots,\lambda^{r_n}x_n)λr⋄x=(λr1​x1​,…,λrn​xn​). A continuous function ϕ:Rn→R\phi:\mathbb R^n\to\mathbb Rϕ:Rn→R is homogeneous in the 0-limit with triple (r0,d0,ϕ0)(r_0,d_0,\phi_0)(r0​,d0​,ϕ0​), degree d0≥0d_0\ge0d0​≥0, if ϕ0\phi_0ϕ0​ is continuous and not identically zero and, for every compact C⊆Rn∖{0}C\subseteq\mathbb R^n\setminus\{0\}C⊆Rn∖{0} and every ε>0\varepsilon>0ε>0, there is λ0>0\lambda_0>0λ0​>0 such that

max⁡x∈C∣ϕ(λr0⋄x)λd0−ϕ0(x)∣≤εfor all λ∈(0,λ0].\max_{x\in C}\left|\frac{\phi(\lambda^{r_0}\diamond x)}{\lambda^{d_0}}-\phi_0(x)\right|\le\varepsilon\qquad\text{for all }\lambda\in(0,\lambda_0].x∈Cmax​​λd0​ϕ(λr0​⋄x)​−ϕ0​(x)​≤εfor all λ∈(0,λ0​].

Homogeneity in the ∞-limit with triple (r∞,d∞,ϕ∞)(r_\infty,d_\infty,\phi_\infty)(r∞​,d∞​,ϕ∞​) is the same statement for all λ≥λ∞\lambda\ge\lambda_\inftyλ≥λ∞​. A vector field f=(f1,…,fn)f=(f_1,\dots,f_n)f=(f1​,…,fn​) is homogeneous with triple (r,d,f0)(r,\mathfrak d,f_0)(r,d,f0​), d∈R\mathfrak d\in\mathbb Rd∈R, when each fif_ifi​ is homogeneous with triple (r,d+ri,f0,i)(r,\mathfrak d+r_i,f_{0,i})(r,d+ri​,f0,i​) and d+ri≥0\mathfrak d+r_i\ge0d+ri​≥0. Bi-limit means both at once.

For the chain of integrators, Snx=(x2,…,xn,0)TS_n x=(x_2,\dots,x_n,0)^TSn​x=(x2​,…,xn​,0)T and Bn=(0,…,0,1)TB_n=(0,\dots,0,1)^TBn​=(0,…,0,1)T. Given degrees d0,d∞∈(−1,1n−1)\mathfrak d_0,\mathfrak d_\infty\in(-1,\frac1{n-1})d0​,d∞​∈(−1,n−11​), the weights are

r0,i=1−d0(n−i),r∞,i=1−d∞(n−i),i=1,…,n.r_{0,i}=1-\mathfrak d_0(n-i),\qquad r_{\infty,i}=1-\mathfrak d_\infty(n-i),\qquad i=1,\dots,n .r0,i​=1−d0​(n−i),r∞,i​=1−d∞​(n−i),i=1,…,n.

The output feedback studied is

x˙=Snx+Bnu,y=x1,X^˙n=L(SnX^n+Bnϕn(X^n)+K1(x1−x^1)),u=Lnϕn(X^n),\dot x=S_nx+B_nu,\quad y=x_1,\qquad \dot{\hat{\mathfrak X}}_n=L\bigl(S_n\hat{\mathfrak X}_n+B_n\phi_n(\hat{\mathfrak X}_n)+K_1(x_1-\hat x_1)\bigr),\quad u=L^n\phi_n(\hat{\mathfrak X}_n),x˙=Sn​x+Bn​u,y=x1​,X^˙n​=L(Sn​X^n​+Bn​ϕn​(X^n​)+K1​(x1​−x^1​)),u=Lnϕn​(X^n​),

with a gain L>0L>0L>0, a state feedback ϕn:Rn→R\phi_n:\mathbb R^n\to\mathbb Rϕn​:Rn→R and an output-injection vector field K1:Rn→RnK_1:\mathbb R^n\to\mathbb R^nK1​:Rn→Rn, where K1(s)K_1(s)K1​(s) means K1(s,0,…,0)K_1(s,0,\dots,0)K1​(s,0,…,0). Its homogeneous approximations are the same closed loop with (ϕn,0,K1,0)(\phi_{n,0},K_{1,0})(ϕn,0​,K1,0​) and with (ϕn,∞,K1,∞)(\phi_{n,\infty},K_{1,\infty})(ϕn,∞​,K1,∞​) in place of (ϕn,K1)(\phi_n,K_1)(ϕn​,K1​).

Formalization targets

Goal: Theorem 5.1

For n≥2n\ge2n≥2 and d0,d∞∈(−1,1n−1)\mathfrak d_0,\mathfrak d_\infty\in(-1,\frac1{n-1})d0​,d∞​∈(−1,n−11​) there exist ϕn\phi_nϕn​, homogeneous in the bi-limit with triples (r0,1+d0,ϕn,0)(r_0,1+\mathfrak d_0,\phi_{n,0})(r0​,1+d0​,ϕn,0​) and (r∞,1+d∞,ϕn,∞)(r_\infty,1+\mathfrak d_\infty,\phi_{n,\infty})(r∞​,1+d∞​,ϕn,∞​), and K1K_1K1​, homogeneous in the bi-limit with triples (r0,d0,K1,0)(r_0,\mathfrak d_0,K_{1,0})(r0​,d0​,K1,0​) and (r∞,d∞,K1,∞)(r_\infty,\mathfrak d_\infty,K_{1,\infty})(r∞​,d∞​,K1,∞​), such that

∀L>0:0∈R2n is globally asymptotically stable for the closed loop and for both of its homogeneous approximations.\forall L>0:\quad 0\in\mathbb R^{2n}\text{ is globally asymptotically stable for the closed loop and for both of its homogeneous approximations.}∀L>0:0∈R2n is globally asymptotically stable for the closed loop and for both of its homogeneous approximations.

The pair (ϕn,K1)(\phi_n,K_1)(ϕn​,K1​) is fixed before LLL. No constant appears in the goal.

Milestones

  1. Proposition 2.10 (composition) and Proposition 2.12 (integration along a coordinate) preserve homogeneity in the limit.
  2. Lemma 2.13: for homogeneous η\etaη and γ≥0\gamma\ge0γ≥0 with η<0\eta<0η<0 where γ=0\gamma=0γ=0, η−cγ<0\eta-c\gamma<0η−cγ<0 off the origin for all large ccc, simultaneously for both approximations.
  3. Theorem 2.20: a converse Lyapunov theorem, giving a C1C^1C1 proper Lyapunov function whose gradient is homogeneous in the bi-limit.
  4. Theorem 3.1 and display (3.12): the recursive observer, an output injection K1K_1K1​ making E˙=SnE+K1(e1)\dot E=S_nE+K_1(e_1)E˙=Sn​E+K1​(e1​) and its approximations globally asymptotically stable.
  5. Theorem 4.1 and display (4.9): the recursive state feedback, a ϕn\phi_nϕn​ making X˙=SnX+Bnϕn(X)\dot{\mathfrak X}=S_n\mathfrak X+B_n\phi_n(\mathfrak X)X˙=Sn​X+Bn​ϕn​(X) and its approximations globally asymptotically stable.

Significance

The theorem gives a single dynamic output feedback for the chain of integrators that is homogeneous with prescribed degrees near the origin and at infinity, and that stabilizes globally for every gain L>0L>0L>0. Because the degrees at the two ends are independent, the same design can be matched to perturbations of different orders at small and large amplitudes; the paper derives from it output-feedback stabilizers for systems in feedback and feedforward form (Corollaries 5.2 and 5.3), which are outside this mission. The converse Lyapunov theorem (Theorem 2.20) and the key lemma (Lemma 2.13) are general tools for any vector field homogeneous in the bi-limit.

The results are proved in the paper; none of them, nor the notion of homogeneity in the bi-limit, has a machine-checked proof. The platform has a definition of global asymptotic stability for continuous vector fields (from the series on Chitour, Ushirobira, Efimov and Perruquetti's prescribed-time stabilization) and Mathlib has the needed analysis, but there is no converse Lyapunov theorem and no theory of weighted homogeneous vector fields. A complete formalization would supply both.

Difficulty

Lyapunov arguments for homogeneous systems usually compare a function with its homogeneous approximation on the unit sphere and then scale. With homogeneity in the bi-limit the comparison holds only for small or for large dilation parameters, with no control at intermediate scales, and the two approximations have different weights, so no single dilation brings the whole space to a compact set. Each statement has to hold for the system and for both approximations at once. Theorem 2.20 additionally requires a converse Lyapunov theorem for continuous, non-Lipschitz vector fields whose solutions need not be unique, so a flow map is not available. Finally, the gain LLL in the goal is arbitrary: an argument that only works for LLL large enough proves a weaker statement.

Formalization scope

Points of Rn\mathbb R^nRn are functions Fin n → ℝ, with the paper's coordinate xix_ixi​ at index i−1i-1i−1; the closed loop lives on Fin (n + n) → ℝ with xxx first and X^n\hat{\mathfrak X}_nX^n​ second. Real powers are Real.rpow; the signed power is wr=sign⁡(w)∣w∣rw^r=\operatorname{sign}(w)|w|^rwr=sign(w)∣w∣r. Every clause of Definitions 2.1, 2.3 and 2.5 is kept: positive weights, nonnegative function degrees, continuity, approximating functions not identically zero, uniformity on compact subsets of Rn∖{0}\mathbb R^n\setminus\{0\}Rn∖{0}. Dropping any of them makes the goal weaker than the paper's.

Global asymptotic stability reuses the published ChitourPrescribedTime.FixedTime.GloballyAsymptoticallyStable on the Euclidean space, applied to the time-invariant field: the origin is an equilibrium, every initial state has a solution on [0,∞)[0,\infty)[0,∞), and stability and uniform attractivity hold for every solution. The mission adds that no solution escapes to infinity in finite time, so that every solution is covered; for continuous autonomous fields this is the textbook notion. Positive and negative definiteness, properness (V→∞V\to\inftyV→∞ along the cocompact filter), C1C^1C1 and partial derivatives (Fréchet derivative on a basis vector) are defined in the mission's definition files.

Corrections and readings, each disclosed in the item concerned:

  • Proposition 2.10 is false as printed. The composite approximation ζ0∘ϕ0\zeta_0\circ\phi_0ζ0​∘ϕ0​ can vanish identically, and in the ∞-limit a degree-0 outer function fails. Both extra hypotheses are added.
  • (5.2) prints K1(x1−x^1)K_1(x_1-\hat x_1)K1​(x1​−x^1​) while (3.3) and (5.9) use x^1−x1\hat x_1-x_1x^1​−x1​. The goal keeps the printed sign; since K1K_1K1​ is existential, the two readings are equivalent.
  • In Theorem 3.1 the hypothesis "GAS for these systems" covers (3.5) and both approximations, as the proof uses. In Theorem 4.1 the implicit ψi0,ψi∞\psi_{i0},\psi_{i\infty}ψi0​,ψi∞​ are existential C1C^1C1 functions, and αi+1>1\alpha_{i+1}>1αi+1​>1 is kept as printed. (4.4) and (4.9) lack the time-derivative dots.

A formalization in which the closed loop is replaced by its linearization, the homogeneity predicate is weakened to pointwise convergence, or the quantifier on LLL is moved before ϕn\phi_nϕn​ and K1K_1K1​, proves a different statement and does not close the goal. Contributions welcome: a library of weighted dilations and homogeneous functions, the converse Lyapunov theorem, and proofs of the milestones in any order.

Selected references

  • V. Andrieu, L. Praly, A. Astolfi, Homogeneous Approximation, Recursive Observer Design, and Output Feedback, arXiv:0903.0298v1, 2009 (SIAM J. Control Optim. 47(4), 2008). https://arxiv.org/abs/0903.0298
  • L. Rosier, Homogeneous Lyapunov function for homogeneous continuous vector field, Systems & Control Letters 19(6), 1992. https://doi.org/10.1016/0167-6911(92)90078-7
  • A. Bacciotti, L. Rosier, Liapunov Functions and Stability in Control Theory, Springer, 2nd ed., 2005. https://doi.org/10.1007/b139028
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Dynamical SystemsOperations Research·Captain: mikedeng1

Dynamic Instabilities and Stabilization Methods in Distributed Real-Time Scheduling of Manufacturing Systems 1: Clearing Policies Are Unstable on a Re-Entrant Two-Machine Line, Even Without Set-UpsResearch Paper

Motivation

A flexible manufacturing system is a set of machines through which parts of several types travel along fixed routes; each machine serves several buffers and must pay a set-up time whenever it switches from one buffer to another. Real-time scheduling decides, as the system evolves, which buffer each machine works on. Perkins and Kumar (IEEE Trans. Automat. Control 34, 1989) introduced simple distributed policies for this problem, of which the most natural is the clearing policy: a machine keeps working on a buffer until it is empty, and only then switches. They proved that every clear-a-fraction policy, a subclass of clearing policies, keeps every buffer bounded on acyclic systems whenever each machine has spare capacity, and left open whether clear-a-fraction policies stabilize all systems in which material flows around cycles.

Kumar and Seidman (IEEE Trans. Automat. Control 35(3), 1990, doi:10.1109/9.50339) answered no. Their Example 1 is a single part type that visits two machines in the order 1, 2, 2, 1. Every machine has spare capacity, yet under the clearing policy the buffer levels grow without bound, and they do so even when all set-up times are zero, so the instability comes from machines starving each other rather than from time lost to set-ups. Until then, instability had been suspected to require positive set-up times. Shortly afterwards Lu and Kumar exhibited instability of a static buffer-priority rule in a re-entrant network (IEEE Trans. Automat. Control 36, 1991); together these examples started the study of stability of multiclass queueing networks.

Setting

A manufacturing system has part types ppp arriving at rates dp>0d_p > 0dp​>0. Parts of type ppp follow a route of length npn_pnp​: their iii-th operation is at machine μp,i\mu_{p,i}μp,i​, and they wait for it in buffer bp,ib_{p,i}bp,i​, where each part needs processing time τp,i>0\tau_{p,i} > 0τp,i​>0. Machine mmm serves the buffers Bm={b:μb=m}B_m = \{b : \mu_b = m\}Bm​={b:μb​=m}, and switching from bbb to b′b'b′ costs set-up time δb,b′≥0\delta_{b,b'} \ge 0δb,b′​≥0.

Flows are continuous (fluid). The level of buffer bbb at time t≥0t \ge 0t≥0 is xb(t)=xb(0)+ub(t)−yb(t)≥0x_b(t) = x_b(0) + u_b(t) - y_b(t) \ge 0xb​(t)=xb​(0)+ub​(t)−yb​(t)≥0, where yb(t)y_b(t)yb​(t) is its cumulative output and ub(t)u_b(t)ub​(t) its cumulative input: dptd_p tdp​t for the first buffer of a route, and the output of the preceding buffer otherwise. Each machine works in runs: run kkk is a set-up phase of length δβk−1,βk\delta_{\beta_{k-1},\beta_k}δβk−1​,βk​​ followed by a processing phase on buffer βk\beta_kβk​, during which the buffer is drained at rate 1/τb1/\tau_b1/τb​ while it is nonempty and passed through at its inflow rate when it is empty. The system is stable if sup⁡0≤t<∞xb(t)<∞\sup_{0 \le t < \infty} x_b(t) < \inftysup0≤t<∞​xb​(t)<∞ for every buffer.

A clearing policy (Definition 1) is one in which a machine processing bbb continues until the first time that bbb is empty and some other buffer of the same machine is nonempty, and then commences a set-up for one of the nonempty buffers.

Example 1. One part type arrives at rate d=1d = 1d=1 and visits machine 1, machine 2, machine 2 and machine 1; its buffers are 1,2,3,41, 2, 3, 41,2,3,4, so B1={1,4}B_1 = \{1, 4\}B1​={1,4} and B2={2,3}B_2 = \{2, 3\}B2​={2,3}. Processing times are τ1,…,τ4>0\tau_1, \dots, \tau_4 > 0τ1​,…,τ4​>0, and δk\delta_kδk​ is the time to set up to buffer kkk. The parameters satisfy the critical condition and the capacity condition

τ2+τ4>1,τ1+τ4<1,τ2+τ3<1.(3–5)\tau_2 + \tau_4 > 1, \qquad \tau_1 + \tau_4 < 1, \qquad \tau_2 + \tau_3 < 1. \tag{3–5}τ2​+τ4​>1,τ1​+τ4​<1,τ2​+τ3​<1.(3–5)

The initial state is x(0)=(ξ,0,0,0)x(0) = (\xi, 0, 0, 0)x(0)=(ξ,0,0,0), with machine 1 set up for buffer 4 and machine 2 set up for buffer 3. Write

λ=τ41−τ2>1,α=(τ4+1)(δ1+δ2)1−τ2+δ3(τ4+1)+δ4,β=τ4(δ1+δ2)1−τ2+τ4δ3+δ4.\lambda = \frac{\tau_4}{1-\tau_2} > 1, \quad \alpha = \frac{(\tau_4+1)(\delta_1+\delta_2)}{1-\tau_2} + \delta_3(\tau_4+1) + \delta_4, \quad \beta = \frac{\tau_4(\delta_1+\delta_2)}{1-\tau_2} + \tau_4\delta_3 + \delta_4.λ=1−τ2​τ4​​>1,α=1−τ2​(τ4​+1)(δ1​+δ2​)​+δ3​(τ4​+1)+δ4​,β=1−τ2​τ4​(δ1​+δ2​)​+τ4​δ3​+δ4​.

Formalization targets

Goal: Example 1, both cases

Assume (3)–(5).

  1. If δ1,…,δ4>0\delta_1, \dots, \delta_4 > 0δ1​,…,δ4​>0, there is ξ0\xi_0ξ0​ such that for every ξ≥ξ0\xi \ge \xi_0ξ≥ξ0​ (ξ>0\xi > 0ξ>0) a clearing trajectory from (ξ,0,0,0)(\xi, 0, 0, 0)(ξ,0,0,0) exists, and every such trajectory has
sup⁡0≤t<∞x1(t)=+∞.\sup_{0 \le t < \infty} x_1(t) = +\infty.0≤t<∞sup​x1​(t)=+∞.
  1. If δ1=⋯=δ4=0\delta_1 = \dots = \delta_4 = 0δ1​=⋯=δ4​=0, the same holds for every ξ>0\xi > 0ξ>0.

Milestone: the Case 1 cycle map

For ξ\xiξ large enough, every clearing trajectory from (ξ,0,0,0)(\xi, 0, 0, 0)(ξ,0,0,0) reaches, at T1=(λ+τ2/(1−τ2))ξ+αT_1 = (\lambda + \tau_2/(1-\tau_2))\xi + \alphaT1​=(λ+τ2​/(1−τ2​))ξ+α,

x(T1)=(λξ+β,0,0,0),x(T_1) = (\lambda\xi + \beta, 0, 0, 0),x(T1​)=(λξ+β,0,0,0),

with machines 1 and 2 again set up for buffers 4 and 3.

Milestone: the Case 2 magnification

With zero set-up times and any ξ>0\xi > 0ξ>0, every clearing trajectory reaches, at t5=(τ2+τ4)ξ/(1−τ2)t_5 = (\tau_2+\tau_4)\xi/(1-\tau_2)t5​=(τ2​+τ4​)ξ/(1−τ2​),

x(t5)=(λξ,0,0,0),x(t_5) = (\lambda\xi, 0, 0, 0),x(t5​)=(λξ,0,0,0),

with machines 1 and 2 again set up for buffers 4 and 3.

Significance

The example shows that the condition ρm<1\rho_m < 1ρm​<1 on every machine, which is necessary for stability and sufficient for the existence of some stabilizing policy, does not make natural distributed policies stable once material flows around a cycle. The throughput of the line falls to 1/(τ2+τ4)<11/(\tau_2+\tau_4) < 11/(τ2​+τ4​)<1 part per unit time although each machine could handle the demand. This motivates the paper's two positive results: sufficient conditions under which clear-a-fraction policies are stable (Theorem 1), and a supervisory mechanism that stabilizes any policy (Theorem 2), which are the subjects of the other missions of this series. The example is also an early instance of the phenomenon later studied as instability of multiclass fluid networks under work-conserving policies.

The paper's argument is a stage-by-stage computation of piecewise linear trajectories. No machine-checked version of it exists. A formal proof has to make precise what the paper leaves to the reader: that the clearing rule determines the trajectory, that the stage formulas are what that trajectory does, and that the cycle can be restarted. The formal model of runs, set-ups and the clearing rule built here is the same as in the other missions of the series.

Difficulty

The arithmetic of each cycle is routine once the trajectory is known. The difficulty is in the universal quantifier: the claim covers every clearing trajectory, and the clearing rule is defined implicitly, through "the first time thereafter" at which a buffer is empty and another one is nonempty. At several switching instants the buffer a machine switches to is empty and only starts to fill at that instant, and with zero set-up times a machine may begin a run at an instant where the switching condition already holds. Showing that each switch happens exactly when the paper says, and that the fluid levels then follow the printed formulas (including the reduced rate of a machine working on an empty buffer), is a uniqueness argument for a hybrid system, not a simulation. The existence half asks for the converse: an explicit trajectory, defined for all time, with infinitely many runs whose start times tend to infinity.

Formalization scope

  • Time is real (t≥0t \ge 0t≥0); flows are fluid; there are no transport delays or assembly.
  • The system is a general structure (part types Fin P, machines Fin M, buffers ⟨p, i⟩ with i : Fin (n p), paper index iii = Lean index i+1i+1i+1), instantiated as Example 1 with d=1d = 1d=1, route (1,2,2,1)(1,2,2,1)(1,2,2,1), and δb,b′=δb′\delta_{b,b'} = \delta_{b'}δb,b′​=δb′​ for b≠b′b \ne b'b=b′; staying on a buffer costs nothing.
  • A trajectory is a schedule of runs per machine (possibly finitely many, the last lasting forever), with only finitely many run starts in any bounded interval. Processing obeys a rate cap (yby_byb​ grows at most at rate 1/τb1/\tau_b1/τb​, and only while machine μb\mu_bμb​ is in a processing phase of bbb) and runs at full rate while the buffer is nonempty.
  • In Definition 1, a target buffer counts as "nonempty" when it is demanding: positive level, or inflow starting at that instant. The no-early-exit condition is imposed on the open processing interval. Under the literal reading (positive level) or a closed interval, the paper's own trajectories are not clearing, and the goal would hold vacuously; the existence clause in the goal rules out that trivialization.
  • "Set up for buffer bbb at time TTT" means the run in force on (sk,sk+1](s_k, s_{k+1}](sk​,sk+1​].
  • Unboundedness is stated for buffer 1: for every CCC there is t≥0t \ge 0t≥0 with x1(t)>Cx_1(t) > Cx1​(t)>C; "ξ\xiξ large enough" is ∃ξ0,∀ξ≥ξ0\exists \xi_0, \forall \xi \ge \xi_0∃ξ0​,∀ξ≥ξ0​.

Useful contributions include lemmas about fluid trajectories that do not depend on the example (continuity of levels, the pass-through rate on an empty buffer, restarting a trajectory at a run boundary), which also serve the other missions of the series.

Selected references

  • P. R. Kumar and T. I. Seidman, Dynamic instabilities and stabilization methods in distributed real-time scheduling of manufacturing systems, IEEE Trans. Automat. Control 35(3), 289–298, 1990. https://doi.org/10.1109/9.50339
  • J. R. Perkins and P. R. Kumar, Stable, distributed, real-time scheduling of flexible manufacturing/assembly/disassembly systems, IEEE Trans. Automat. Control 34, 139–148, 1989 (reference [18] of the paper).
  • S. H. Lu and P. R. Kumar, Distributed scheduling based on due dates and buffer priorities, IEEE Trans. Automat. Control 36, 1991.
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Convex OptimizationProbability·Captain: mikedeng1

Convex Duality in Constrained Portfolio Optimization I: Financibility, Minimality, Dual Optimality and Parsimony of an Auxiliary Market Are Equivalent and Yield the Optimal Constrained PolicyResearch Paper

Motivation

An investor in a continuous-time market chooses, at every instant, how to split wealth between a bond and ddd stocks and how fast to consume, so as to maximize expected utility of consumption and terminal wealth. Without constraints on the portfolio, this problem was solved by the martingale method: Pliska (1986), Karatzas, Lehoczky and Shreve (1987) and Cox and Huang (1989) showed that in a complete market the optimal terminal wealth and consumption are explicit functions of a single state-price density, and the portfolio that finances them comes from the martingale representation theorem.

Real investors face constraints: no short selling, no borrowing, a cap on the fraction of wealth in a sector, an incomplete market in which some stocks cannot be traded at all. Each makes the market effectively incomplete, and the single state-price density no longer exists. Karatzas, Lehoczky, Shreve and Xu (1991) treated incompleteness, Xu (1990, thesis) short-selling prohibition, and He and Pearson (1991) short-sale constraints in a general setting. Cvitanić and Karatzas (1992) unified these cases: the portfolio must take values in an arbitrary nonempty closed convex set K⊂RdK\subset\mathbb R^dK⊂Rd, and the problem is embedded in a family of auxiliary unconstrained markets indexed by a dual process ν\nuν. This mission formalizes the paper's central characterization, Theorem 10.1, and the results its proof rests on.

Setting

A standard Brownian motion WWW in Rd\mathbb R^dRd lives on a complete probability space with its augmented filtration {Ft}\{\mathcal F_t\}{Ft​}, on a finite horizon [0,T][0,T][0,T]. The market M\mathcal MM has progressively measurable interest rate rrr, appreciation rates bbb and volatility matrix σ\sigmaσ, with r≥−ηr\ge-\etar≥−η, ξ∗σσ∗ξ≥ε∥ξ∥2\xi^*\sigma\sigma^*\xi\ge\varepsilon\|\xi\|^2ξ∗σσ∗ξ≥ε∥ξ∥2, E∫0Tr dt<∞E\int_0^Tr\,dt<\inftyE∫0T​rdt<∞, and a relative risk θ=σ−1(b−r1)\theta=\sigma^{-1}(b-r\mathbf 1)θ=σ−1(b−r1) with E∫0T∥θ∥2dt<∞E\int_0^T\|\theta\|^2dt<\inftyE∫0T​∥θ∥2dt<∞. The state-price density is H0=γ0Z0H_0=\gamma_0Z_0H0​=γ0​Z0​, with γ0(t)=e−∫0tr\gamma_0(t)=e^{-\int_0^tr}γ0​(t)=e−∫0t​r and Z0(t)=exp⁡(−∫0tθ∗dW−12∫0t∥θ∥2)Z_0(t)=\exp(-\int_0^t\theta^*dW-\frac12\int_0^t\|\theta\|^2)Z0​(t)=exp(−∫0t​θ∗dW−21​∫0t​∥θ∥2).

A portfolio π\piπ gives the proportions of wealth in the stocks, a consumption rate is c≥0c\ge0c≥0, and the wealth solves

dX=(rX−c) dt+Xπ∗σ (dW+θ dt),X(0)=x>0.dX=(rX-c)\,dt+X\pi^*\sigma\,(dW+\theta\,dt),\qquad X(0)=x>0.dX=(rX−c)dt+Xπ∗σ(dW+θdt),X(0)=x>0.

The pair is admissible, (π,c)∈A0(x)(\pi,c)\in\mathcal A_0(x)(π,c)∈A0​(x), if X≥0X\ge0X≥0. With utility functions U1(t,⋅)U_1(t,\cdot)U1​(t,⋅), U2U_2U2​ (strictly increasing, strictly concave, C1C^1C1, U′(0+)=∞U'(0+)=\inftyU′(0+)=∞, U′(∞)=0U'(\infty)=0U′(∞)=0), inverse marginals I1,I2I_1,I_2I1​,I2​ and conjugates U~1,U~2\tilde U_1,\tilde U_2U~1​,U~2​, the investor maximizes

J(x;π,c)=E∫0TU1(t,c(t)) dt+EU2(X(T))J(x;\pi,c)=E\int_0^TU_1(t,c(t))\,dt+EU_2(X(T))J(x;π,c)=E∫0T​U1​(t,c(t))dt+EU2​(X(T))

over A′(x)\mathcal A'(x)A′(x), the admissible pairs with integrable utility losses and π∈K\pi\in Kπ∈K almost everywhere. The value is V(x)V(x)V(x).

The support function δ(ν)=sup⁡π∈K(−π∗ν)∈R∪{+∞}\delta(\nu)=\sup_{\pi\in K}(-\pi^*\nu)\in\mathbb R\cup\{+\infty\}δ(ν)=supπ∈K​(−π∗ν)∈R∪{+∞} drives the duality. For ν\nuν in the class D\mathcal DD of square-integrable processes with E∫0Tδ(ν) dt<∞E\int_0^T\delta(\nu)\,dt<\inftyE∫0T​δ(ν)dt<∞, the auxiliary market Mν\mathcal M_\nuMν​ has interest rate r+δ(ν)r+\delta(\nu)r+δ(ν) and appreciation rates b+ν+δ(ν)1b+\nu+\delta(\nu)\mathbf 1b+ν+δ(ν)1, state-price density HνH_\nuHν​ and unconstrained value Vν(x)V_\nu(x)Vν​(x). For λ\lambdaλ in the subclass D′\mathcal D'D′ (where Xλ(y)=E[∫0THλI1(t,yHλ) dt+Hλ(T)I2(yHλ(T))]\mathcal X_\lambda(y)=E[\int_0^TH_\lambda I_1(t,yH_\lambda)\,dt+H_\lambda(T)I_2(yH_\lambda(T))]Xλ​(y)=E[∫0T​Hλ​I1​(t,yHλ​)dt+Hλ​(T)I2​(yHλ​(T))] is finite for all y>0y>0y>0), let y=Yλ(x)y=\mathcal Y_\lambda(x)y=Yλ​(x) solve Xλ(y)=x\mathcal X_\lambda(y)=xXλ​(y)=x. The Mλ\mathcal M_\lambdaMλ​-optimal consumption, terminal wealth and wealth are cλ=I1(t,yHλ)c_\lambda=I_1(t,yH_\lambda)cλ​=I1​(t,yHλ​), ξλ=I2(yHλ(T))\xi_\lambda=I_2(yH_\lambda(T))ξλ​=I2​(yHλ​(T)) and XλX_\lambdaXλ​.

Formalization targets

Goal: Theorem 10.1

Five conditions are considered for a capital x>0x>0x>0: (A) optimality of a pair (π^,c^)∈A′(x)(\hat\pi,\hat c)\in\mathcal A'(x)(π^,c^)∈A′(x), together with E[∫0Tc^U1′(t,c^) dt+X^(T)U2′(X^(T))]<∞E[\int_0^T\hat cU_1'(t,\hat c)\,dt+\hat X(T)U_2'(\hat X(T))]<\inftyE[∫0T​c^U1′​(t,c^)dt+X^(T)U2′​(X^(T))]<∞; and, for λ∈D′\lambda\in\mathcal D'λ∈D′, (B) financibility: some π^λ∈K\hat\pi_\lambda\in Kπ^λ​∈K with δ(λ)+π^λ∗λ=0\delta(\lambda)+\hat\pi_\lambda^*\lambda=0δ(λ)+π^λ∗​λ=0 finances (cλ,ξλ)(c_\lambda,\xi_\lambda)(cλ​,ξλ​) in M\mathcal MM; (C) minimality: Vλ(x)≤Vν(x)V_\lambda(x)\le V_\nu(x)Vλ​(x)≤Vν​(x) for all ν∈D\nu\in\mathcal Dν∈D, with Vλ(x)V_\lambda(x)Vλ​(x) attained by (cλ,ξλ)(c_\lambda,\xi_\lambda)(cλ​,ξλ​); (D) dual optimality: λ\lambdaλ minimizes ν↦E[∫0TU~1(t,yHν) dt+U~2(yHν(T))]\nu\mapsto E[\int_0^T\tilde U_1(t,yH_\nu)\,dt+\tilde U_2(yH_\nu(T))]ν↦E[∫0T​U~1​(t,yHν​)dt+U~2​(yHν​(T))] over D\mathcal DD; (E) parsimony: E[∫0THνcλ dt+Hν(T)ξλ]≤xE[\int_0^TH_\nu c_\lambda\,dt+H_\nu(T)\xi_\lambda]\le xE[∫0T​Hν​cλ​dt+Hν​(T)ξλ​]≤x for all ν∈D\nu\in\mathcal Dν∈D. The theorem asserts

(B)  ⟺  (C)  ⟺  (D)  ⟺  (E)  ⟹  (A) for (π^λ,cλ),(\mathrm B)\iff(\mathrm C)\iff(\mathrm D)\iff(\mathrm E)\implies(\mathrm A)\text{ for }(\hat\pi_\lambda,c_\lambda),(B)⟺(C)⟺(D)⟺(E)⟹(A) for (π^λ​,cλ​),

and, under the conditions (5.8) (c↦cU′(c)c\mapsto cU'(c)c↦cU′(c) nondecreasing), (8.25) (a uniform growth bound αU′(x)≥U′(γx)\alpha U'(x)\ge U'(\gamma x)αU′(x)≥U′(γx)) and (12.2) (finiteness of the dual functional for some ν\nuν), that (A) implies (B)–(E) for some λ∈D′\lambda\in\mathcal D'λ∈D′ with π^λ=π^\hat\pi_\lambda=\hat\piπ^λ​=π^.

Milestones

In proof order: the conjugate inequalities (5.5)–(5.6); the budget constraint (3.6); the unconstrained solution (Lemma 7.2, Proposition 7.3, Theorem 7.4); the embedding (8.14), V(x)≤Vν(x)V(x)\le V_\nu(x)V(x)≤Vν​(x); Proposition 8.3, (B) ⇒\Rightarrow⇒ optimality; the constrained budget constraint (9.4) and the hedging Theorem 9.1, (E) ⇒\Rightarrow⇒ (B); and Appendix A's Lemma A.1, Lemma A.2 and Proposition A.4, the steps of (A) ⇒\Rightarrow⇒ (B).

Significance

Theorem 10.1 turns a constrained stochastic control problem into a family of unconstrained ones plus a minimization over the dual process λ\lambdaλ. Condition (D) is a convex minimization over ν\nuν that does not involve portfolios. It leads to the dual problem of Section 12, whose solvability gives existence of optimal constrained policies (Theorem 13.1, the companion mission). Section 9's hedging theorem is the superreplication principle under convex constraints, the basis of later work on constrained hedging and pricing. With logarithmic utility the theorem gives explicit optimal policies, and for deterministic coefficients the dual problem reduces to a deterministic one.

These results are proved in the paper, which is the standard reference for the convex-duality approach. To our knowledge they have no machine-checked proof. The mission's statements also produce a reusable Lean model of a continuous-time Itô market with stochastic coefficients, admissible portfolios, consumption, utility functions and their conjugates.

Difficulty

The obvious argument, Lagrange duality for max⁡J\max JmaxJ subject to π∈K\pi\in Kπ∈K, fails at the first step: the constraint is on the control process, not on terminal wealth, so there is no static budget constraint to dualize. The paper's dual variable is a process, and for each candidate it changes both the interest rate and the drift. The direction (B) ⇒\Rightarrow⇒ (A) is relatively direct. The direction (E) ⇒\Rightarrow⇒ (B) is a hedging theorem under convex constraints (Theorem 9.1), where financing a claim requires the portfolio to land in KKK and to satisfy the complementary-slackness identity δ(λ)+π∗λ=0\delta(\lambda)+\pi^*\lambda=0δ(λ)+π∗λ=0, which no unconstrained construction delivers. The converse (A) ⇒\Rightarrow⇒ (B) must produce the dual process λ\lambdaλ from an optimal pair that is only assumed to exist, and the paper needs the extra growth conditions (5.8), (8.25), (12.2) for it. In Lean, stochastic integrals for integrands that are square integrable only almost surely, the martingale representation theorem for the Brownian filtration, and the product rule for Itô processes are not available in Mathlib.

Formalization scope

Processes are functions R≥0×Ω→E\mathbb R_{\ge0}\times\Omega\to ER≥0​×Ω→E constrained on [0,T][0,T][0,T]; vectors are EuclideanSpace ℝ (Fin d), matrices Matrix (Fin d) (Fin d) ℝ. The Brownian motion is the published EthierKurtz.IsStandardBrownian. The stochastic integral is a binder I, constrained only by the standing hypothesis that it is an Itô integral for every locally square-integrable integrand. This almost-sure variant of EthierKurtz.HasBrownianItoIntegral uses the published dyadic step helpers itoStepValue and itoStepSum. The hypothesis is satisfiable, by the classical construction.

The following readings are explicit in the Lean.

  • Triples. Classes are sets of triples (π,c,X)(\pi,c,X)(π,c,X) with XXX a wealth process: an adapted, a.s. continuous solution of the integral form of (3.1) or (8.10) whose integrals exist.
  • Extended reals. Utility expectations are extended reals, computed as positive minus negative parts. A utility at 000 is U(0+)U(0+)U(0+). Suprema are taken in the extended reals.
  • The support function. δ\deltaδ takes values in the extended reals. In drifts and discounts it enters as a real number, which is finite almost everywhere for ν∈D\nu\in\mathcal Dν∈D. The page's "E∫δ(ν)≤∞E\int\delta(\nu)\le\inftyE∫δ(ν)≤∞" in (8.1) is read as "<∞<\infty<∞".
  • Inverse marginals and conjugates. I(y)=inf⁡{x>0:U′(x)≤y}I(y)=\inf\{x>0: U'(x)\le y\}I(y)=inf{x>0:U′(x)≤y} and U~(y)=sup⁡x>0(U(x)−xy)\tilde U(y)=\sup_{x>0}(U(x)-xy)U~(y)=supx>0​(U(x)−xy).
  • The inverse Yλ\mathcal Y_\lambdaYλ​. Yλ(x)\mathcal Y_\lambda(x)Yλ​(x) and Y0(x)\mathcal Y_0(x)Y0​(x) are represented by a number y>0y>0y>0 with X(y)=x\mathcal X(y)=xX(y)=x.
  • The wealth XλX_\lambdaXλ​. It is a conditional expectation for each ttt. "X=XλX=X_\lambdaX=Xλ​" means X(t)=Xλ(t)X(t)=X_\lambda(t)X(t)=Xλ​(t) a.s. for every t≤Tt\le Tt≤T.
  • Almost everywhere. "ℓ⊗P\ell\otimes Pℓ⊗P-a.e." is almost everywhere for the product of Lebesgue measure on [0,T][0,T][0,T] and PPP. "a.s." is almost everywhere for PPP.
  • Theorem 9.1. Its conclusion "(π,c)∈A′(x)(\pi,c)\in\mathcal A'(x)(π,c)∈A′(x)" is formalized as A0(x)\mathcal A_0(x)A0​(x) plus π∈K\pi\in Kπ∈K a.e., since the theorem involves no utility.
  • (4.4). By Remark 4.2 it is not used in Theorem 10.1. It is kept, because the paper assumes it throughout.

A formalization in which the stochastic integral is an unconstrained function, a wealth process need not solve its equation, or δ\deltaδ is real-valued (so that sup⁡\supsup over an unbounded set returns 000) would make the statements vacuous or false; each is ruled out above. The proof will need almost-surely-square-integrable Itô integrals, Itô's product rule, nonnegative local martingales as supermartingales, and martingale representation in the Brownian filtration. All of these are reusable well beyond this mission, and contributions of any of them are welcome.

Selected references

  • J. Cvitanić and I. Karatzas, Convex duality in constrained portfolio optimization, Ann. Appl. Probab. 2(4) (1992) 767–818. https://doi.org/10.1214/aoap/1177005576
  • I. Karatzas, J. P. Lehoczky and S. E. Shreve, Optimal portfolio and consumption decisions for a "small investor" on a finite horizon, SIAM J. Control Optim. 25 (1987) 1557–1586. https://doi.org/10.1137/0325086
  • J. C. Cox and C. F. Huang, Optimal consumption and portfolio policies when asset prices follow a diffusion process, J. Econom. Theory 49 (1989) 33–83. https://doi.org/10.1016/0022-0531(89)90067-7
  • S. R. Pliska, A stochastic calculus model of continuous trading: optimal portfolios, Math. Oper. Res. 11 (1986) 371–382. https://doi.org/10.1287/moor.11.2.371
  • I. Karatzas, J. P. Lehoczky, S. E. Shreve and G. L. Xu, Martingale and duality methods for utility maximization in an incomplete market, SIAM J. Control Optim. 29 (1991) 702–730. https://doi.org/10.1137/0329039
  • H. He and N. D. Pearson, Consumption and portfolio policies with incomplete markets and short-sale constraints: the infinite-dimensional case, J. Econom. Theory 54 (1991) 259–304. https://doi.org/10.1016/0022-0531(91)90123-L
  • I. Karatzas and S. E. Shreve, Brownian Motion and Stochastic Calculus, Springer, 1988. https://doi.org/10.1007/978-1-4684-0302-2
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Scheduling a Multi Class Queue with Many Exponential Servers: Asymptotic Optimality in Heavy Traffic: The HJB-Based Preemptive Policy Is Asymptotically Optimal Among Work-Conserving PoliciesResearch Paper

Motivation

Large call centers route several types of customers to a common pool of agents. When the pool is large and highly utilized, the relevant asymptotic regime is the quality-and-efficiency-driven (QED) or Halfin–Whitt regime (Halfin & Whitt 1981). The number of servers nnn grows while the offered load stays within O(n)O(\sqrt n)O(n​) of nnn. Waiting is then neither negligible nor overwhelming (Gans, Koole & Mandelbaum 2003).

Which class should a freed agent serve next? Exact optimization of a multi-class many-server queue with abandonment is intractable. The standard route is to solve a limiting diffusion control problem and translate its optimal control back into a policy for the queue. Atar, Mandelbaum and Reiman (Ann. Appl. Probab. 2004) carried this out for kkk customer classes, exponential service and abandonment, general renewal arrivals and general convex-type holding costs. They proved that the translated policy is asymptotically optimal. This mission formalizes that result for the preemptive policy.

Context:

  • Harrison & Zeevi (2004) studied the same multi-class many-server problem.
  • Bell & Williams (2001) proved asymptotic optimality of a threshold policy for a two-server system in conventional heavy traffic.
  • The present paper is the first to cover the QED regime with general costs and abandonment.

Setting

There are k≥1k\ge1k≥1 customer classes and nnn identical servers.

Primitives.

  • Arrivals. Class-iii customers arrive according to a renewal process AinA^n_iAin​ with interarrival times Uˇi(j)/λin\check U_i(j)/\lambda^n_iUˇi​(j)/λin​. Here the Uˇi(j)\check U_i(j)Uˇi​(j) are i.i.d., positive, of mean one and squared coefficient of variation CU,i2C^2_{U,i}CU,i2​.
  • Service. Service times are exponential with rate μin\mu^n_iμin​, represented by Poisson processes SinS^n_iSin​.
  • Abandonment. Waiting customers abandon at rate θin≥0\theta^n_i\ge0θin​≥0, represented by Poisson processes RinR^n_iRin​.

State. Xin(t)X^n_i(t)Xin​(t) is the number of class-iii customers in the system, Ψin(t)\Psi^n_i(t)Ψin​(t) the number in service and Φin=Xin−Ψin\Phi^n_i=X^n_i-\Psi^n_iΦin​=Xin​−Ψin​ the number waiting. The dynamics are

Xin(t)=Xi0,n+Ain(t)−Rin(∫0tΦin)−Sin(∫0tΨin),Ψn,Φn∈Z+k,∑iΨin≤n.X^n_i(t)=X^{0,n}_i+A^n_i(t)-R^n_i\Big(\int_0^t\Phi^n_i\Big)-S^n_i\Big(\int_0^t\Psi^n_i\Big),\qquad \Psi^n,\Phi^n\in\mathbb Z^k_+,\quad \textstyle\sum_i\Psi^n_i\le n .Xin​(t)=Xi0,n​+Ain​(t)−Rin​(∫0t​Φin​)−Sin​(∫0t​Ψin​),Ψn,Φn∈Z+k​,∑i​Ψin​≤n.

Policies.

  • A scheduling control policy (SCP) is the process Ψn\Psi^nΨn.
  • It is admissible if it does not anticipate the future beyond the time of the next arrival: past information is independent of future primitive increments.
  • It is work-conserving if no server idles while customers wait: (1⋅Xn−n)+=1⋅Φn(\mathbb 1\cdot X^n-n)^+=\mathbb 1\cdot\Phi^n(1⋅Xn−n)+=1⋅Φn.

Scaling and cost. In the QED scaling n−1λin→λin^{-1}\lambda^n_i\to\lambda_in−1λin​→λi​ with ∑iλi/μi=1\sum_i\lambda_i/\mu_i=1∑i​λi​/μi​=1. With ρi=λi/μi\rho_i=\lambda_i/\mu_iρi​=λi​/μi​ the centred processes are X^n=n−1/2(Xn−ρn)\hat X^n=n^{-1/2}(X^n-\rho n)X^n=n−1/2(Xn−ρn), Φ^n=n−1/2Φn\hat\Phi^n=n^{-1/2}\Phi^nΦ^n=n−1/2Φn and Ψ^n=n−1/2(Ψn−ρn)\hat\Psi^n=n^{-1/2}(\Psi^n-\rho n)Ψ^n=n−1/2(Ψn−ρn). The cost is

Cn=E∫0∞e−γtL~(Φ^n(t),Ψ^n(t)) dt.C^n=E\int_0^\infty e^{-\gamma t}\tilde L(\hat\Phi^n(t),\hat\Psi^n(t))\,dt .Cn=E∫0∞​e−γtL~(Φ^n(t),Ψ^n(t))dt.

The limiting control problem. It controls

X(t)=x+rW(t)+∫0tb(X(s),u(s)) ds,b(x,u)=ℓ+(μ−θ)(1⋅x)+u−μx,X(t)=x+rW(t)+\int_0^t b(X(s),u(s))\,ds,\qquad b(x,u)=\ell+(\mu-\theta)(\mathbb 1\cdot x)^+u-\mu x,X(t)=x+rW(t)+∫0t​b(X(s),u(s))ds,b(x,u)=ℓ+(μ−θ)(1⋅x)+u−μx,

where the control uuu takes values in the simplex Sk\mathbb S^kSk and WWW is a kkk-dimensional Brownian motion. The data are ri=(λiCU,i2+λi)1/2r_i=(\lambda_iC^2_{U,i}+\lambda_i)^{1/2}ri​=(λi​CU,i2​+λi​)1/2 and ℓi=λ^i−ρiμ^i\ell_i=\hat\lambda_i-\rho_i\hat\mu_iℓi​=λ^i​−ρi​μ^​i​. Its value V(x)V(x)V(x) is the infimum of E∫0∞e−γtL(X,u) dtE\int_0^\infty e^{-\gamma t}L(X,u)\,dtE∫0∞​e−γtL(X,u)dt, with L(x,u)=L~((1⋅x)+u,x−(1⋅x)+u)L(x,u)=\tilde L((\mathbb 1\cdot x)^+u,x-(\mathbb 1\cdot x)^+u)L(x,u)=L~((1⋅x)+u,x−(1⋅x)+u).

HJB equation and the proposed policy. The HJB equation is 12∑iri2∂iif+H(x,Df)−γf=0\tfrac12\sum_ir_i^2\partial_{ii}f+H(x,Df)-\gamma f=021​∑i​ri2​∂ii​f+H(x,Df)−γf=0 with H(x,p)=inf⁡u∈Sk[b(x,u)⋅p+L(x,u)]H(x,p)=\inf_{u\in\mathbb S^k}[b(x,u)\cdot p+L(x,u)]H(x,p)=infu∈Sk​[b(x,u)⋅p+L(x,u)]. Let hhh be a measurable selection of its minimizers. The proposed preemptive policy (P-SCP) sets the queue vector to Θ[(1⋅Xn−n)+h(X^n)]\Theta[(\mathbb 1\cdot X^n-n)^+h(\hat X^n)]Θ[(1⋅Xn−n)+h(X^n)], an integer rounding, and falls back to a static priority rule when that is infeasible.

Formalization targets

Goal: Theorem 2(i)

For a Cpol2C^2_{\mathrm{pol}}Cpol2​ solution fff of the HJB equation, a measurable minimizer selection hhh, and initial states with X^0,n→x\hat X^{0,n}\to xX^0,n→x:

lim⁡n→∞E∫0∞e−γtL~(Φ^tn,∗,Ψ^tn,∗) dt  ≤  lim inf⁡n→∞E∫0∞e−γtL~(Φ^tn,Ψ^tn) dt\lim_{n\to\infty}E\int_0^\infty e^{-\gamma t}\tilde L(\hat\Phi^{n,*}_t,\hat\Psi^{n,*}_t)\,dt\;\le\;\liminf_{n\to\infty}E\int_0^\infty e^{-\gamma t}\tilde L(\hat\Phi^n_t,\hat\Psi^n_t)\,dtn→∞lim​E∫0∞​e−γtL~(Φ^tn,∗​,Ψ^tn,∗​)dt≤n→∞liminf​E∫0∞​e−γtL~(Φ^tn​,Ψ^tn​)dt

This holds for every sequence of work-conserving admissible SCPs, and the left-hand limit exists and is finite. No constants are hard-coded.

Milestones

The milestones follow the proof:

  • on the diffusion side, Proposition 2 (well-posedness), Proposition 4 (stability and moment bounds), Proposition 5(i)–(ii) (growth and continuity of VVV) and Theorem 3 (VVV is the unique Cpol2C^2_{\mathrm{pol}}Cpol2​ HJB solution, and an optimal Markov policy exists);
  • on the queueing side, Proposition 1 (feedback rules give admissible SCPs), Lemmas 2–3 (moment bounds), Lemma 4(i)–(ii) (FCLT for the primitives and the fluid limit (Ψˉn,Φˉn)⇒(ρ,0)(\bar\Psi^n,\bar\Phi^n)\Rightarrow(\rho,0)(Ψˉn,Φˉn)⇒(ρ,0)), and Theorem 4(i)–(ii): lim inf⁡≥V(x)\liminf\ge V(x)liminf≥V(x) always, and lim sup⁡≤V(x)\limsup\le V(x)limsup≤V(x) under condition (49).

Significance

The result. Theorem 2(i) justifies using the diffusion control problem as a design tool for multi-class many-server systems. The policy is explicit given hhh, and it is optimal in the limit against all non-anticipating work-conserving policies, including those that use the full history and the time of the next arrival. The proof also identifies the limit cost with V(x)V(x)V(x).

Formalizing it. The result is proved on paper, with some steps (Proposition 1, the principle of optimality, the time-change and martingale limit theorems) given as sketches or citations. No part of it is machine-checked. A formalization requires:

  • a counting-process model of the queue;
  • a careful definition of non-anticipation;
  • a pathwise controlled SDE;
  • classical solvability of a semilinear elliptic HJB equation on Rk\mathbb R^kRk;
  • a weak-convergence argument in Skorokhod space.

Each of these is reusable well beyond this paper.

Difficulty

The obvious argument would show that X^n\hat X^nX^n converges to the controlled diffusion and pass the costs to the limit. This fails for two reasons:

  • the comparison class contains arbitrary non-Markov, history-dependent policies, so the queue does not converge to a single controlled diffusion;
  • the optimal selector hhh is in general discontinuous (for linear costs it is), so the proposed policy is not a continuous function of the state.

The proof instead compares every policy with the HJB solution through Itô's formula on the prelimit processes. This needs:

  • uniform moment bounds;
  • tightness of the integral processes;
  • the convergence of stochastic integrals of Kurtz and Protter;
  • and, for the proposed policy, the fact that the rounding Θ\ThetaΘ and the priority fallback perturb the minimizer by O(n−1/2)O(n^{-1/2})O(n−1/2).

Existence of a classical HJB solution on all of Rk\mathbb R^kRk, with only Hölder-continuous costs and polynomial growth, rests on a bounded-domain existence theorem for fully nonlinear elliptic equations.

Formalization scope

The Lean development commits to the following conventions.

  • Indexing and norms. Classes are Fin k with k≥1k\ge1k≥1; paper class iii is index i−1i-1i−1, so "class kkk" (highest priority, rounding remainder of Θ\ThetaΘ) is the last index. Vectors are Fin k → ℝ and ∥⋅∥\|\cdot\|∥⋅∥ is the paper's ℓ1\ell^1ℓ1 norm; the paper's ∣⋅∣|\cdot|∣⋅∣ on vectors is read the same way.
  • Probability space and paths. All systems share one complete probability space. Time is real and every condition is for t≥0t\ge0t≥0. The paper's "without loss" path regularity (finite arrival counts, Poisson paths Z+\mathbb Z_+Z+​-valued, nondecreasing and càdlàg) holds for every ω\omegaω.
  • Poisson processes are defined by independent Poisson increments; rate 000 gives the zero process.
  • Policies. A policy is a pair of real processes (Ψn,Xn)(\Psi^n,X^n)(Ψn,Xn) with integer values. Admissibility is Definition 2 verbatim, with the future σ\sigmaσ-field built from the next arrival time τin(t)\tau^n_i(t)τin​(t). Work conservation is (18).
  • Costs and value are lower Lebesgue integrals in [0,∞][0,\infty][0,∞], and lim⁡\limlim/lim inf⁡\liminfliminf are taken there. The integrands are nonnegative under work conservation.
  • Admissible systems range over sample spaces Ω : Type (universe 0). "Complete filtered probability space" means PPP complete with all null sets in F0\mathcal F_0F0​. Brownian motion is Mathlib's IsBrownianReal per coordinate, with independence and the (Ft)(\mathcal F_t)(Ft​)-Brownian property stated explicitly. VVV is the infimum over systems and their controlled processes.
  • Discount rate. γ>0\gamma>0γ>0 is a hypothesis; the paper leaves it implicit.
  • Initial states are integer vectors X0,n∈Z+kX^{0,n}\in\mathbb Z^k_+X0,n∈Z+k​ with n−1/2(X0,n−ρn)→xn^{-1/2}(X^{0,n}-\rho n)\to xn−1/2(X0,n−ρn)→x. The literal "X^0,n∈n−1/2Zk\hat X^{0,n}\in n^{-1/2}\mathbb Z^kX^0,n∈n−1/2Zk" would require ρin∈Z\rho_in\in\mathbb Zρi​n∈Z. Assumption 1(ii) is not imposed: each policy chooses its own initial split.
  • Lemma 3 is stated for all nnn beyond a threshold that depends on the sequence, with constants c,mˉc,\bar mc,mˉ chosen before xxx and the sequence. The printed all-nnn bound with ccc independent of xxx fails when the early terms X^0,n\hat X^{0,n}X^0,n are large.
  • Weak convergence to a continuous limit uses the coupling form CouplingConverges of the published BellWilliams2001.ThresholdPolicy.Paths; convergence to a deterministic limit is UocInProb.

The goal hypothesizes fff and hhh with the pointwise identity b(x,h(x))⋅Df(x)+L(x,h(x))=H(x,Df(x))b(x,h(x))\cdot Df(x)+L(x,h(x))=H(x,Df(x))b(x,h(x))⋅Df(x)+L(x,h(x))=H(x,Df(x)) for all xxx. An arbitrary "optimal Markov control policy" may differ from a minimizer selection on the Lebesgue-null lattice where X^n\hat X^nX^n lives, and that formalization would make the goal false. Restricting the comparators to feedback, Markov or nonpreemptive policies, fixing kkk, dropping abandonment, specializing to Poisson arrivals or linear costs, or imposing a common initial split would each trivialize or weaken the statement and is ruled out.

Not formalized:

  • Lemma 4(iii) (tightness);
  • Lemma 5 (Kurtz–Protter, which needs semimartingale theory absent from Mathlib);
  • Lemma 6 (convergence of Stieltjes integrals at limit points);
  • Proposition 5(iii);
  • the nonpreemptive results, Theorem 2(ii)–(iii).

Contributions are welcome on any milestone, and especially on infrastructure: Poisson and renewal processes, functional central limit theorems in Skorokhod space, classical solvability of elliptic HJB equations, and measurable selection of minimizers.

Selected references

  • R. Atar, A. Mandelbaum, M. I. Reiman, Scheduling a multi class queue with many exponential servers: asymptotic optimality in heavy traffic, Ann. Appl. Probab. 14(3), 2004. https://arxiv.org/abs/math/0407058
  • S. Halfin, W. Whitt, Heavy-traffic limits for queues with many exponential servers, Oper. Res. 29(3), 1981. https://doi.org/10.1287/opre.29.3.567
  • N. Gans, G. Koole, A. Mandelbaum, Telephone call centers: tutorial, review, and research prospects, Manuf. Serv. Oper. Manag. 5(2), 2003. https://doi.org/10.1287/msom.5.2.79.16071
  • J. M. Harrison, A. Zeevi, Dynamic scheduling of a multiclass queue in the Halfin–Whitt heavy traffic regime, Oper. Res. 52(2), 2004. https://doi.org/10.1287/opre.1040.0109
  • S. L. Bell, R. J. Williams, Dynamic scheduling of a system with two parallel servers in heavy traffic with resource pooling: asymptotic optimality of a threshold policy, Ann. Appl. Probab. 11(3), 2001. https://doi.org/10.1214/aoap/1015345343
  • T. G. Kurtz, P. Protter, Weak limit theorems for stochastic integrals and stochastic differential equations, Ann. Probab. 19(3), 1991. https://doi.org/10.1214/aop/1176990334
16 thms1 active userReviewed
Dynamic ProgrammingProbability·Captain: mikedeng1

Discrete-Time Controlled Markov Processes with Average Cost Criterion: A Survey 6: A Canonical Policy Is Strong Average Optimal and Its Average Cost Is the Optimal OneResearch Paper

Motivation

A controlled Markov process (CMP), or Markov decision process, models a system that moves randomly between states while a controller chooses actions that influence both the cost incurred and the next state. When the planning horizon is long and no discounting is natural (queueing control, inventory, communication networks, maintenance), the criterion of interest is the long-run average cost. Average-cost problems are harder than discounted ones: the dynamic programming operator is no longer a contraction, and an optimal policy need not exist without structure.

The survey of Arapostathis, Borkar, Fernández-Gaucherand, Ghosh and Marcus (SIAM J. Control Optim. 31 (1993)) organizes the theory by state space. For Borel state spaces and bounded costs, §6.1 follows Dynkin and Yushkevich and works with canonical triplets: a pair of bounded functions and a policy that make the policy optimal for every finite horizon with a fixed terminal cost. Theorem 6.3 is the statement that explains why this notion is the right one: a canonical triplet solves the average-cost problem.

Timeline. The notion of a canonical policy was introduced by Yushkevich (1973) and developed in Dynkin and Yushkevich's Controlled Markov Processes (1979, Chap. 7), which contains the substance of Theorem 6.3 (i)–(iii). Mandl (1974) introduced the discrepancy function that bears his name. The almost-sure statements (v)–(vi) are due to Georgin (1978). Coupled optimality equations for the multichain case go back to Howard (1960).

Setting

The model is a five-tuple (S,A,U,P,c)(S, A, U, P, c)(S,A,U,P,c). The state space SSS and the action space AAA are Borel spaces. For each state xxx, U(x)⊆AU(x)\subseteq AU(x)⊆A is a nonempty compact set of admissible actions, and K={(x,a):a∈U(x)}K = \{(x,a): a\in U(x)\}K={(x,a):a∈U(x)} is measurable. P(dy∣x,a)P(dy\mid x,a)P(dy∣x,a) is a transition kernel and ccc a measurable one-stage cost, nonnegative on KKK.

A policy π=(πt)\pi = (\pi_t)π=(πt​) chooses the action at time ttt at random from a kernel πt(da∣ht)\pi_t(da\mid h_t)πt​(da∣ht​) that may depend on the whole history ht=(x0,a0,…,xt)h_t = (x_0,a_0,\dots,x_t)ht​=(x0​,a0​,…,xt​) and charges only U(xt)U(x_t)U(xt​). The class of all such policies is Π\PiΠ. Each policy and initial state xxx determine a law Pxπ\mathcal P^\pi_xPxπ​ of the state–action process (Xt,At)(X_t, A_t)(Xt​,At​), with expectation ExπE^\pi_xExπ​.

For a horizon NNN and a terminal cost hhh,

JN(x,π,h)=Exπ[∑t=0N−1c(Xt,At)+h(XN)],JN(x,π)=JN(x,π,0),JN∗(x,h)=inf⁡π∈ΠJN(x,π,h).J_N(x,\pi,h) = E^\pi_x\Big[\sum_{t=0}^{N-1}c(X_t,A_t) + h(X_N)\Big],\qquad J_N(x,\pi)=J_N(x,\pi,0),\qquad J^*_N(x,h)=\inf_{\pi\in\Pi}J_N(x,\pi,h).JN​(x,π,h)=Exπ​[t=0∑N−1​c(Xt​,At​)+h(XN​)],JN​(x,π)=JN​(x,π,0),JN∗​(x,h)=π∈Πinf​JN​(x,π,h).

The average cost is J(x,π)=lim sup⁡N1NJN(x,π)J(x,\pi)=\limsup_N \frac1N J_N(x,\pi)J(x,π)=limsupN​N1​JN​(x,π) and the optimal average cost is J∗(x)=inf⁡π∈ΠJ(x,π)J^*(x)=\inf_{\pi\in\Pi}J(x,\pi)J∗(x)=infπ∈Π​J(x,π). The span of a bounded function is span⁡(h)=sup⁡h−inf⁡h\operatorname{span}(h)=\sup h-\inf hspan(h)=suph−infh.

With Mb(S)\mathcal M_b(S)Mb​(S) the bounded measurable functions, a triplet (ρ,h,π∗)(\rho,h,\pi^*)(ρ,h,π∗) with ρ,h∈Mb(S)\rho,h\in\mathcal M_b(S)ρ,h∈Mb​(S) and π∗∈Π\pi^*\in\Piπ∗∈Π is canonical if

JN(x,π∗,h)=JN∗(x,h)=h(x)+Nρ(x)∀N∈N0, x∈S.(6.4)J_N(x,\pi^*,h) = J^*_N(x,h) = h(x)+N\rho(x)\qquad\forall N\in\mathbb N_0,\ x\in S. \tag{6.4}JN​(x,π∗,h)=JN∗​(x,h)=h(x)+Nρ(x)∀N∈N0​, x∈S.(6.4)

A policy π∗\pi^*π∗ is strong average optimal if

lim sup⁡N→∞1NJN(x,π∗)≤lim inf⁡N→∞1NJN(x,π)∀x∈S, π∈Π.(6.5)\limsup_{N\to\infty}\frac1N J_N(x,\pi^*)\le\liminf_{N\to\infty}\frac1N J_N(x,\pi)\qquad\forall x\in S,\ \pi\in\Pi. \tag{6.5}N→∞limsup​N1​JN​(x,π∗)≤N→∞liminf​N1​JN​(x,π)∀x∈S, π∈Π.(6.5)

Formalization targets

Goal: Theorem 6.3 (i)–(iii)

Let (ρ,h,π∗)(\rho,h,\pi^*)(ρ,h,π∗) be a canonical triplet and let ccc be bounded on KKK. Then for each x∈Sx\in Sx∈S:

(i)JN(x,π∗)≤JN(x,π)+span⁡(h)∀N, ∀π∈Π;\text{(i)}\quad J_N(x,\pi^*)\le J_N(x,\pi)+\operatorname{span}(h)\quad\forall N,\ \forall\pi\in\Pi;(i)JN​(x,π∗)≤JN​(x,π)+span(h)∀N, ∀π∈Π; (ii)π∗ is strong average optimal;(iii)J(x,π∗)=J∗(x)=ρ(x).\text{(ii)}\quad \pi^* \text{ is strong average optimal};\qquad \text{(iii)}\quad J(x,\pi^*)=J^*(x)=\rho(x).(ii)π∗ is strong average optimal;(iii)J(x,π∗)=J∗(x)=ρ(x).

Steps toward the goal

The proof's milestones are: JN(x,π∗,h)≤JN(x,π,h)J_N(x,\pi^*,h)\le J_N(x,\pi,h)JN​(x,π∗,h)≤JN​(x,π,h); the decomposition JN(x,π,h)=JN(x,π)+Exπ[h(XN)]J_N(x,\pi,h)=J_N(x,\pi)+E^\pi_x[h(X_N)]JN​(x,π,h)=JN​(x,π)+Exπ​[h(XN​)]; part (i) on its own; and ρ(x)=lim⁡N1NJN(x,π∗)\rho(x)=\lim_N\frac1N J_N(x,\pi^*)ρ(x)=limN​N1​JN​(x,π∗).

Further targets: Theorem 6.3 (v)–(vi)

If ρ≡ρ∗\rho\equiv\rho^*ρ≡ρ∗ is constant and Φ(x,a)=c(x,a)+∫h(y)P(dy∣x,a)−ρ∗−h(x)\Phi(x,a)=c(x,a)+\int h(y)P(dy\mid x,a)-\rho^*-h(x)Φ(x,a)=c(x,a)+∫h(y)P(dy∣x,a)−ρ∗−h(x) is Mandl's discrepancy function, then for every π∈Π\pi\in\Piπ∈Π and xxx,

lim sup⁡N→∞1N∑t=0N−1c(Xt,At)≥ρ∗Pxπ-a.s.,\limsup_{N\to\infty}\frac1N\sum_{t=0}^{N-1}c(X_t,A_t)\ge\rho^*\quad\mathcal P^\pi_x\text{-a.s.},N→∞limsup​N1​t=0∑N−1​c(Xt​,At​)≥ρ∗Pxπ​-a.s.,

and the running average converges to ρ∗\rho^*ρ∗ almost surely if and only if 1N∑t<NΦ(Xt,At)→0\frac1N\sum_{t<N}\Phi(X_t,A_t)\to0N1​∑t<N​Φ(Xt​,At​)→0 almost surely. Moreover π∗\pi^*π∗ is sample path average cost optimal. The intermediate milestones are Φ≥0\Phi\ge0Φ≥0 on KKK, the almost-sure limit 1N∑c−ρ∗−1N∑Φ→0\frac1N\sum c-\rho^*-\frac1N\sum\Phi\to0N1​∑c−ρ∗−N1​∑Φ→0 under every policy, and Φ(Xt,At)=0\Phi(X_t,A_t)=0Φ(Xt​,At​)=0 almost surely under π∗\pi^*π∗.

Significance

The result. Theorem 6.3 reduces the average-cost problem on a general Borel space to finding a canonical triplet. Once one is found, ρ\rhoρ is the optimal average cost from every initial state, possibly state-dependent as in multichain models, and the canonical policy is optimal in a strong sense: its worst-case long-run performance is no worse than the best-case long-run performance of any competitor, at every finite horizon up to the additive constant span⁡(h)\operatorname{span}(h)span(h). With constant ρ\rhoρ, optimality also holds path by path. The rest of §6 of the survey looks for conditions on ccc and PPP that produce a canonical triplet, and those results rely on this theorem.

Formalizing it. The result is classical and proved; it has no machine-checked proof that we know of. Formalization requires measure-theoretic infrastructure for history-dependent policies on Borel spaces (Ionescu-Tulcea path measures, finite-horizon costs, infima over all admissible policies) together with a strong law for bounded martingale differences for parts (v)–(vi). Both are reusable for any average-cost result on general state spaces.

Difficulty

Parts (i)–(iii) are short on paper; the work is in making every quantity genuine. The infimum JN∗J^*_NJN∗​ ranges over a class of kernels, and turning (6.4) into a usable inequality needs the family bounded below. The decomposition of JN(x,π,h)J_N(x,\pi,h)JN​(x,π,h) needs integrability, which comes from the almost-sure confinement of the trajectory to KKK, a consequence of admissibility under the path measure. Parts (v)–(vi) need the conditional expectation identity Exπ[c(Xt,At)+h(Xt+1)−ρ∗−h(Xt)∣Ht,At]=Φ(Xt,At)E^\pi_x[c(X_t,A_t)+h(X_{t+1})-\rho^*-h(X_t)\mid H_t,A_t]=\Phi(X_t,A_t)Exπ​[c(Xt​,At​)+h(Xt+1​)−ρ∗−h(Xt​)∣Ht​,At​]=Φ(Xt​,At​) from the Markov structure of the path measure, and a martingale strong law. The tempting shortcut of restricting to stationary or Markov policies is not available: π∗\pi^*π∗ and every competitor are arbitrary history-dependent randomized policies.

Formalization scope

  • SSS is a standard Borel space and AAA a Borel space; U(x)U(x)U(x) is nonempty and compact with measurable graph KKK; c≥0c\ge0c≥0 on KKK (Assumption 2.1, which the paper assumes throughout). ccc and PPP are defined on S×AS\times AS×A and only their values on KKK enter.
  • Π\PiΠ is the class of history-dependent randomized admissible policies (p. 285). Neither π∗\pi^*π∗ nor the competitors are restricted.
  • Pxπ\mathcal P^\pi_xPxπ​ is Mathlib's Kernel.trajMeasure. JNJ_NJN​ is a Bochner integral and JN∗J^*_NJN∗​ a real infimum; every theorem assumes ccc bounded on KKK, which makes both genuine.
  • JJJ, J∗J^*J∗, both sides of (6.5), and the sample path average cost JSJ_SJS​ are computed in EReal, so no limit superior or inferior is a junk value. Part (iii) is the two equalities J(x,π∗)=J∗(x)J(x,\pi^*)=J^*(x)J(x,π∗)=J∗(x) and J∗(x)=ρ(x)J^*(x)=\rho(x)J∗(x)=ρ(x).
  • Part (iv) is not posed: its proof goes through value iteration under Assumptions 2.1–2.3, which Theorem 6.3 does not assume.
  • Part (vi) is stated under the hypothesis of (v), ρ≡ρ∗\rho\equiv\rho^*ρ≡ρ∗ constant. As printed it has no hypothesis on ρ\rhoρ and is false: two absorbing states with costs 000 and 111 give a canonical triplet whose pathwise average costs differ by state.
  • The identity JN(x,π,h)=JN(x,π)+Exπ[h(XN)]J_N(x,\pi,h)=J_N(x,\pi)+E^\pi_x[h(X_N)]JN​(x,π,h)=JN​(x,π)+Exπ​[h(XN​)] is stated for every π\piπ; the page writes it for π∗\pi^*π∗ and applies it to an arbitrary π\piπ in the proof of (i).
  • The sentence "for a canonical policy π∗\pi^*π∗, Φ(Xt,At)=0\Phi(X_t,A_t)=0Φ(Xt​,At​)=0, Pxπ\mathcal P^\pi_xPxπ​-a.s." is stated with Pxπ∗\mathcal P^{\pi^*}_xPxπ∗​, the only reading that makes sense.
  • Φ≥0\Phi\ge0Φ≥0 is derived on the page from (6.7) via Theorem 6.2, which covers stationary π∗\pi^*π∗; here it is stated directly from the canonical triplet for arbitrary π∗∈Π\pi^*\in\Piπ∗∈Π.
  • Sample path optimality quantifies over all initial laws (probability measures on SSS), as on p. 288.
  • None of the hypotheses is vacuous: the one-state, one-action model with zero cost and ρ≡h≡0\rho\equiv h\equiv0ρ≡h≡0 is a canonical triplet (checked in Lean). Strong average optimality is stated as limsup against liminf, not the weaker limsup against limsup.

Contributions welcome: a.s. confinement of trajectories to KKK, integrability lemmas for JNJ_NJN​, the Markov property of trajMeasure in the form above, and a strong law for bounded martingale differences.

Selected references

  • A. Arapostathis, V. S. Borkar, E. Fernández-Gaucherand, M. K. Ghosh, S. I. Marcus, Discrete-time controlled Markov processes with average cost criterion: a survey, SIAM J. Control Optim. 31(2) (1993) 282–344. https://doi.org/10.1137/0331018 (Theorem 6.3 on p. 318, its proof on pp. 318–319; (6.4), (6.5) on p. 316)
  • E. B. Dynkin, A. A. Yushkevich, Controlled Markov Processes, Springer-Verlag, New York, 1979 (reference [51] of the survey; Chap. 7).
  • A. A. Yushkevich, On a class of strategies in general Markov decision models, Theory Probab. Appl. 18 (1973) 777–779 (reference [204] of the survey).
  • P. Mandl, Estimation and control in Markov chains, Adv. Appl. Probab. 6 (1974) 40–60 (reference [124] of the survey).
  • J.-P. Georgin, Contrôle de chaînes de Markov sur des espaces arbitraires, Ann. Inst. H. Poincaré Sect. B 14 (1978) 255–277 (reference [72] of the survey).
  • R. A. Howard, Dynamic Programming and Markov Processes, MIT Press, Cambridge, MA, 1960 (reference [95] of the survey).
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Discrete-Time Controlled Markov Processes with Average Cost Criterion: A Survey 5: Canonical Triplets Are Exactly the Solutions of the Coupled Optimality EquationsResearch Paper

Motivation

A controlled Markov process run under the long-run average cost criterion asks for a policy minimizing the asymptotic cost per stage. When every stationary policy induces a single recurrent class, the optimal average cost is a constant and is characterized by one equation, the average cost optimality equation (ACOE). In general it is not: under some policies the state process splits into several ergodic classes, different classes have different optimal costs, and the optimal average cost is a function ρ(x)\rho(x)ρ(x) of the initial state. This is the multichain case.

For finite models, Howard ([Dynamic Programming and Markov Processes, 1960, pp. 61–62]) introduced a pair of coupled equations for this situation: one for the gain function ρ\rhoρ alone, and one, the ACOE, for ρ\rhoρ together with a relative value function hhh. Denardo and Fox (1968) developed the approach for finite multichain Markov renewal programs. For general Borel models, Yushkevich (1973) and Dynkin and Yushkevich (1979) introduced canonical triplets: a gain ρ\rhoρ, a terminal cost hhh and a policy π∗\pi^*π∗ such that π∗\pi^*π∗ is optimal for every finite horizon NNN with terminal cost hhh, and the optimal NNN-stage cost is exactly h+Nρh + N\rhoh+Nρ. The survey of Arapostathis, Borkar, Fernández-Gaucherand, Ghosh and Marcus (SIAM J. Control Optim. 31 (1993), §6.1) states the link between the two notions as Theorem 6.2 and proves it on p. 317.

Setting

A controlled Markov process is a five-tuple (S,A,U,P,c)(\mathbf S, \mathbf A, U, P, c)(S,A,U,P,c):

  1. S\mathbf SS, the state space, and A\mathbf AA, the action space, are Borel spaces;
  2. U(x)⊆AU(x) \subseteq \mathbf AU(x)⊆A is the nonempty compact set of admissible actions at xxx, and K={(x,a):a∈U(x)}\mathbf K = \{(x,a) : a \in U(x)\}K={(x,a):a∈U(x)} is measurable;
  3. P(dy∣x,a)P(dy \mid x, a)P(dy∣x,a) is a transition kernel on S\mathbf SS given K\mathbf KK;
  4. c:K→Rc : \mathbf K \to \mathbb Rc:K→R is a measurable one-stage cost with c≥0c \ge 0c≥0 (the paper's standing Assumption 2.1).

A history is ht=(x0,a0,…,xt−1,at−1,xt)h_t = (x_0, a_0, \dots, x_{t-1}, a_{t-1}, x_t)ht​=(x0​,a0​,…,xt−1​,at−1​,xt​). An admissible policy π=(πt)\pi = (\pi_t)π=(πt​) is a sequence of stochastic kernels πt(⋅∣ht)\pi_t(\cdot \mid h_t)πt​(⋅∣ht​) on A\mathbf AA with πt(U(xt)∣ht)=1\pi_t(U(x_t) \mid h_t) = 1πt​(U(xt​)∣ht​)=1; the class of all of them is Π\PiΠ. A stationary deterministic policy f∈ΠSDf \in \Pi_{SD}f∈ΠSD​ is a measurable map f:S→Af : \mathbf S \to \mathbf Af:S→A with f(x)∈U(x)f(x) \in U(x)f(x)∈U(x). An initial state xxx and a policy π\piπ determine a probability measure Pxπ\mathcal P^\pi_xPxπ​ on trajectories, with expectation ExπE^\pi_xExπ​. For a terminal cost hhh and N∈N0N \in \mathbb N_0N∈N0​,

JN(x,π,h)=Exπ[∑t=0N−1c(Xt,At)+h(XN)],JN∗(x,h)=inf⁡π∈ΠJN(x,π,h).J_N(x, \pi, h) = E^\pi_x\Big[\sum_{t=0}^{N-1} c(X_t, A_t) + h(X_N)\Big], \qquad J^*_N(x, h) = \inf_{\pi \in \Pi} J_N(x, \pi, h).JN​(x,π,h)=Exπ​[t=0∑N−1​c(Xt​,At​)+h(XN​)],JN∗​(x,h)=π∈Πinf​JN​(x,π,h).

Mb(S)\mathcal M_b(\mathbf S)Mb​(S) denotes the bounded measurable real functions on S\mathbf SS. For R,H∈Mb(S)R, H \in \mathcal M_b(\mathbf S)R,H∈Mb​(S) and π∗∈Π\pi^* \in \Piπ∗∈Π, the triplet (R,H,π∗)(R, H, \pi^*)(R,H,π∗) is canonical if

JN(x,π∗,H)=JN∗(x,H)=H(x)+NR(x)∀N∈N0, x∈S.(6.4)J_N(x, \pi^*, H) = J^*_N(x, H) = H(x) + N R(x) \qquad \forall N \in \mathbb N_0,\ x \in \mathbf S. \tag{6.4}JN​(x,π∗,H)=JN∗​(x,H)=H(x)+NR(x)∀N∈N0​, x∈S.(6.4)

Formalization targets

Goal: Theorem 6.2

Let π∗∈ΠSD\pi^* \in \Pi_{SD}π∗∈ΠSD​, ρ,h∈Mb(S)\rho, h \in \mathcal M_b(\mathbf S)ρ,h∈Mb​(S), and ccc bounded on K\mathbf KK. Then (ρ,h,π∗)(\rho, h, \pi^*)(ρ,h,π∗) is a canonical triplet if and only if, for all x∈Sx \in \mathbf Sx∈S,

ρ(x)=inf⁡a∈U(x){∫Sρ(y)P(dy∣x,a)},(6.6)\rho(x) = \inf_{a \in U(x)} \Big\{ \int_{\mathbf S} \rho(y) P(dy \mid x, a) \Big\}, \tag{6.6}ρ(x)=a∈U(x)inf​{∫S​ρ(y)P(dy∣x,a)},(6.6) ρ(x)+h(x)=inf⁡a∈U(x){c(x,a)+∫Sh(y)P(dy∣x,a)},(6.7)\rho(x) + h(x) = \inf_{a \in U(x)} \Big\{ c(x,a) + \int_{\mathbf S} h(y) P(dy \mid x, a) \Big\}, \tag{6.7}ρ(x)+h(x)=a∈U(x)inf​{c(x,a)+∫S​h(y)P(dy∣x,a)},(6.7)

and π∗(x)\pi^*(x)π∗(x) attains the infimum in both (6.6) and (6.7).

Milestones (the steps of the proof on p. 317)

  1. One-step decomposition (last line of (6.8)): for f∈ΠSDf \in \Pi_{SD}f∈ΠSD​, JN+1(x,f,h)=c(x,f(x))+∫JN(y,f,h)P(dy∣x,f(x))J_{N+1}(x, f, h) = c(x, f(x)) + \int J_N(y, f, h) P(dy \mid x, f(x))JN+1​(x,f,h)=c(x,f(x))+∫JN​(y,f,h)P(dy∣x,f(x)).
  2. Dynamic programming step (second line of (6.8)): if JN∗(⋅,h)J^*_N(\cdot, h)JN∗​(⋅,h) is bounded and measurable, then JN+1(x,π,h)≥T(JN∗)(x)J_{N+1}(x, \pi, h) \ge T(J^*_N)(x)JN+1​(x,π,h)≥T(JN∗​)(x) for every admissible π\piπ, where T(v)(x)=inf⁡a∈U(x){c(x,a)+∫v dP(⋅∣x,a)}T(v)(x) = \inf_{a \in U(x)}\{c(x,a) + \int v\, dP(\cdot \mid x, a)\}T(v)(x)=infa∈U(x)​{c(x,a)+∫vdP(⋅∣x,a)} is the map (2.5).
  3. Sufficiency, lower bound: under (6.6)–(6.7) and JN∗=h+NρJ^*_N = h + N\rhoJN∗​=h+Nρ, JN+1∗≥h+(N+1)ρJ^*_{N+1} \ge h + (N+1)\rhoJN+1∗​≥h+(N+1)ρ.
  4. Sufficiency, upper bound: under (6.6)–(6.7) and JN(⋅,π∗,h)=h+NρJ_N(\cdot, \pi^*, h) = h + N\rhoJN​(⋅,π∗,h)=h+Nρ, JN+1(⋅,π∗,h)=h+(N+1)ρ≥JN+1∗J_{N+1}(\cdot, \pi^*, h) = h + (N+1)\rho \ge J^*_{N+1}JN+1​(⋅,π∗,h)=h+(N+1)ρ≥JN+1∗​.

Significance

The result. Theorem 6.2 turns a statement about every finite horizon and every history-dependent randomized policy into two pointwise equations in (ρ,h)(\rho, h)(ρ,h) and a pointwise selection condition on π∗\pi^*π∗. A canonical policy is NNN-stage optimal for every NNN with terminal cost hhh; dividing (6.4) by NNN shows that its average cost is ρ\rhoρ. In the paper this is the entry point of Theorem 6.3, which shows that a canonical policy is strong average optimal and that ρ\rhoρ is the optimal average cost, without any recurrence assumption. Equation (6.6) is the condition that makes ρ\rhoρ behave as a constant in the optimization; when ρ\rhoρ is constant it holds trivially, and Theorem 6.2 specializes to the bounded ACOE with a minimizing selector.

Formalizing it. The theorem is proved in the paper (and earlier by Yushkevich). This mission formalizes that proof on a general Borel model with history-dependent randomized policies and path measures built by the Ionescu-Tulcea theorem. Prove2Me has no formalization of the multichain coupled equations or of canonical triplets beyond finite models. The finite-horizon dynamic programming inequality of milestone 2, for policies that may use the whole history, is reusable in any finite-horizon or average-cost development on Borel spaces.

Difficulty

The algebra in the proof takes a few lines. The work is in two probabilistic facts that the paper uses without comment.

The first is the Markov decomposition of the (N+1)(N+1)(N+1)-stage cost: conditioning on the first state–action pair turns the remaining NNN stages into an NNN-stage problem started from the next state. For a stationary policy the continuation is the same policy. For a history-dependent policy, the continuation is a policy that depends measurably on (x0,a0)(x_0, a_0)(x0​,a0​). Expressing this on the Ionescu-Tulcea measure is where the effort goes.

The second is the identity JN+1∗=T(JN∗)J^*_{N+1} = T(J^*_N)JN+1∗​=T(JN∗​). On a Borel model, JN∗J^*_NJN∗​ need not be measurable and the infimum need not be attained by a measurable selector. That is why the paper usually works with semicontinuous models (p. 288). Theorem 6.2 avoids the issue: only the inequality JN+1∗≥T(JN∗)J^*_{N+1} \ge T(J^*_N)JN+1∗​≥T(JN∗​) is needed, under the measurability that JN∗=h+NρJ^*_N = h + N\rhoJN∗​=h+Nρ supplies, and the reverse direction is supplied by the given π∗\pi^*π∗. A first attempt that proves the full identity JN+1∗=T(JN∗)J^*_{N+1} = T(J^*_N)JN+1∗​=T(JN∗​) for general Borel models runs into measurable selection problems that the theorem never needs.

Formalization scope

  • Model. BorelCMP S A has standard Borel S and Borel A, compact nonempty U x with measurable graph, a measurable cost c : S × A → ℝ with c ≥ 0 on K, and a Markov kernel P. c and P are total on S × A; only values on K enter. No continuity of c or P is assumed: Theorem 6.2 does not use Assumptions 2.2, 2.3 or 6.1.
  • Policies. Policy M is the paper's Π\PiΠ: history-dependent, randomized, with admissibility πt(U(xt)c∣ht)=0\pi_t(U(x_t)^c \mid h_t) = 0πt​(U(xt​)c∣ht​)=0. StationaryPolicy M is ΠSD\Pi_{SD}ΠSD​ (measurable fff with f(x)∈U(x)f(x) \in U(x)f(x)∈U(x)). The infimum JN∗J^*_NJN∗​ ranges over all of Policy M. Restricting it to stationary policies would make sufficiency trivial and necessity false, and is not what the paper states.
  • Costs. JN(x,π,h)J_N(x, \pi, h)JN​(x,π,h) is a Bochner integral against the path measure. Every statement assumes ccc bounded on K\mathbf KK and hhh bounded measurable, so the integral is a genuine expectation. JN∗J^*_NJN∗​ is a real infimum, which is the true infimum because the family is bounded below by −sup⁡∣h∣-\sup|h|−sup∣h∣ and nonempty whenever a stationary policy is given.
  • Coupled equations. (6.6) and (6.7) with "π∗(x)\pi^*(x)π∗(x) attains the infimum" are encoded in attained form: equality at a=π∗(x)a = \pi^*(x)a=π∗(x) and the inequality for every a∈U(x)a \in U(x)a∈U(x). This is equivalent to the printed condition and never forms a real infimum.
  • The gain is a function. ρ\rhoρ is a function of the state, not a constant. Specializing to a constant ρ\rhoρ (the unichain case) would trivialize (6.6) and is not the theorem.
  • Explicit choices. The paper's induction from N−1N-1N−1 to NNN is stated from NNN to N+1N+1N+1, so that no natural-number subtraction appears. Milestone 2 takes the measurability and boundedness of JN∗(⋅,h)J^*_N(\cdot, h)JN∗​(⋅,h) as a hypothesis, and takes any pointwise lower bound www of T(JN∗)T(J^*_N)T(JN∗​) in place of the infimum. In the second display of the sufficiency part, the paper prints JN−1∗(y,π∗,h)J^*_{N-1}(y, \pi^*, h)JN−1∗​(y,π∗,h); the quantity meant is JN−1(y,π∗,h)J_{N-1}(y, \pi^*, h)JN−1​(y,π∗,h), which milestone 4 uses.
  • Infrastructure. A complete development needs the Markov property of Kernel.trajMeasure at the first step, the shifted (continuation) policy and its measurability in the first state–action pair, and bounded-convergence bookkeeping for the Bochner integrals. These are reusable for every finite-horizon statement on this model. Proofs of the milestones are welcome independently. So are alternative proofs of the goal that bypass milestone 2 and argue directly with the canonical policy.

Selected references

  • A. Arapostathis, V. S. Borkar, E. Fernández-Gaucherand, M. K. Ghosh, S. I. Marcus, Discrete-time controlled Markov processes with average cost criterion: a survey, SIAM J. Control Optim. 31(2) (1993), 282–344, §6.1, Theorem 6.2. https://doi.org/10.1137/0331018
  • A. A. Yushkevich, On a class of strategies in general Markov decision models, Theory Probab. Appl. 18 (1973), 777–779.
  • E. B. Dynkin, A. A. Yushkevich, Controlled Markov Processes, Springer-Verlag, New York, 1979.
  • R. A. Howard, Dynamic Programming and Markov Processes, MIT Press, Cambridge, MA, 1960, pp. 61–62.
  • E. V. Denardo, B. L. Fox, Multichain Markov renewal programs, SIAM J. Appl. Math. 16 (1968), 468–487.
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Dynamic ProgrammingOperations ResearchProbability+1·Captain: mikedeng1

Stochastic Optimal Control: The Discrete-Time Case VIII: The Infinite-Horizon Borel Models — the Optimality Equation J* = T(J*) under (P), (N), (D)Textbook

Motivation

Infinite horizon dynamic programming asks for the least expected cost of controlling a stochastic system forever, and for a policy attaining it. On finite or countable state spaces the theory has been classical since Bellman, Blackwell (1965) and Strauch (1966). Many models in operations research, inventory control, queueing and economics have continuous states and controls, however, and there the Bellman equation raises a question the countable theory never meets: the optimal cost need not be Borel-measurable, so its expectation under the transition law, which the equation requires, may not be defined.

Bertsekas and Shreve (1978) settled this question by working with lower semianalytic cost functions and universally measurable policies. In that framework the optimal cost is always measurable enough to be integrated, and the optimality equation holds with no continuity or compactness assumption. Chapter 9 of their book treats the infinite horizon model under the three classical cost structures: nonnegative costs (P), nonpositive costs (N), and bounded discounted costs (D).

Timeline:

  • 1965: Blackwell, discounted dynamic programming on Borel spaces with Borel-measurable data, case (D).
  • 1966: Strauch, negative dynamic programming, case (N), with Borel-measurable data.
  • 1978: Bertsekas and Shreve, Chapter 9: lower semianalytic costs and universally measurable policies, in all three cases (P), (N), (D).
  • 1979: Shreve and Bertsekas, the journal account of universally measurable policies.

Setting

An infinite horizon stochastic optimal control model (SM) is an eight-tuple (S,C,U,W,p,f,α,g)(S, C, U, W, p, f, \alpha, g)(S,C,U,W,p,f,α,g). The state space SSS, the control space CCC and the disturbance space WWW are nonempty Borel spaces, that is, spaces homeomorphic to Borel subsets of complete separable metric spaces. The control constraint UUU assigns to each state xxx a nonempty set U(x)⊆CU(x) \subseteq CU(x)⊆C, and the set Γ={(x,u)∣u∈U(x)}\Gamma = \{(x,u) \mid u \in U(x)\}Γ={(x,u)∣u∈U(x)} is analytic. The disturbance kernel p(dw∣x,u)p(dw \mid x, u)p(dw∣x,u) is a Borel stochastic kernel and the system function f:SCW→Sf : SCW \to Sf:SCW→S is Borel. The discount factor is α>0\alpha > 0α>0, and the one-stage cost g:Γ→[−∞,∞]g : \Gamma \to [-\infty, \infty]g:Γ→[−∞,∞] is lower semianalytic: each sublevel set {g<c}\{g < c\}{g<c} is analytic. The state moves by xk+1=f(xk,uk,wk)x_{k+1} = f(x_k, u_k, w_k)xk+1​=f(xk​,uk​,wk​), with transition kernel t(B∣x,u)=p({w∣f(x,u,w)∈B}∣x,u)t(B \mid x, u) = p(\{w \mid f(x,u,w) \in B\} \mid x, u)t(B∣x,u)=p({w∣f(x,u,w)∈B}∣x,u).

A policy π=(μ0,μ1,… )\pi = (\mu_0, \mu_1, \dots)π=(μ0​,μ1​,…) chooses uku_kuk​ at random from a universally measurable stochastic kernel μk(duk∣x0,u0,…,xk)\mu_k(du_k \mid x_0, u_0, \dots, x_k)μk​(duk​∣x0​,u0​,…,xk​) concentrated on U(xk)U(x_k)U(xk​); Π′\Pi'Π′ is the set of all policies. A policy is Markov if each μk\mu_kμk​ depends only on xkx_kxk​, and it is stationary if, moreover, μk=μ\mu_k = \muμk​=μ for all kkk. Writing qk(π,px)q_k(\pi, p_x)qk​(π,px​) for the law of (xk,uk)(x_k, u_k)(xk​,uk​) started from x0=xx_0 = xx0​=x, the cost of π\piπ and the optimal cost are

Jπ(x)=∑k=0∞αk∫g dqk(π,px),J∗(x)=inf⁡π∈Π′Jπ(x).J_\pi(x) = \sum_{k=0}^\infty \alpha^k \int g\, dq_k(\pi, p_x), \qquad J^*(x) = \inf_{\pi \in \Pi'} J_\pi(x).Jπ​(x)=k=0∑∞​αk∫gdqk​(π,px​),J∗(x)=π∈Π′inf​Jπ​(x).

For J:S→[−∞,∞]J : S \to [-\infty, \infty]J:S→[−∞,∞], the dynamic programming operators are

T(J)(x)=inf⁡u∈U(x){g(x,u)+α∫SJ(x′) t(dx′∣x,u)},Tμ(J)(x)=∫C[g(x,u)+α∫SJ dt]μ(du∣x).T(J)(x) = \inf_{u \in U(x)} \Big\{ g(x,u) + \alpha \int_S J(x')\, t(dx' \mid x, u) \Big\}, \qquad T_\mu(J)(x) = \int_C \Big[ g(x,u) + \alpha \int_S J\, dt \Big] \mu(du \mid x).T(J)(x)=u∈U(x)inf​{g(x,u)+α∫S​J(x′)t(dx′∣x,u)},Tμ​(J)(x)=∫C​[g(x,u)+α∫S​Jdt]μ(du∣x).

The three cases are (P) g≥0g \ge 0g≥0 on Γ\GammaΓ; (N) g≤0g \le 0g≤0 on Γ\GammaΓ; (D) α<1\alpha < 1α<1 and ∣g∣≤b|g| \le b∣g∣≤b on Γ\GammaΓ for some real bbb.

Formalization targets

Goal: the optimality equation (Proposition 9.8, Eq. (22))

Under each of (P), (N) and (D),

J∗=T(J∗).J^* = T(J^*).J∗=T(J∗).

Milestones

  • J∗J^*J∗ is lower semianalytic (Corollary 9.4.1).
  • For a stationary policy, Jμ=Tμ(Jμ)J_\mu = T_\mu(J_\mu)Jμ​=Tμ​(Jμ​) (Proposition 9.9).
  • Optimality tests for stationary policies: under (P) or (D), (μ,μ,… )(\mu, \mu, \dots)(μ,μ,…) is optimal iff J∗=Tμ(J∗)J^* = T_\mu(J^*)J∗=Tμ​(J∗) (Proposition 9.12); under (N) or (D), iff Jμ=T(Jμ)J_\mu = T(J_\mu)Jμ​=T(Jμ​) (Proposition 9.13).
  • Under (N) or (D), value iteration from 000 converges to J∗J^*J∗, and under (D) it converges uniformly from every bounded lower semianalytic start (Proposition 9.14).

Further statements of the mission

  • Markov policies suffice: at each state some Markov policy matches any policy's cost (Proposition 9.1), so J∗=inf⁡π∈ΠJπJ^* = \inf_{\pi \in \Pi} J_\piJ∗=infπ∈Π​Jπ​ (Corollary 9.1.1).
  • Partial converses of the optimality equation: J≥T(J)J \ge T(J)J≥T(J), J≥0J \ge 0J≥0 gives J≥J∗J \ge J^*J≥J∗ under (P); J≤T(J)J \le T(J)J≤T(J), J≤0J \le 0J≤0 gives J≤J∗J \le J^*J≤J∗ under (N); a bounded solution of J=T(J)J = T(J)J=T(J) equals J∗J^*J∗ under (D) (Proposition 9.10). The analogous statements for TμT_\muTμ​ and JμJ_\muJμ​ (Proposition 9.11).

Significance

The optimality equation is the basic structural fact of infinite horizon control. Corollary 9.12.1 uses it to construct optimal stationary policies from minimizers in the equation. The existence results for ε\varepsilonε-optimal policies (Propositions 9.19 and 9.20), the convergence analysis of value iteration in Section 9.5, and the reduction of imperfect state information problems in Chapter 10 all build on it. It holds for arbitrary Borel models, with no continuity or compactness assumption.

All results of the mission were proved in 1978. None of them has a machine-checked proof: Mathlib has stochastic kernels and the Ionescu-Tulcea construction for measurable kernels, but no theory of lower semianalytic functions, universally measurable kernels, or dynamic programming on Borel spaces. A formal development would fix the measurability bookkeeping on which the textbook proofs rest and supply a reusable substrate for the stochastic control papers that cite this book.

Difficulty

Under (D), TTT is a contraction on bounded functions, and its fixed point is the limit of value iteration. That argument, however, gives a fixed point only within a fixed class of measurable functions. Showing that this fixed point equals J∗J^*J∗ requires knowing that J∗J^*J∗ belongs to the class and that history-dependent randomized policies do no better. Under (P), value iteration can converge to the wrong limit (Example 1 of the chapter: lim⁡kJk(0)=0\lim_k J_k(0) = 0limk​Jk​(0)=0 while J∗(0)=∞J^*(0) = \inftyJ∗(0)=∞). Even when each JkJ_kJk​ is Borel, J∗J^*J∗ may fail to be (Example 2). So J∗=T(J∗)J^* = T(J^*)J∗=T(J∗) cannot be obtained as a limit of the finite horizon equations, and the natural class of Borel functions is not closed under the partial minimization that defines TTT.

The book's route lifts (SM) to a deterministic model on the space of probability measures P(S)P(S)P(S), where no measurability restriction is needed, and transfers the results back. Making this transfer rigorous requires that the cost of a randomized policy be a measurable functional of its law, and that the infimum over policies preserve lower semianalyticity.

Formalization scope

The draft fixes the following conventions.

  • Spaces. Borel spaces are topological spaces homeomorphic to Borel subsets of complete separable metric spaces, carrying their Borel σ\sigmaσ-algebras. Analytic sets are Mathlib's AnalyticSet. A set is universally measurable if it is null-measurable for every probability measure.
  • Extended reals. Values lie in EReal. The book's convention ∞−∞=−∞+∞=∞\infty - \infty = -\infty + \infty = \infty∞−∞=−∞+∞=∞ is implemented explicitly, because Mathlib's EReal sets ⊥+⊤=⊥\bot + \top = \bot⊥+⊤=⊥. The integral of an extended-real function is ∫f+−∫f−\int f^+ - \int f^-∫f+−∫f− with the same convention.
  • Policies. These are sequences of universally measurable stochastic kernels on the history spaces S0C0⋯SkS_0C_0 \cdots S_kS0​C0​⋯Sk​, charging U(xk)U(x_k)U(xk​) with mass one. The laws of (x0,u0,…,xk,uk)(x_0, u_0, \dots, x_k, u_k)(x0​,u0​,…,xk​,uk​) are built recursively from the kernels.
  • Costs. JπJ_\piJπ​ is the series ∑kαk∫g dqk\sum_k \alpha^k \int g\, dq_k∑k​αk∫gdqk​, computed as the difference of the series of positive and negative parts. Under each of (P), (N), (D) it coincides with the integral of the total discounted cost. J∗J^*J∗ is the infimum over all policies.
  • Case labels. Each statement carries the case labels the book attaches to it, as hypotheses on the model.
  • Scope. Only the (SM) statements are formalized. The deterministic model (DM) on P(S)P(S)P(S) is the book's proof device and enters no statement.

The goal admits a trivializing formalization that this draft rules out. J∗J^*J∗ is not defined as a fixed point of TTT, nor as the limit of Tk(0)T^k(0)Tk(0); it is the infimum of the costs of all policies, which under (P) can differ from that limit.

A complete development needs universally measurable kernels and their compositions on product spaces, measurability of x↦∫f(x,y) q(dy∣x)x \mapsto \int f(x, y)\, q(dy \mid x)x↦∫f(x,y)q(dy∣x) for universally measurable integrands, the measurable selection theorem of Jankov and von Neumann, and the closure of lower semianalytic functions under partial infimum. These are the subject of the series' mission on Chapter 7, and they are reusable for any stochastic control model on Borel spaces. Contributions are welcome at any level: these foundations, the Markov reduction (Proposition 9.1), or the case-by-case arguments.

Selected references

  • D. P. Bertsekas and S. E. Shreve, Stochastic Optimal Control: The Discrete-Time Case, Academic Press, 1978; Athena Scientific reprint, 1996. Chapter 9. https://web.mit.edu/dimitrib/www/soc.html
  • D. Blackwell, Discounted dynamic programming, Annals of Mathematical Statistics 36 (1965), 226–235. https://doi.org/10.1214/aoms/1177700285
  • R. E. Strauch, Negative dynamic programming, Annals of Mathematical Statistics 37 (1966), 871–890. https://doi.org/10.1214/aoms/1177699369
  • S. E. Shreve and D. P. Bertsekas, Universally measurable policies in dynamic programming, Mathematics of Operations Research 4 (1979), 15–30. https://doi.org/10.1287/moor.4.1.15
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Calculus of VariationsOptimization·Captain: mikedeng1

On the Variational Principle III: Every Terminal-Cost Control Problem Has ε-Optimal Measurable Controls Satisfying the Pontryagin Maximum Principle up to εResearch Paper

Motivation

The Pontryagin maximum principle is the basic first-order necessary condition of optimal control: along an optimal control, the control value at almost every time extremizes a Hamiltonian built from the dynamics and an adjoint vector. The classical statement presupposes that an optimal control exists. For many problems none does: the set of trajectories is not closed, or the cost does not attain its infimum, and the classical principle then says nothing.

Ekeland's 1974 paper On the Variational Principle (DOI 10.1016/0022-247X(74)90025-0) proves a general result about lower semicontinuous functions on complete metric spaces (its Theorem 1.1, now called Ekeland's variational principle) and closes with an application to control theory in §7 (pp. 348–351): for every terminal-cost problem satisfying mild regularity and growth conditions, there are ε-optimal controls that satisfy the maximum principle up to ε, whether or not an optimal control exists. The argument equips the measurable controls with the metric "measure of the set where two controls differ", which has since become a standard device in nonsmooth and approximate optimal control. For the classical theory, Ekeland refers to the treatise of Pallu de la Barrière (Optimal Control Theory, Saunders, 1967).

Setting

Fix n≥0n \ge 0n≥0, a horizon T>0T > 0T>0, an initial state x0∈Rnx_0 \in \mathbb R^nx0​∈Rn, and a nonempty compact metrizable space KKK of control values, with its Borel σ-algebra. A control is a measurable map u:[0,T]→Ku : [0, T] \to Ku:[0,T]→K. The dynamics are a map f:Rn×K×[0,T]→Rnf : \mathbb R^n \times K \times [0, T] \to \mathbb R^nf:Rn×K×[0,T]→Rn, and the state obeys

dxdt(t)=f(x(t),u(t),t)  a.e.,x(0)=x0.(7.1)\frac{dx}{dt}(t) = f(x(t), u(t), t) \ \text{ a.e.}, \qquad x(0) = x_0. \qquad (7.1)dtdx​(t)=f(x(t),u(t),t)  a.e.,x(0)=x0​.(7.1)

A trajectory of uuu (Lean: IsTrajectory f x₀ T u x) is a function xxx continuous on [0,T][0, T][0,T] with x(t)=x0+∫0tf(x(s),u(s),s) dsx(t) = x_0 + \int_0^t f(x(s), u(s), s)\,dsx(t)=x0​+∫0t​f(x(s),u(s),s)ds for all t∈[0,T]t \in [0, T]t∈[0,T]. The standing hypotheses are:

  • (a) fff and its state Jacobian fx′=(∂f/∂x1,…,∂f/∂xn)f_x' = (\partial f/\partial x_1, \dots, \partial f/\partial x_n)fx′​=(∂f/∂x1​,…,∂f/∂xn​) (Lean: fx) are continuous on Rn×K×[0,T]\mathbb R^n \times K \times [0, T]Rn×K×[0,T];
  • (b) ⟨x,f(x,u,t)⟩≤c (1+∥x∥2)\langle x, f(x, u, t)\rangle \le c\,(1 + \|x\|^2)⟨x,f(x,u,t)⟩≤c(1+∥x∥2) for some constant ccc.

The terminal cost is given by a C1C^1C1 function g:Rn→Rg : \mathbb R^n \to \mathbb Rg:Rn→R, and the problem is to minimize g(x(T))g(x(T))g(x(T)) over all controls. The adjoint vector ppp along a pair (u,x)(u, x)(u,x) (Lean: IsAdjoint fx g T u x p) solves the linear equation

dpdt(t)=−tfx′(x(t),u(t),t) p(t),p(T)=g′(x(T)),\frac{dp}{dt}(t) = -{}^t f_x'(x(t), u(t), t)\, p(t), \qquad p(T) = g'(x(T)),dtdp​(t)=−tfx′​(x(t),u(t),t)p(t),p(T)=g′(x(T)),

where tA{}^t AtA is the transpose. The control distance (Lean: ctrlDist T u₁ u₂) is

δ(u1,u2)=meas⁡{t∈[0,T]∣u1(t)≠u2(t)},\delta(u_1, u_2) = \operatorname{meas}\{t \in [0, T] \mid u_1(t) \neq u_2(t)\},δ(u1​,u2​)=meas{t∈[0,T]∣u1​(t)=u2​(t)},

and the needle variation vτv_\tauvτ​ of a control uεu_\varepsilonuε​ at t0t_0t0​ with value u0∈Ku_0 \in Ku0​∈K (Lean: needle T uε u₀ t₀ τ) equals u0u_0u0​ on [0,T]∩ ]t0−τ,t0[[0, T] \cap\, ]t_0 - \tau, t_0[[0,T]∩]t0​−τ,t0​[ and uεu_\varepsilonuε​ elsewhere.

Formalization targets

Goal: Theorem 7.1

For every ε>0\varepsilon > 0ε>0 there is a control uεu_\varepsilonuε​ with trajectory xεx_\varepsilonxε​ and adjoint vector pεp_\varepsilonpε​ such that

g(xε(T))≤inf⁡ug(x(T))+ε,⟨f(xε(t),uε(t),t),pε(t)⟩≤min⁡w∈K⟨f(xε(t),w,t),pε(t)⟩+ε  a.e. on [0,T].g(x_\varepsilon(T)) \le \inf_u g(x(T)) + \varepsilon, \qquad \langle f(x_\varepsilon(t), u_\varepsilon(t), t), p_\varepsilon(t)\rangle \le \min_{w \in K} \langle f(x_\varepsilon(t), w, t), p_\varepsilon(t)\rangle + \varepsilon \ \text{ a.e. on } [0, T].g(xε​(T))≤uinf​g(x(T))+ε,⟨f(xε​(t),uε​(t),t),pε​(t)⟩≤w∈Kmin​⟨f(xε​(t),w,t),pε​(t)⟩+ε  a.e. on [0,T].

Milestones

  1. (7.2), a priori bound: every trajectory satisfies ∥x(t)∥2≤(∥x0∥2+2cT)e2cT\|x(t)\|^2 \le (\|x_0\|^2 + 2cT)e^{2cT}∥x(t)∥2≤(∥x0​∥2+2cT)e2cT.
  2. Well-posedness (p. 348): every control has exactly one trajectory on [0,T][0, T][0,T].
  3. Lemma 7.2: (U,δ)(\mathcal U, \delta)(U,δ) is a complete metric space (on almost-everywhere classes).
  4. Lemma 7.3: u↦g(x(T))u \mapsto g(x(T))u↦g(x(T)) is continuous on (U,δ)(\mathcal U, \delta)(U,δ).
  5. (7.15)–(7.16): a control uεu_\varepsilonuε​ with F(uε)≤inf⁡F+ε2F(u_\varepsilon) \le \inf F + \varepsilon^2F(uε​)≤infF+ε2 and F(u)≥F(uε)−ε δ(u,uε)F(u) \ge F(u_\varepsilon) - \varepsilon\,\delta(u, u_\varepsilon)F(u)≥F(uε​)−εδ(u,uε​) for all uuu, where F(u)=g(x(T))F(u) = g(x(T))F(u)=g(x(T)).
  6. Lemma 7.4: the right derivative of τ↦g(xτ(T))\tau \mapsto g(x_\tau(T))τ↦g(xτ​(T)) at τ=0\tau = 0τ=0, for the needle variations vτv_\tauvτ​, equals ⟨f(xε(t0),u0,t0)−f(xε(t0),uε(t0),t0),pε(t0)⟩\langle f(x_\varepsilon(t_0), u_0, t_0) - f(x_\varepsilon(t_0), u_\varepsilon(t_0), t_0), p_\varepsilon(t_0)\rangle⟨f(xε​(t0​),u0​,t0​)−f(xε​(t0​),uε​(t0​),t0​),pε​(t0​)⟩.

Significance

The result. Theorem 7.1 decouples the maximum principle from existence of optimal controls. Any minimizing sequence can be replaced by one consisting of controls that satisfy the necessary condition up to a vanishing error, so approximate extremals are available for numerical schemes and for limiting arguments (relaxation, convergence of extremals) in problems without compactness or convexity of the velocity sets. The same scheme, a complete metric on controls plus Ekeland's principle plus needle variations, underlies later proofs of the maximum principle with state constraints and in nonsmooth settings.

Formalizing it. The theorem has a published proof, which the paper sketches in four pages and partly defers to classical results (local existence for measurable controls, differentiability of trajectories with respect to needle variations). Neither Mathlib nor the platform contains this theorem or a maximum principle for measurable controls with time-dependent dynamics; the nearest platform items assume an exact optimum, a running cost and globally Lipschitz autonomous dynamics. A formalization requires a Carathéodory theory of ODEs in Lean, the complete metric space of controls, and a rigorous version of the classical first-variation computation. Each of these is useful well beyond this paper.

Difficulty

The obvious argument fails at its first step: a minimizing sequence of controls has no convergent subsequence in any useful sense, because measurable controls with values in KKK are not compact in the metric δ\deltaδ and their weak limits are relaxed controls, which are not controls. Ekeland's principle avoids compactness, but it needs a complete metric space on which the cost is lower semicontinuous. Completeness of (U,δ)(\mathcal U, \delta)(U,δ) (Lemma 7.2) and continuity of the cost (Lemma 7.3) both require care. Continuity must hold for trajectories driven by merely measurable controls, which converge only in measure. The needle derivative (Lemma 7.4) holds only at times where the trajectory satisfies the state equation in the classical sense, which is almost every time but not every time.

Formalization scope

  • Controls are functions ℝ → K with Measurable u; only values on [0,T][0, T][0,T] matter. Trajectories and adjoint vectors are functions ℝ → EuclideanSpace ℝ (Fin n), continuous on [0,T][0, T][0,T] and solving the integral form of their equation. The paper uses the same form in (7.13). A definition that asks for a derivative at every time would be unsatisfiable for discontinuous controls and would make the goal vacuous; the integral form avoids this.
  • Hypothesis (a) is stated as joint continuity of f and fx on univ ×ˢ univ ×ˢ Icc 0 T together with HasFDerivAt (fun y => f y u t) (fx x u t) x. Hypothesis (b) is ∃ c, … with the order of arguments f(x,u,t)f(x, u, t)f(x,u,t); the page prints f(t,x,u)f(t, x, u)f(t,x,u) in (b), a slip.
  • The transpose tfx′{}^t f_x'tfx′​ is ContinuousLinearMap.adjoint, and g′(x)g'(x)g′(x) is gradient g x.
  • Infima over controls are never taken as real ⨅; (7.4) and (7.15) are stated as "for every control uuu with trajectory xxx".
  • (7.5) is printed with "× ε\times\,\varepsilon×ε". The proof's last line (7.21) gives "+ ε+\,\varepsilon+ε", which is what is stated. The minimum over the compact KKK is replaced by the equivalent "for every w∈Kw \in Kw∈K", with one null set for all www.
  • Added hypothesis: [Nonempty K] in the goal and milestone 5. With KKK empty no control exists and the existential statements would be false.
  • Lemma 7.2 is stated as the triangle inequality, "δ=0\delta = 0δ=0 iff almost-everywhere equality on [0,T][0, T][0,T]", and sequential completeness for measurable controls. Lemma 7.3 is sequential continuity. Lemma 7.4 is a one-sided derivative within [0,t0][0, t_0][0,t0​] at 000, stated for an arbitrary measurable uεu_\varepsilonuε​.
  • Theorem 1.1 (Ekeland's principle) is a separate mission of this series and still a draft, so milestone 5 states the instance used here directly.
  • Out of scope: the uniform bound (7.3) and the remark after Theorem 7.1 that one may take ε=0\varepsilon = 0ε=0 in (7.5) when (7.4) holds with ε=0\varepsilon = 0ε=0.

Welcome contributions include Carathéodory existence and uniqueness for ODEs with measurable time dependence, Gronwall-type estimates for absolutely continuous functions, the complete metric space of measurable maps under the disagreement measure, and differentiability of flows with respect to initial data.

Selected references

  • I. Ekeland, On the Variational Principle, J. Math. Anal. Appl. 47 (1974), 324–353. https://doi.org/10.1016/0022-247X(74)90025-0
  • I. Ekeland, Nonconvex minimization problems, Bull. Amer. Math. Soc. (N.S.) 1 (1979), 443–474. https://doi.org/10.1090/S0273-0979-1979-14595-6
  • R. Pallu de la Barrière, Optimal Control Theory, Saunders, Philadelphia, 1967.
  • L. S. Pontryagin, V. G. Boltyanskii, R. V. Gamkrelidze, E. F. Mishchenko, The Mathematical Theory of Optimal Processes, Interscience, New York, 1962.
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Dynamic Scheduling of a System with Two Parallel Servers in Heavy Traffic with Resource Pooling: The Threshold Policy Is Asymptotically OptimalResearch Paper

Motivation

Many service systems route several classes of work to servers with overlapping skills: call centers with cross-trained agents, manufacturing cells with flexible machines, computing clusters with heterogeneous processors. Choosing which server works on which class at each moment is a dynamic scheduling problem. Exact optimal policies are out of reach except in toy cases, so heavy-traffic theory replaces the queueing system by a Brownian control problem, solves that limit problem, and then asks for a policy in the original system whose performance converges to the Brownian optimum. This programme was proposed by Harrison (Harrison 1988), and the parallel server system studied here is the example Harrison used (Harrison, Ann. Appl. Probab. 1998) to show that the greedy static priority rule can be very inefficient.

Bell and Williams (2001) gave the first proof of asymptotic optimality of a continuous-review policy for this system, with renewal arrivals and general service times. Harrison (1998) had treated Poisson arrivals and deterministic service times with a discrete-review policy and a pathwise criterion. Harrison and López (Queueing Systems, 1999) identified the complete resource pooling condition for general parallel server systems. The threshold policy and the proof method of Bell and Williams were later extended to multiserver systems (Bell and Williams, Electron. J. Probab., 2005).

Setting

There are two job classes and two servers. Server 1 serves class 1 (activity 1); server 2 serves class 1 (activity 2) and class 2 (activity 3). A sequence of such systems is indexed by r→∞r\to\inftyr→∞. On a probability space, i.i.d. sequences uˇk(i)\check u_k(i)uˇk​(i) (k=1,2k=1,2k=1,2) and vˇj(i)\check v_j(i)vˇj​(i) (j=1,2,3j=1,2,3j=1,2,3), i≥1i\ge1i≥1, are fixed: strictly positive, mutually independent, with mean one and finite variances αk2,βj2\alpha_k^2,\beta_j^2αk2​,βj2​. In system rrr the interarrival times are ukr(i)=uˇk(i)/λkru_k^r(i)=\check u_k(i)/\lambda_k^rukr​(i)=uˇk​(i)/λkr​ and the service times are vjr(i)=vˇj(i)/μjrv_j^r(i)=\check v_j(i)/\mu_j^rvjr​(i)=vˇj​(i)/μjr​. The renewal processes Akr(t)A_k^r(t)Akr​(t) and Sjr(t)S_j^r(t)Sjr​(t) count arrivals and potential service completions.

A scheduling control policy is an allocation T=(T1,T2,T3)T=(T_1,T_2,T_3)T=(T1​,T2​,T3​), where Tj(t)T_j(t)Tj​(t) is the time devoted to activity jjj in [0,t][0,t][0,t]. Each Tj(t)T_j(t)Tj​(t) is a random variable, each TjT_jTj​ is continuous and nondecreasing from 000, and so are the idle times I1=t−T1I_1=t-T_1I1​=t−T1​ and I2=t−T2−T3I_2=t-T_2-T_3I2​=t−T2​−T3​. The queue lengths

Q1(t)=A1(t)−S1(T1(t))−S2(T2(t)),Q2(t)=A2(t)−S3(T3(t))Q_1(t)=A_1(t)-S_1(T_1(t))-S_2(T_2(t)),\qquad Q_2(t)=A_2(t)-S_3(T_3(t))Q1​(t)=A1​(t)−S1​(T1​(t))−S2​(T2​(t)),Q2​(t)=A2​(t)−S3​(T3​(t))

must be nonnegative. Policies may anticipate the future. The rates satisfy Assumption 3.1: λ1>μ1\lambda_1>\mu_1λ1​>μ1​, 1−(λ1−μ1)/μ2=λ2/μ31-(\lambda_1-\mu_1)/\mu_2=\lambda_2/\mu_31−(λ1​−μ1​)/μ2​=λ2​/μ3​, and the rates converge at rate 1/r1/r1/r to limits with second-order parameters θ1,θ2\theta_1,\theta_2θ1​,θ2​. Assumption 3.2 is h1μ2≥h2μ3h_1\mu_2\ge h_2\mu_3h1​μ2​≥h2​μ3​, and Assumption 3.3 gives finite exponential moments near 000. With Q^r(t)=r−1Qr(r2t)\hat Q^r(t)=r^{-1}Q^r(r^2t)Q^​r(t)=r−1Qr(r2t) the cost is

J^r(Tr)=E(∫0∞e−γt h⋅Q^r(t) dt).\hat J^r(T^r)=\mathbf E\Big(\int_0^\infty e^{-\gamma t}\,h\cdot\hat Q^r(t)\,dt\Big).J^r(Tr)=E(∫0∞​e−γth⋅Q^​r(t)dt).

The threshold policy with Lr=[clog⁡r]L^r=[c\log r]Lr=[clogr] works as follows. Server 1 works whenever it has a class 1 job available. Server 2 serves class 1 with preemptive-resume priority when more than LrL^rLr class 1 jobs are present, and otherwise serves class 2. The Brownian benchmark is built from a two-dimensional Brownian motion X~\tilde XX~ with drift θ\thetaθ and diagonal covariance, from y=(1,μ2/μ3)y=(1,\mu_2/\mu_3)y=(1,μ2​/μ3​), and from the reflected process W~∗=y⋅X~+V~∗\tilde W^*=y\cdot\tilde X+\tilde V^*W~∗=y⋅X~+V~∗ with V~∗(t)=−inf⁡s≤ty⋅X~(s)\tilde V^*(t)=-\inf_{s\le t}y\cdot\tilde X(s)V~∗(t)=−infs≤t​y⋅X~(s). Its cost is J∗=E∫0∞e−γth2 W~∗(t)/y2 dtJ^*=\mathbf E\int_0^\infty e^{-\gamma t}h_2\,\tilde W^*(t)/y_2\,dtJ∗=E∫0∞​e−γth2​W~∗(t)/y2​dt.

Formalization targets

Goal: Theorem 5.3

For ccc larger than a constant c0c_0c0​ that depends only on the model data, and for every sequence {Tr}\{T^r\}{Tr} of scheduling control policies,

lim inf⁡r→∞J^r(Tr) ≥ J∗ = lim⁡r→∞J^r(Tr,∗),J∗<∞.\liminf_{r\to\infty}\hat J^r(T^r)\ \ge\ J^*\ =\ \lim_{r\to\infty}\hat J^r(T^{r,*}),\qquad J^*<\infty .r→∞liminf​J^r(Tr) ≥ J∗ = r→∞lim​J^r(Tr,∗),J∗<∞.

Milestones

  • Proposition B.1: the one-dimensional Skorokhod problem, its explicit solution and its minimality.
  • Appendix A, (181) and (184): Cramér-type deviation bounds for delayed renewal processes.
  • Theorem 7.2: after first reaching LrL^rLr, the class 1 queue stays within Lr−1L^r-1Lr−1 of the threshold, with probability tending to one.
  • Theorem 7.1: (Q^1r,I^1r)⇒(0,0)(\hat Q_1^r,\hat I_1^r)\Rightarrow(0,0)(Q^​1r​,I^1r​)⇒(0,0) under the threshold policy.
  • Lemma 8.1: the fluid-scaled threshold allocations converge to Tˉ∗(t)=(t,λ1−μ1μ2t,λ2μ3t)\bar T^*(t)=(t,\frac{\lambda_1-\mu_1}{\mu_2}t,\frac{\lambda_2}{\mu_3}t)Tˉ∗(t)=(t,μ2​λ1​−μ1​​t,μ3​λ2​​t).
  • Theorem 5.2 (state-space collapse): (Q^1r,Q^2r,I^1r,I^2r)⇒(0,Q~2∗,0,I~2∗)(\hat Q_1^r,\hat Q_2^r,\hat I_1^r,\hat I_2^r)\Rightarrow(0,\tilde Q_2^*,0,\tilde I_2^*)(Q^​1r​,Q^​2r​,I^1r​,I^2r​)⇒(0,Q~​2∗​,0,I~2∗​).
  • Lemma 9.3: along a subsequence achieving a finite lim inf⁡\liminfliminf cost, the fluid-scaled processes converge to (0,λt,μt,Tˉ∗,0)(0,\lambda t,\mu t,\bar T^*,0)(0,λt,μt,Tˉ∗,0).

A further draft theorem states that Definition 5.1 determines an admissible allocation, unique pathwise, whenever Lr≥1L^r\ge1Lr≥1.

Significance

The theorem proves that a simple state-dependent rule, which sends server 2 to class 1 only when the class 1 queue exceeds a logarithmic safety stock, is asymptotically optimal among all policies, including those that anticipate the future. The limiting cost is the explicit optimum of the Brownian control problem. The proof gives a template for heavy-traffic asymptotic optimality under complete resource pooling: a lower bound valid for every policy, and state-space collapse under the proposed policy. The residual process analysis of Section 7 shows how a threshold of order log⁡r\log rlogr makes starvation of server 1 negligible on the diffusion time scale.

The paper's results are proved but not machine-checked; no formal proof exists in any proof assistant. The mission asks for formal statements of the paper's main theorem and its supporting lemmas, followed by formal proofs. Parts of the development are independent of the paper: the one-dimensional Skorokhod map, renewal large deviation bounds, and convergence encodings on path space.

Difficulty

The lower bound must hold for arbitrary, possibly anticipating, policies, so no Markov structure is available. The argument has to pass through fluid limits of an arbitrary cost-minimizing subsequence and a pathwise minimality property, and Fatou's lemma for the limit needs uniform control. For the upper bound, the obvious approach, a static priority rule, is known to fail: it starves server 1 and produces a large class 1 queue. With a threshold policy, the hard step is to show that the class 1 queue, once at the threshold, rarely moves Lr−1L^r-1Lr−1 away from it over a time interval of length r2tr^2tr2t. That requires large deviation estimates for renewal processes started at random, multiparameter stopping times. Showing that J^r(Tr,∗)\hat J^r(T^{r,*})J^r(Tr,∗) converges to J∗J^*J∗, rather than only that the processes converge in distribution, also requires uniform integrability of the scaled queue lengths.

Formalization scope

Classes and activities are indexed by Fin 2 and Fin 3. The i.i.d. sequences keep the paper's index base i≥1i\ge1i≥1, and the systems are indexed by n∈Nn\in\mathbb Nn∈N with r=rn∈[1,∞)r=r_n\in[1,\infty)r=rn​∈[1,∞), rn→∞r_n\to\inftyrn​→∞. Time is real, and every condition is imposed for t≥0t\ge0t≥0. Admissibility is exactly (11)–(14). Measurability in (11) is with respect to the completion of P\mathbf PP, since the paper's space is complete. Finiteness of the renewal processes everywhere on Ω\OmegaΩ, which the paper obtains by discarding a null set, is a hypothesis. Queue lengths are real, costs are lower Lebesgue integrals in [0,∞][0,\infty][0,∞], counting processes take values in N∪{∞}\mathbb N\cup\{\infty\}N∪{∞}, and Λ\LambdaΛ, Λ∗\Lambda^*Λ∗ take values in the extended reals.

The constant c0c_0c0​ is existential and is chosen after the model data and before ccc, the policies and the Brownian motions. The threshold relations are required only for the systems with Lr≥1L^r\ge1Lr≥1, which are all but finitely many. Each convergence to a deterministic limit (Theorem 7.1, Lemmas 8.1 and 9.3) is stated as u.o.c. convergence in probability, the paper's own equivalence (p. 633). Theorem 5.2 is stated in coupling form: there are copies of the processes on one probability space, with Skorokhod paths and the same laws, that converge almost surely uniformly on compacts. This is equivalent to weak convergence in D4\mathbf D^4D4 to a limit with continuous paths. J∗J^*J∗ is defined by (44) from an arbitrary pair of independent standard Brownian motions (Mathlib's IsBrownianReal), not by a closed form.

Two formalizations would make the goal trivial, and both are excluded. Leaving out the requirement that Tr,∗T^{r,*}Tr,∗ actually follow the policy would make the goal false or empty. Narrowing the class of competing policies, for example to non-anticipating ones, would weaken the theorem. A draft theorem also states that the threshold allocation exists and is unique pathwise, so the hypothesis on Tr,∗T^{r,*}Tr,∗ can be satisfied.

The development needs renewal theory (functional central limit theorems, Cramér bounds), multiparameter stopping times, tightness in D\mathbf DD, the Skorokhod representation theorem, the reflection map, and properties of reflected Brownian motion. Contributions are welcome at every level: proofs of milestones, reusable lemmas on renewal processes and the Skorokhod map, and further lemmas of the paper (Lemmas 7.5, 7.6 and 9.2 are not yet stated).

Selected references

  • S. L. Bell and R. J. Williams, Dynamic scheduling of a system with two parallel servers in heavy traffic with resource pooling: asymptotic optimality of a threshold policy, Ann. Appl. Probab. 11 (2001) 608–649. https://doi.org/10.1214/aoap/1015345343
  • J. M. Harrison, Heavy traffic analysis of a system with parallel servers: asymptotic optimality of discrete-review policies, Ann. Appl. Probab. 8 (1998) 822–848.
  • J. M. Harrison and M. J. López, Heavy traffic resource pooling in parallel-server systems, Queueing Systems 33 (1999) 339–368.
  • J. M. Harrison, Brownian models of queueing networks with heterogeneous customer populations, in Stochastic Differential Systems, Stochastic Control Theory and Their Applications, Springer (1988) 147–186.
  • S. L. Bell and R. J. Williams, Dynamic scheduling of a parallel server system in heavy traffic with complete resource pooling: asymptotic optimality of a threshold policy, Electron. J. Probab. 10 (2005) 1044–1115.
  • J. M. Harrison, Brownian Motion and Stochastic Flow Systems, Wiley (1985).
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Mathematical PhysicsOptimizationPartial Differential Equations+2·Captain: mikedeng1

Optimization of Mean-field Spin Glasses III: The Lagrangian Value of the Stochastic Control Problem Equals the Parisi FunctionalResearch Paper

Motivation

The ground-state energy of a mixed ppp-spin spin glass, OPTN=max⁡σ∈{±1}NHN(σ)/N\mathsf{OPT}_N=\max_{\sigma\in\{\pm1\}^N}H_N(\sigma)/NOPTN​=maxσ∈{±1}N​HN​(σ)/N, converges almost surely to the infimum of the Parisi functional over non-decreasing order parameters (Auffinger–Chen 2017). El Alaoui, Montanari and Sellke (arXiv:2001.00904v1) study algorithms that find near-optimal configurations. They introduce incremental approximate message passing (IAMP) and show that, among a broad class of such algorithms, the best achievable energy is the infimum of the Parisi functional over a larger space of order parameters (their Theorem 4).

The upper bound in Theorem 4 is reduced, in Section 4 of the paper, to a stochastic optimal control problem. The energy reached by a message-passing algorithm becomes the objective of a control problem driven by a Brownian motion, with a terminal constraint and a variance constraint. The variance constraint is removed by a Lagrange multiplier 12ξ′′γ\tfrac12\xi''\gamma21​ξ′′γ. Proposition 4.1 states that the resulting Lagrangian value is exactly the Parisi functional P(γ)\mathsf P(\gamma)P(γ). This mission formalizes that duality and the verification argument behind it (Section 7).

Setting

Mixture. Real coefficients (ck)k≥2(c_k)_{k\ge2}(ck​)k≥2​ define the mixture ξ(t)=∑k≥2ck2tk\xi(t)=\sum_{k\ge2}c_k^2t^kξ(t)=∑k≥2​ck2​tk, with the standing assumption ξ(1+ε)<∞\xi(1+\varepsilon)<\inftyξ(1+ε)<∞ for some ε>0\varepsilon>0ε>0. Its derivatives ξ′\xi'ξ′, ξ′′\xi''ξ′′ are nonnegative and nondecreasing on [0,1][0,1][0,1].

Order parameters. SF+\mathsf{SF}_+SF+​ is the set of nonnegative step functions

γ=∑i=1mγi I[ti−1,ti),0=t0<t1<⋯<tm=1, γi≥0.\gamma=\sum_{i=1}^m\gamma_i\,\mathbb I_{[t_{i-1},t_i)},\qquad 0=t_0<t_1<\dots<t_m=1,\ \gamma_i\ge0 .γ=i=1∑m​γi​I[ti−1​,ti​)​,0=t0​<t1​<⋯<tm​=1, γi​≥0.

Put ν(t)=∫t1ξ′′(s)γ(s) ds\nu(t)=\int_t^1\xi''(s)\gamma(s)\,dsν(t)=∫t1​ξ′′(s)γ(s)ds.

Parisi PDE and functional. Φγ:[0,1]×R→R\Phi_\gamma:[0,1]\times\mathbb R\to\mathbb RΦγ​:[0,1]×R→R solves

∂tΦγ+12ξ′′(t)(∂x2Φγ+γ(t)(∂xΦγ)2)=0,Φγ(1,x)=∣x∣.\partial_t\Phi_\gamma+\tfrac12\xi''(t)\big(\partial_x^2\Phi_\gamma+\gamma(t)(\partial_x\Phi_\gamma)^2\big)=0,\qquad\Phi_\gamma(1,x)=|x| .∂t​Φγ​+21​ξ′′(t)(∂x2​Φγ​+γ(t)(∂x​Φγ​)2)=0,Φγ​(1,x)=∣x∣.

For γ∈SF+\gamma\in\mathsf{SF}_+γ∈SF+​ it is given explicitly by the Cole–Hopf recursion: with r(t)=ξ′(1)−ξ′(t)r(t)=\xi'(1)-\xi'(t)r(t)=ξ′(1)−ξ′(t) and G∼N(0,1)G\sim\mathsf N(0,1)G∼N(0,1), for t∈[ti−1,ti)t\in[t_{i-1},t_i)t∈[ti−1​,ti​),

Φγ(t,x)=1γilog⁡Eexp⁡{γiΦγ(ti,x+r(t)−r(ti) G)}.\Phi_\gamma(t,x)=\frac1{\gamma_i}\log\mathbb E\exp\big\{\gamma_i\Phi_\gamma(t_i,x+\sqrt{r(t)-r(t_i)}\,G)\big\}.Φγ​(t,x)=γi​1​logEexp{γi​Φγ​(ti​,x+r(t)−r(ti​)​G)}.

The Parisi functional is P(γ)=Φγ(0,0)−12∫01t ξ′′(t)γ(t) dt\mathsf P(\gamma)=\Phi_\gamma(0,0)-\tfrac12\int_0^1t\,\xi''(t)\gamma(t)\,dtP(γ)=Φγ​(0,0)−21​∫01​tξ′′(t)γ(t)dt.

Control problem. Let BBB be a standard Brownian motion. A control u∈D[t,1]u\in D[t,1]u∈D[t,1] is a process on [t,1][t,1][t,1], progressively measurable for the filtration of (Br)r∈[t,1](B_r)_{r\in[t,1]}(Br​)r∈[t,1]​, with E∫t1ξ′′(s)us2 ds<∞\mathbb E\int_t^1\xi''(s)u_s^2\,ds<\inftyE∫t1​ξ′′(s)us2​ds<∞. The value is

Jγ(t,z)=sup⁡u∈D[t,1]E[∫t1ξ′′(s)us ds+12∫t1ν(s)(ξ′′(s)us2−1)ds]s.t.z+∫t1ξ′′(s) us dBs∈(−1,1) a.s.\mathcal J_\gamma(t,z)=\sup_{u\in D[t,1]}\mathbb E\Big[\int_t^1\xi''(s)u_s\,ds+\frac12\int_t^1\nu(s)\big(\xi''(s)u_s^2-1\big)ds\Big]\quad\text{s.t.}\quad z+\int_t^1\sqrt{\xi''(s)}\,u_s\,dB_s\in(-1,1)\ \text{a.s.}Jγ​(t,z)=u∈D[t,1]sup​E[∫t1​ξ′′(s)us​ds+21​∫t1​ν(s)(ξ′′(s)us2​−1)ds]s.t.z+∫t1​ξ′′(s)​us​dBs​∈(−1,1) a.s.

Candidate value function. With Φγ∗(t,z)=inf⁡x{Φγ(t,x)−xz}\Phi^*_\gamma(t,z)=\inf_x\{\Phi_\gamma(t,x)-xz\}Φγ∗​(t,z)=infx​{Φγ​(t,x)−xz},

V(t,z)=Φγ∗(t,z)−12ν(t)z2−12∫t1ν(s) ds.V(t,z)=\Phi^*_\gamma(t,z)-\tfrac12\nu(t)z^2-\tfrac12\int_t^1\nu(s)\,ds .V(t,z)=Φγ∗​(t,z)−21​ν(t)z2−21​∫t1​ν(s)ds.

Formalization targets

Goal: Proposition 4.1

Jγ(0,0)=P(γ)for every γ∈SF+.\mathcal J_\gamma(0,0)=\mathsf P(\gamma)\qquad\text{for every }\gamma\in\mathsf{SF}_+ .Jγ​(0,0)=P(γ)for every γ∈SF+​.

Milestones

  1. Lemma 7.2 (a)–(e): Φγ(t,⋅)\Phi_\gamma(t,\cdot)Φγ​(t,⋅) is smooth for t<1t<1t<1, with derivatives jointly continuous on [0,1)×R[0,1)\times\mathbb R[0,1)×R and C1C^1C1 in time where γ\gammaγ is constant. The range of ∂xΦγ(t,⋅)\partial_x\Phi_\gamma(t,\cdot)∂x​Φγ​(t,⋅) is (−1,1)(-1,1)(−1,1), it is strictly increasing, and 0<∂x2Φγ(t′,x)≤C(t,γ)0<\partial_x^2\Phi_\gamma(t',x)\le C(t,\gamma)0<∂x2​Φγ​(t′,x)≤C(t,γ) for t′≤tt'\le tt′≤t.
  2. Envelope identities (proof of Lemma 7.3): ∂zΦγ∗(t,z)=−xt∗(z)\partial_z\Phi^*_\gamma(t,z)=-x^*_t(z)∂z​Φγ∗​(t,z)=−xt∗​(z) and ∂z2Φγ∗(t,z)=−1/∂x2Φγ(t,xt∗(z))\partial_z^2\Phi^*_\gamma(t,z)=-1/\partial_x^2\Phi_\gamma(t,x^*_t(z))∂z2​Φγ∗​(t,z)=−1/∂x2​Φγ​(t,xt∗​(z)), where xt∗(z)x^*_t(z)xt∗​(z) is the unique root of ∂xΦγ(t,x)=z\partial_x\Phi_\gamma(t,x)=z∂x​Φγ​(t,x)=z.
  3. Lemma 7.3: VVV solves the HJB equation
∂tV+ξ′′(t)sup⁡λ∈R{λ+λ22(ν(t)+∂z2V)}−12ν(t)=0,V(1,z)=0.\partial_tV+\xi''(t)\sup_{\lambda\in\mathbb R}\Big\{\lambda+\frac{\lambda^2}{2}\big(\nu(t)+\partial_z^2V\big)\Big\}-\frac12\nu(t)=0,\qquad V(1,z)=0 .∂t​V+ξ′′(t)λ∈Rsup​{λ+2λ2​(ν(t)+∂z2​V)}−21​ν(t)=0,V(1,z)=0.
  1. Evaluation at the origin: V(0,0)=P(γ)V(0,0)=\mathsf P(\gamma)V(0,0)=P(γ).
  2. Proposition 7.1: Jγ(t,z)=V(t,z)\mathcal J_\gamma(t,z)=V(t,z)Jγ​(t,z)=V(t,z) for all (t,z)∈[0,1]×(−1,1)(t,z)\in[0,1]\times(-1,1)(t,z)∈[0,1]×(−1,1).

Proposition 7.1 at (0,0)(0,0)(0,0) together with milestone 4 gives the goal.

Significance

The result. By integration by parts (Eq. (4.4) of the paper), Jγ(0,0)\mathcal J_\gamma(0,0)Jγ​(0,0) bounds the value of the constrained control problem (4.2). That problem in turn bounds the asymptotic energy of every message-passing algorithm in the class of Theorem 4. Proposition 4.1 turns the bound into inf⁡γ∈SF+P(γ)\inf_{\gamma\in\mathsf{SF}_+}\mathsf P(\gamma)infγ∈SF+​​P(γ), which is the analytic core of the optimality statement for IAMP. It is also an instance of a broader principle: the Parisi functional has a stochastic-control representation (Jagannath–Tobasco 2016).

Formalizing it. The result is proved in the paper; no machine-checked version exists. A complete formalization needs a verification theorem for a control problem with a state constraint (M1∈(−1,1)M_1\in(-1,1)M1​∈(−1,1)), Itô's formula for a C1,2C^{1,2}C1,2 function that is only piecewise C1C^1C1 in time, and quantitative regularity of the Cole–Hopf solution. Each of these is reusable well beyond spin glasses.

Difficulty

The value function Jγ\mathcal J_\gammaJγ​ is not known to be smooth, and the dynamic-programming equation (4.6) is only heuristic. The proof therefore guesses a solution and verifies it. Two steps carry the difficulty.

First, the guess VVV is a Legendre transform. Its regularity, and the sign ν+∂z2V<0\nu+\partial_z^2V<0ν+∂z2​V<0 that makes the HJB supremum finite, rest on strict convexity and bounded curvature of Φγ(t,⋅)\Phi_\gamma(t,\cdot)Φγ​(t,⋅) (Lemma 7.2). These must be proved by induction through the Cole–Hopf recursion, including the steps with γi=0\gamma_i=0γi​=0.

Second, the verification argument applies Itô's formula to V(s,Msu)V(s,M^u_s)V(s,Msu​), where MuM^uMu is a martingale confined to (−1,1)(-1,1)(−1,1) and VVV is only C1C^1C1 in time between the jumps of γ\gammaγ. The boundary θ→1\theta\to1θ→1 needs a dominated-convergence argument, and attaining the supremum needs an explicit optimal feedback control built from an SDE.

Formalization scope

  • Mixture. ξ\xiξ is a coefficient sequence c:N→Rc:\mathbb N\to\mathbb Rc:N→R with c0=c1=0c_0=c_1=0c0​=c1​=0 imposed. ξ′\xi'ξ′ and ξ′′\xi''ξ′′ are explicit termwise series.
  • Step functions. SF+\mathsf{SF}_+SF+​ is represented by its data (breakpoints and values). γ\gammaγ is extended by 000 outside [0,1)[0,1)[0,1); its value at t=1t=1t=1 never matters.
  • Cole–Hopf. Φγ\Phi_\gammaΦγ​ is defined by the recursion. When γi=0\gamma_i=0γi​=0, the recursion uses its limit, the heat semigroup, instead of dividing by zero. Expectations over GGG are integrals against gaussianReal 0 1.
  • Derivatives. Space derivatives are deriv/iteratedDeriv. Time derivatives are right derivatives, because γ\gammaγ jumps.
  • Legendre transform. Φγ∗\Phi^*_\gammaΦγ∗​ is a real infimum, used only for ∣z∣<1|z|<1∣z∣<1, where it is bounded below.
  • Brownian motion and filtration. BBB is a Mathlib IsBrownianReal process on R≥0\mathbb R_{\ge0}R≥0​, with each BrB_rBr​ measurable. The filtration is Fst=σ(Br:t≤r≤s)\mathcal F^t_s=\sigma(B_r:t\le r\le s)Fst​=σ(Br​:t≤r≤s).
  • Stochastic integral. It is the L2L^2L2 Itô integral of the published definition Peng1990.SMP.IsItoIntegral (horizon 111), whose integrability class is exactly E∫ξ′′u2<∞\mathbb E\int\xi''u^2<\inftyE∫ξ′′u2<∞.
  • Supremum. Jγ(t,z)=v\mathcal J_\gamma(t,z)=vJγ​(t,z)=v is stated as "vvv is the least upper bound of the objective values of admissible controls" (IsLUB), never as a real sSup. A default value of an empty or unbounded supremum therefore cannot make a statement trivially true.
  • Disclosed hypothesis. Lemma 7.2, the envelope identities and Lemma 7.3 assume that ξ\xiξ is not identically zero (some ck≠0c_k\neq0ck​=0). For ξ≡0\xi\equiv0ξ≡0 one has Φγ(t,x)=∣x∣\Phi_\gamma(t,x)=|x|Φγ​(t,x)=∣x∣ for all ttt, and these statements fail. Proposition 7.1, the evaluation at the origin and the goal need no such hypothesis.
  • Lemma 7.3. The statement includes the inequality ν+∂z2V<0\nu+\partial_z^2V<0ν+∂z2​V<0, which the page proves. This rules out reading the HJB supremum as a default value.

The paper's algorithmic results (Theorems 2–4, Corollary 2.2) are out of scope. They need the AMP and state-evolution machinery of Section 5 and Appendix A, and an informal model of computation. The optional bound (4.4) is not stated.

Welcome contributions include the regularity of Cole–Hopf solutions (Gaussian convolution, log-moment-generating functions), a general verification theorem for one-dimensional controlled martingales with a terminal state constraint, and Itô's formula for C1,2C^{1,2}C1,2 functions.

Selected references

  • A. El Alaoui, A. Montanari, M. Sellke, Optimization of Mean-field Spin Glasses, arXiv:2001.00904v1, 2020. https://arxiv.org/abs/2001.00904
  • A. Auffinger, W.-K. Chen, Parisi formula for the ground state energy in the mixed p-spin model, Ann. Probab. 45(6b), 2017. https://arxiv.org/abs/1606.05335
  • A. Jagannath, I. Tobasco, A dynamic programming approach to the Parisi functional, Proc. AMS 144, 2016. https://arxiv.org/abs/1502.04398
  • N. Touzi, Optimal Stochastic Control, Stochastic Target Problems, and Backward SDE, Fields Institute Monographs 29, Springer, 2012 (cited as [Tou12] in the paper; the verification argument of Section 7 follows its Theorem 4.1).
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Algorithmic Game TheoryOperations ResearchStochastic Systems·Captain: mikedeng1

Nonzero-Sum Stochastic Differential Games with Impulse Controls: A Verification Theorem with Applications 1: Regular Solutions of the Quasi-Variational Inequalities Give Nash Equilibrium PayoffsResearch Paper

Motivation

Many economic and engineering systems are steered by agents who act at discrete instants rather than continuously: a central bank intervenes on an exchange rate, two energy producers adjust a shared stock, a firm rebalances inventory. Each action has a fixed cost, so continuous control is not realistic. The mathematical model is impulse control: the state follows a diffusion, and a controller may shift it at chosen stopping times by paying a cost. The single-controller theory is classical (Øksendal and Sulem, Applied Stochastic Control of Jump Diffusions, 2007). When two controllers with different objectives act on the same state, the result is a nonzero-sum stochastic differential game with impulse controls.

Before Aïd, Basei, Callegaro, Campi and Vargiolu, the literature on games with impulse controls was almost entirely zero-sum: Cosso (SIAM J. Control Optim., 2013) characterised the value of zero-sum impulse games through a double-obstacle quasi-variational inequality in the viscosity sense. Their paper (Math. Oper. Res. 45(1), 2020; arXiv:1605.00039) gives the first general formulation of the nonzero-sum case together with a verification theorem: a system of quasi-variational inequalities (QVIs) whose sufficiently regular solutions are the equilibrium payoffs. Its Section 4 then computes Nash equilibria in closed form for a one-dimensional game.

Setting

A kkk-dimensional Brownian motion WWW on a filtered probability space satisfying the usual conditions drives the state equation

dYs=b(Ys) ds+σ(Ys) dWs,Ys∈Rd,dY_s=b(Y_s)\,ds+\sigma(Y_s)\,dW_s ,\qquad Y_s\in\mathbb R^d,dYs​=b(Ys​)ds+σ(Ys​)dWs​,Ys​∈Rd,

with globally Lipschitz bbb and σ\sigmaσ. The game takes place in an open set S⊆RdS\subseteq\mathbb R^dS⊆Rd and ends at the exit time τS\tau_SτS​ of the state from SSS. Each of two players i∈{1,2}i\in\{1,2\}i∈{1,2} has a nonempty impulse set Zi⊆RliZ_i\subseteq\mathbb R^{l_i}Zi​⊆Rli​ and a continuous impulse map Γi:S×Zi→S\Gamma^i:S\times Z_i\to SΓi:S×Zi​→S: an intervention with impulse δ\deltaδ moves the state from yyy to Γi(y,δ)\Gamma^i(y,\delta)Γi(y,δ).

A strategy of player iii is a pair φi=(Ci,ξi)\varphi_i=(\mathcal C_i,\xi_i)φi​=(Ci​,ξi​) with Ci⊆S\mathcal C_i\subseteq SCi​⊆S open and ξi:S→Zi\xi_i:S\to Z_iξi​:S→Zi​ continuous. Player iii intervenes as soon as the state leaves Ci\mathcal C_iCi​, with impulse ξi(y)\xi_i(y)ξi​(y) at the current state yyy. Player 1 has priority on ties, and several interventions may happen at the same instant. This defines the controlled process XXX, the intervention times τi,n\tau_{i,n}τi,n​ and impulses δi,n\delta_{i,n}δi,n​ of each player, and the states X(τi,n)−X_{(\tau_{i,n})^-}X(τi,n​)−​ just before each intervention. The payoff of player iii is

Ji(x;φ1,φ2)=E[∫0τSe−ρisfi(Xs)ds+∑τi,n<τSe−ρiτi,nϕi(X(τi,n)−,δi,n)+∑τj,n<τSe−ρiτj,nψi(X(τj,n)−,δj,n)+e−ρiτShi(XτS)1{τS<∞}],J^i(x;\varphi_1,\varphi_2)=\mathbb E\Big[\int_0^{\tau_S}e^{-\rho_is}f_i(X_s)ds+\sum_{\tau_{i,n}<\tau_S}e^{-\rho_i\tau_{i,n}}\phi_i(X_{(\tau_{i,n})^-},\delta_{i,n})+\sum_{\tau_{j,n}<\tau_S}e^{-\rho_i\tau_{j,n}}\psi_i(X_{(\tau_{j,n})^-},\delta_{j,n})+e^{-\rho_i\tau_S}h_i(X_{\tau_S})\mathbf 1_{\{\tau_S<\infty\}}\Big],Ji(x;φ1​,φ2​)=E[∫0τS​​e−ρi​sfi​(Xs​)ds+τi,n​<τS​∑​e−ρi​τi,n​ϕi​(X(τi,n​)−​,δi,n​)+τj,n​<τS​∑​e−ρi​τj,n​ψi​(X(τj,n​)−​,δj,n​)+e−ρi​τS​hi​(XτS​​)1{τS​<∞}​],

where j≠ij\ne ij=i, ρi>0\rho_i>0ρi​>0, fif_ifi​ is a running payoff, ϕi\phi_iϕi​ the cost of one's own interventions, ψi\psi_iψi​ the gain from the opponent's, and hih_ihi​ a terminal payoff on ∂S\partial S∂S. A pair of strategies is xxx-admissible, (φ1,φ2)∈Φx(\varphi_1,\varphi_2)\in\Phi_x(φ1​,φ2​)∈Φx​, when these four terms are integrable, sup⁡s≤τS∣Xs∣\sup_{s\le\tau_S}|X_s|sups≤τS​​∣Xs​∣ has all moments, and the interventions do not accumulate before τS\tau_SτS​. A Nash equilibrium is a pair in Φx\Phi_xΦx​ from which no player gains by a unilateral admissible deviation.

Given candidate payoff functions V1,V2V_1,V_2V1​,V2​ on Sˉ\bar SSˉ, let δi(x)\delta_i(x)δi​(x) be the unique maximiser of Vi(Γi(x,δ))+ϕi(x,δ)V_i(\Gamma^i(x,\delta))+\phi_i(x,\delta)Vi​(Γi(x,δ))+ϕi​(x,δ) over ZiZ_iZi​. Define MiVi(x)=Vi(Γi(x,δi(x)))+ϕi(x,δi(x))\mathcal M_iV_i(x)=V_i(\Gamma^i(x,\delta_i(x)))+\phi_i(x,\delta_i(x))Mi​Vi​(x)=Vi​(Γi(x,δi​(x)))+ϕi​(x,δi​(x)), HiVi(x)=Vi(Γj(x,δj(x)))+ψi(x,δj(x))\mathcal H_iV_i(x)=V_i(\Gamma^j(x,\delta_j(x)))+\psi_i(x,\delta_j(x))Hi​Vi​(x)=Vi​(Γj(x,δj​(x)))+ψi​(x,δj​(x)), the continuation region Di={MiVi−Vi<0}\mathcal D_i=\{\mathcal M_iV_i-V_i<0\}Di​={Mi​Vi​−Vi​<0} and the generator AV=b⋅∇V+12tr⁡(σσtD2V)\mathcal AV=b\cdot\nabla V+\tfrac12\operatorname{tr}(\sigma\sigma^tD^2V)AV=b⋅∇V+21​tr(σσtD2V). The QVI system is

Vi=hi on ∂S,MjVj−Vj≤0 on S,HiVi−Vi=0 on {MjVj=Vj},max⁡{AVi−ρiVi+fi, MiVi−Vi}=0 on Dj.V_i=h_i\ \text{on }\partial S,\quad \mathcal M_jV_j-V_j\le0\ \text{on }S,\quad \mathcal H_iV_i-V_i=0\ \text{on }\{\mathcal M_jV_j=V_j\},\quad \max\{\mathcal AV_i-\rho_iV_i+f_i,\ \mathcal M_iV_i-V_i\}=0\ \text{on }\mathcal D_j .Vi​=hi​ on ∂S,Mj​Vj​−Vj​≤0 on S,Hi​Vi​−Vi​=0 on {Mj​Vj​=Vj​},max{AVi​−ρi​Vi​+fi​, Mi​Vi​−Vi​}=0 on Dj​.

Formalization targets

Goal: Theorem 3.3 (verification theorem)

Suppose V1,V2V_1,V_2V1​,V2​ solve the QVI system, Vi∈C2(Dj∖∂Di)∩C1(Dj)∩C(Sˉ)V_i\in C^2(\mathcal D_j\setminus\partial\mathcal D_i)\cap C^1(\mathcal D_j)\cap C(\bar S)Vi​∈C2(Dj​∖∂Di​)∩C1(Dj​)∩C(Sˉ) with polynomial growth, ∂Di\partial\mathcal D_i∂Di​ is a Lipschitz surface near which ViV_iVi​ has locally bounded first and second derivatives, x∈Sx\in Sx∈S, and the threshold pair φi∗=(Di,δi)\varphi_i^*=(\mathcal D_i,\delta_i)φi∗​=(Di​,δi​) is xxx-admissible. Then

(φ1∗,φ2∗) is a Nash equilibrium andVi(x)=Ji(x;φ1∗,φ2∗),i=1,2.(\varphi_1^*,\varphi_2^*)\ \text{is a Nash equilibrium and}\quad V_i(x)=J^i(x;\varphi_1^*,\varphi_2^*),\qquad i=1,2 .(φ1∗​,φ2∗​) is a Nash equilibrium andVi​(x)=Ji(x;φ1∗​,φ2∗​),i=1,2.

Milestones

  • Lemma 2.3: the controlled process is the concatenation of diffusion pieces, it jumps only at interventions, and between interventions it stays in C1∩C2\mathcal C_1\cap\mathcal C_2C1​∩C2​.
  • Remark 3.6, (3.8b), (3.8d), (3.8f): against φ2∗\varphi_2^*φ2∗​, the state stays in D2\mathcal D_2D2​, and player 2 intervenes only on {M2V2=V2}\{\mathcal M_2V_2=V_2\}{M2​V2​=V2​} with impulse δ2\delta_2δ2​.
  • Step 1 of the proof: V1(x)≥J1(x;φ1,φ2∗)V_1(x)\ge J^1(x;\varphi_1,\varphi_2^*)V1​(x)≥J1(x;φ1​,φ2∗​) for every admissible deviation φ1\varphi_1φ1​.
  • Step 2 of the proof: V1(x)=J1(x;φ1∗,φ2∗)V_1(x)=J^1(x;\varphi_1^*,\varphi_2^*)V1​(x)=J1(x;φ1∗​,φ2∗​).

The goal follows from Steps 1 and 2 and their mirror images for player 2.

Significance

The theorem turns the search for Nash equilibria of nonzero-sum impulse games, an infinite-dimensional fixed-point problem over strategy pairs, into a deterministic problem: find functions satisfying a system of coupled QVIs with prescribed regularity. The regularity conditions become smooth-pasting conditions, hence a system of algebraic equations; Section 4 of the paper solves it explicitly for a one-dimensional game with linear payoffs. A further consequence is structural: equilibrium payoffs need only be C2C^2C2 on the opponent's continuation region, which is what lets non-smooth, piecewise-defined candidates qualify.

The result is proved in the paper; no machine-checked version exists. A complete formalization would be the first verified verification theorem for impulse control, single-player or game, and would expose every convention of the model: priority on ties, simultaneous interventions, the treatment of exit, and the integrability of the payoff. Several of these conventions need correction on the page, as listed below.

Difficulty

The heuristic argument applies Itô's formula to e−ρ1tV1(Xt)e^{-\rho_1t}V_1(X_t)e−ρ1​tV1​(Xt​) and uses the QVIs term by term. This fails on two counts. First, V1V_1V1​ is only C1C^1C1 across the free boundary ∂D1\partial\mathcal D_1∂D1​, so Itô's formula does not apply directly. The paper mollifies V1V_1V1​ (following Øksendal's proof of his verification theorem for optimal stopping) and must control the second derivatives near a Lipschitz boundary. Second, the sums over interventions may be infinite and the horizon unbounded, so expectations and limits do not commute. The passage to the limit needs the integrability built into Φx\Phi_xΦx​ and the polynomial growth of ViV_iVi​. The stochastic-calculus infrastructure itself (Itô's formula for continuous semimartingales stopped at random times, strong solutions of Lipschitz SDEs restarted at stopping times) is largely missing from Mathlib.

Formalization scope

The Lean model is pathwise. A realization is a sequence of diffusion pieces, each solving the state equation from the random restart time with the restart value. The Itô integral is the published relation EthierKurtz.HasBrownianItoIntegral, and the stochastic basis uses the published You2015.Shared.UsualConditions and IsFBrownian. Times take values in [0,∞][0,\infty][0,∞] with e−ρ⋅∞=0e^{-\rho\cdot\infty}=0e−ρ⋅∞=0, and the state space is EuclideanSpace ℝ (Fin d). Φx\Phi_xΦx​ asks for one admissible realization, while the Nash inequalities and the payoff identity hold on every admissible realization; strong uniqueness makes these readings equivalent.

The following deviate from the page and are disclosed in the items:

  1. δi\delta_iδi​ is assumed continuous, so that φi∗\varphi_i^*φi∗​ is a strategy.
  2. The fourth QVI is imposed on Dj∖∂Di\mathcal D_j\setminus\partial\mathcal D_iDj​∖∂Di​, where AVi\mathcal AV_iAVi​ exists.
  3. The exit time is αkˉ+1S\alpha^S_{\bar k+1}αkˉ+1S​, not the printed αkˉS\alpha^S_{\bar k}αkˉS​.
  4. The gain term of (2.7) is read with the opponent's interventions.
  5. The supremum in (2.8) is taken over [0,τS][0,\tau_S][0,τS​].
  6. Interventions accumulating at a finite τS\tau_SτS​ are excluded from Φx\Phi_xΦx​, since the page leaves XτSX_{\tau_S}XτS​​ undefined there.
  7. Lemma 2.3 is stated in corrected form for simultaneous and boundary interventions.

The payoff is a Bochner expectation only inside Φx\Phi_xΦx​, which requires the L1L^1L1 conditions of (2.7) and the integrability of each payoff. A non-integrable deviation therefore never receives the junk payoff 000, and the Nash inequality cannot hold vacuously.

Contributions are welcome on the stochastic-calculus layer this needs (Itô's formula, strong existence and uniqueness for Lipschitz SDEs, optional stopping for stochastic integrals) and on the mollification lemma for functions that are C1C^1C1 with piecewise bounded second derivatives across a Lipschitz surface. These are reusable well beyond this mission.

Selected references

  • R. Aïd, M. Basei, G. Callegaro, L. Campi, T. Vargiolu, Nonzero-sum stochastic differential games with impulse controls: a verification theorem with applications, Math. Oper. Res. 45(1), 2020 (accepted manuscript, arXiv:1605.00039v4). https://arxiv.org/abs/1605.00039
  • A. Cosso, Stochastic differential games involving impulse controls and double-obstacle quasi-variational inequalities, SIAM J. Control Optim. 51(3), 2102–2131, 2013.
  • B. Øksendal, Stochastic Differential Equations, 6th ed., Springer, 2003. https://doi.org/10.1007/978-3-642-14394-6
  • B. Øksendal, A. Sulem, Applied Stochastic Control of Jump Diffusions, 2nd ed., Springer, 2007. https://doi.org/10.1007/978-3-540-69826-5
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AnalysisPartial Differential Equations·Captain: mikedeng1

Stability and Instability Results of the Wave Equation with a Delay Term in the Boundary or Internal Feedbacks II: Exponential Decay under Delayed Internal DampingResearch Paper

Motivation

Feedback laws that damp vibrations in elastic structures are implemented by sensors and actuators, and a physical loop always reacts with some time delay τ>0\tau>0τ>0: the damping force at time ttt is computed from the velocity measured at time t−τt-\taut−τ. Datko, Lagnese and Polis showed in 1986 that an arbitrarily small delay in a boundary feedback can destroy the stability of a one-dimensional wave equation (Datko–Lagnese–Polis, SIAM J. Control Optim. 24 (1986)), and Datko showed that such fragility is common to a broad class of feedback-stabilized hyperbolic systems (Datko, SIAM J. Control Optim. 26 (1988)). Delay-robustness is therefore a genuine question for every stabilizing feedback, not a technicality.

Nicaise and Pignotti (SIAM J. Control Optim. 45 (2006) 1561–1585) identified a simple sufficient condition in several space dimensions: if the feedback contains an undelayed velocity term with gain μ1\mu_1μ1​ and a delayed one with gain μ2\mu_2μ2​, and μ2<μ1\mu_2<\mu_1μ2​<μ1​, the energy still decays exponentially; if μ2≥μ1\mu_2\ge\mu_1μ2​≥μ1​, instabilities appear for some delays. This mission formalizes the stability half for internal (distributed) damping, localized near the Neumann part of the boundary.

Timeline.

  • 1986: Datko, Lagnese, Polis — small delays destabilize a boundary-damped 1D wave equation.
  • 1988: Datko — many feedback-stabilized hyperbolic systems are not robust with respect to small delays.
  • 1990: Zuazua — exponential decay for the semilinear wave equation with locally distributed damping, without delay (Comm. PDE 15 (1990)); Liu (1997) treats locally distributed damping for general conservative systems (SIAM J. Control Optim. 35 (1997)).
  • 2006: Nicaise, Pignotti — exponential decay with a delayed boundary or internal feedback under μ2<μ1\mu_2<\mu_1μ2​<μ1​ (Theorems 1.1 and 1.3), and instability examples when μ2≥μ1\mu_2\ge\mu_1μ2​≥μ1​ (Theorems 1.2 and 1.4).

Setting

Let Ω⊂Rn\Omega\subset\mathbb{R}^nΩ⊂Rn, n≥1n\ge1n≥1, be a bounded open set with boundary Γ\GammaΓ of class C2C^2C2, split as Γ=ΓD∪ΓN\Gamma=\Gamma_D\cup\Gamma_NΓ=ΓD​∪ΓN​ with ΓD‾∩ΓN‾=∅\overline{\Gamma_D}\cap\overline{\Gamma_N}=\emptysetΓD​​∩ΓN​​=∅ and ΓD≠∅\Gamma_D\neq\emptysetΓD​=∅. Write ν\nuν for the outer unit normal, dΓd\GammadΓ for the surface measure, ut,uttu_t,u_{tt}ut​,utt​ for time derivatives and Δ\DeltaΔ for the Laplacian in xxx.

Geometric hypothesis (1.6)–(1.7): there are a C2C^2C2 function vvv and α>0\alpha>0α>0 with ⟨D2v(x)ξ,ξ⟩≥2α∣ξ∣2\langle D^2v(x)\xi,\xi\rangle\ge2\alpha|\xi|^2⟨D2v(x)ξ,ξ⟩≥2α∣ξ∣2 for all x∈Ω‾x\in\overline\Omegax∈Ω, ξ∈Rn\xi\in\mathbb{R}^nξ∈Rn, and ∇v(x)⋅ν(x)≤0\nabla v(x)\cdot\nu(x)\le0∇v(x)⋅ν(x)≤0 on ΓD\Gamma_DΓD​.

Damping coefficient. ω⊂Ω\omega\subset\Omegaω⊂Ω is an open neighbourhood of ΓN\Gamma_NΓN​ (in Ω\OmegaΩ), and a∈L∞(Ω)a\in L^\infty(\Omega)a∈L∞(Ω) satisfies

a(x)≥0 a.e. in Ω(1.17),a(x)>a0>0 a.e. in ω(1.18).a(x)\ge0\ \text{a.e. in }\Omega\quad(1.17),\qquad a(x)>a_0>0\ \text{a.e. in }\omega\quad(1.18).a(x)≥0 a.e. in Ω(1.17),a(x)>a0​>0 a.e. in ω(1.18).

The system (1.12)–(1.16): for gains μ1,μ2>0\mu_1,\mu_2>0μ1​,μ2​>0 and delay τ>0\tau>0τ>0,

utt(x,t)−Δu(x,t)+a(x)[μ1ut(x,t)+μ2ut(x,t−τ)]=0in Ω×(0,∞),u_{tt}(x,t)-\Delta u(x,t)+a(x)\big[\mu_1u_t(x,t)+\mu_2u_t(x,t-\tau)\big]=0\quad\text{in }\Omega\times(0,\infty),utt​(x,t)−Δu(x,t)+a(x)[μ1​ut​(x,t)+μ2​ut​(x,t−τ)]=0in Ω×(0,∞),

with u=0u=0u=0 on ΓD\Gamma_DΓD​, ∂u/∂ν=0\partial u/\partial\nu=0∂u/∂ν=0 on ΓN\Gamma_NΓN​, initial data u(⋅,0)=u0u(\cdot,0)=u_0u(⋅,0)=u0​, ut(⋅,0)=u1u_t(\cdot,0)=u_1ut​(⋅,0)=u1​, and history ut(x,t−τ)=g0(x,t−τ)u_t(x,t-\tau)=g_0(x,t-\tau)ut​(x,t−τ)=g0​(x,t−τ) for t∈(0,τ)t\in(0,\tau)t∈(0,τ).

The energy. Assume μ2<μ1\mu_2<\mu_1μ2​<μ1​ (1.8) and fix ξ\xiξ with τμ2<ξ<τ(2μ1−μ2)\tau\mu_2<\xi<\tau(2\mu_1-\mu_2)τμ2​<ξ<τ(2μ1​−μ2​) (1.10). Then

F(t)=12∫Ω{ut2(x,t)+∣∇u(x,t)∣2}dx+ξ2∫Ωa(x)∫01ut2(x,t−τρ) dρ dx(1.19).\mathcal F(t)=\frac12\int_\Omega\big\{u_t^2(x,t)+|\nabla u(x,t)|^2\big\}dx+\frac\xi2\int_\Omega a(x)\int_0^1u_t^2(x,t-\tau\rho)\,d\rho\,dx\qquad(1.19).F(t)=21​∫Ω​{ut2​(x,t)+∣∇u(x,t)∣2}dx+2ξ​∫Ω​a(x)∫01​ut2​(x,t−τρ)dρdx(1.19).

The first summand is the standard energy E(t)\mathcal E(t)E(t); the second accounts for the velocity history on the delay window.

Formalization targets

Goal: Theorem 1.3

There exist C1,C2>0C_1,C_2>0C1​,C2​>0, depending on the data but not on the solution, such that every solution satisfies

F(t)≤C1 F(0) e−C2t∀t≥0.\mathcal F(t)\le C_1\,\mathcal F(0)\,e^{-C_2t}\qquad\forall t\ge0.F(t)≤C1​F(0)e−C2​t∀t≥0.

The constants are left existential, as in the paper, so no later sharpening of rates invalidates the goal.

Milestones (in the order of the proof)

  1. (4.4) The energy identity
F′(t)=−μ1 ⁣∫Ωaut2(t)−μ2 ⁣∫Ωaut(t)ut(t−τ)+ξτ−12 ⁣∫Ωaut2(t)−ξτ−12 ⁣∫Ωaut2(t−τ).\mathcal F'(t)=-\mu_1\!\int_\Omega a u_t^2(t)-\mu_2\!\int_\Omega a u_t(t)u_t(t-\tau)+\frac{\xi\tau^{-1}}2\!\int_\Omega a u_t^2(t)-\frac{\xi\tau^{-1}}2\!\int_\Omega a u_t^2(t-\tau).F′(t)=−μ1​∫Ω​aut2​(t)−μ2​∫Ω​aut​(t)ut​(t−τ)+2ξτ−1​∫Ω​aut2​(t)−2ξτ−1​∫Ω​aut2​(t−τ).
  1. Proposition 4.1 F\mathcal FF is nonincreasing and F′(t)≤−C∫Ωa{ut2(t)+ut2(t−τ)}dx\mathcal F'(t)\le-C\int_\Omega a\{u_t^2(t)+u_t^2(t-\tau)\}dxF′(t)≤−C∫Ω​a{ut2​(t)+ut2​(t−τ)}dx with C>0C>0C>0.
  2. Proposition 4.2 Observability for the undamped mixed problem: for TTT larger than some T0T_0T0​, Ew(0)≤C1∫0T∫ωwt2 dx dt\mathcal E_w(0)\le C_1\int_0^T\int_\omega w_t^2\,dx\,dtEw​(0)≤C1​∫0T​∫ω​wt2​dxdt.
  3. Proposition 4.3 Observability for the delayed system: for TTT larger than some T‾\overline TT, F(0)≤C0∫0T∫Ωa{ut2(t)+ut2(t−τ)}dx dt\mathcal F(0)\le C_0\int_0^T\int_\Omega a\{u_t^2(t)+u_t^2(t-\tau)\}dx\,dtF(0)≤C0​∫0T​∫Ω​a{ut2​(t)+ut2​(t−τ)}dxdt.
  4. Contraction step (p. 1579): some T>0T>0T>0 and C~∈[0,1)\widetilde C\in[0,1)C∈[0,1) with F(T)≤C~ F(0)\mathcal F(T)\le\widetilde C\,\mathcal F(0)F(T)≤CF(0) for every solution.

Significance

The result. Theorem 1.3 shows that a localized viscous damping acting only near the Neumann boundary keeps its exponential stabilizing effect when part of the feedback is delayed, provided the delayed gain is dominated by the undelayed one. Together with Theorem 1.4 of the same paper (instability for μ2≥μ1\mu_2\ge\mu_1μ2​≥μ1​ and suitable delays) it gives a sharp threshold in terms of the gains. The energy F\mathcal FF with its history term became the standard Lyapunov functional for delayed wave and plate equations in the literature that followed.

Formalizing it. The theorem is proved in the paper; no machine-checked proof of it, or of any exponential decay result for a multidimensional wave equation, is known to exist. A complete development would produce reusable Lean infrastructure: energy identities for the wave equation on C2C^2C2 domains via the divergence theorem, the delay-energy calculus, and an observability inequality for the wave equation with mixed boundary conditions. Each milestone has value on its own; Proposition 4.2 in particular is a classical control-theoretic result.

Difficulty

The energy estimates (milestones 1 and 2) are calculus once the divergence theorem is available. The central difficulty is observability. Energy dissipation alone gives only F\mathcal FF nonincreasing; exponential decay needs the energy at time 000 to be controlled by the energy dissipated on [0,T][0,T][0,T] (Proposition 4.3), and that needs the conservative wave equation to be observable from ω\omegaω (Proposition 4.2). The observability inequality does not follow from energy identities: the paper relies on Carleman estimates of Lasiecka–Triggiani–Yao (1999) and a compactness–uniqueness argument, neither of which is available in Mathlib. The obvious attempt, a multiplier identity with ∇v⋅∇u\nabla v\cdot\nabla u∇v⋅∇u alone, leaves boundary terms on ΓN\Gamma_NΓN​ that cannot be absorbed without a localization near ΓN\Gamma_NΓN​ and a lower-order compactness step.

Formalization scope

  • Points are EuclideanSpace ℝ (Fin n) with 1 ≤ n; solutions are real valued.
  • The C2C^2C2 boundary is given by a global C2C^2C2 defining function ψ\psiψ with Ω={ψ<0}\Omega=\{\psi<0\}Ω={ψ<0}, ∂Ω={ψ=0}\partial\Omega=\{\psi=0\}∂Ω={ψ=0}, ∇ψ≠0\nabla\psi\ne0∇ψ=0 on ∂Ω\partial\Omega∂Ω; ν=∇ψ/∣∇ψ∣\nu=\nabla\psi/|\nabla\psi|ν=∇ψ/∣∇ψ∣.
  • The surface measure dΓd\GammadΓ is a finite measure carried by ∂Ω\partial\Omega∂Ω for which the Gauss–Green formula holds for every C1C^1C1 vector field; this determines it uniquely. It is not Mathlib's unnormalized Hausdorff measure.
  • Solutions are classical: uuu is C2C^2C2 on Rn×R\mathbb{R}^n\times\mathbb{R}Rn×R, the equation holds for every t>0t>0t>0 and almost every x∈Ωx\in\Omegax∈Ω (because aaa is only L∞L^\inftyL∞), and the initial data and history are the values of uuu and utu_tut​ at t≤0t\le0t≤0. This is a subclass of the paper's solutions, so the formal theorems are consequences of the paper's.
  • aaa is measurable and essentially bounded on Ω\OmegaΩ; (1.17) and (1.18) are almost-everywhere conditions. "Open neighbourhood of ΓN\Gamma_NΓN​" means ω⊇O∩Ω\omega\supseteq O\cap\Omegaω⊇O∩Ω for some open O⊇ΓNO\supseteq\Gamma_NO⊇ΓN​ (a subset of Ω\OmegaΩ cannot contain ΓN\Gamma_NΓN​ itself).
  • Added hypothesis (Propositions 4.2, 4.3, the contraction step and Theorem 1.3): the closure of every connected component of Ω\OmegaΩ meets ΓD\Gamma_DΓD​; this holds whenever Ω\OmegaΩ is connected. The proof of Proposition 4.2 uses Poincaré's inequality for functions vanishing on ΓD\Gamma_DΓD​, and its compactness–uniqueness step concludes that a harmonic function vanishing on ΓD\Gamma_DΓD​ with zero normal derivative on ΓN\Gamma_NΓN​ is zero; both need this condition.
  • "Decreasing" in Proposition 4.1 is read as nonincreasing; its constant C>0C>0C>0 is existential, chosen before the solution.
  • Printed slips on p. 1575: the last line of (4.3) integrates with dΓd\GammadΓ where dxdxdx is meant, and its first line repeats uρ(x,t−τ)u_\rho(x,t-\tau)uρ​(x,t−τ) for uρ(x,t−τρ)u_\rho(x,t-\tau\rho)uρ​(x,t−τρ). Neither affects any formal statement; (4.4) itself is correct.
  • A formalization in which the aaa-weighted integrals are Lean's junk value 000 (non-measurable aaa), in which ω\omegaω is required to contain ΓN\Gamma_NΓN​ (unsatisfiable), or in which the surface measure is arbitrary, would trivialize or falsify the targets; all three are excluded by the definitions.

Needed infrastructure: the divergence theorem on C2C^2C2 domains (assumed here as a structure field), differentiation under the integral sign for the energies, Carleman estimates or another route to observability for the mixed wave problem, and a compactness argument (Rellich). Contributions of any of these as standalone lemmas are welcome.

Selected references

  • S. Nicaise, C. Pignotti, Stability and instability results of the wave equation with a delay term in the boundary or internal feedbacks, SIAM J. Control Optim. 45(5):1561–1585, 2006. https://doi.org/10.1137/060648891
  • R. Datko, J. Lagnese, M. P. Polis, An example on the effect of time delays in boundary feedback stabilization of wave equations, SIAM J. Control Optim. 24:152–156, 1986. https://doi.org/10.1137/0324007
  • R. Datko, Not all feedback stabilized hyperbolic systems are robust with respect to small time delays in their feedbacks, SIAM J. Control Optim. 26:697–713, 1988. https://doi.org/10.1137/0326040
  • E. Zuazua, Exponential decay for the semilinear wave equation with locally distributed damping, Comm. Partial Differential Equations 15:205–235, 1990. https://doi.org/10.1080/03605309908820684
  • K. Liu, Locally distributed control and damping for the conservative systems, SIAM J. Control Optim. 35:1574–1590, 1997. https://doi.org/10.1137/S0363012995284928
  • I. Lasiecka, R. Triggiani, P. F. Yao, Inverse/observability estimates for second-order hyperbolic equations with variable coefficients, J. Math. Anal. Appl. 235:13–57, 1999 (reference [14] of the paper; the Carleman estimates used in Proposition 4.2). https://doi.org/10.1006/jmaa.1999.6348
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AnalysisPartial Differential Equations·Captain: mikedeng1

Stability and Instability Results of the Wave Equation with a Delay Term in the Boundary or Internal Feedbacks I: Exponential Decay under Delayed Boundary FeedbackResearch Paper

Motivation

Boundary feedback stabilization of the wave equation asks whether a vibrating body at rest on part of its boundary can be brought to rest by a damping law on the rest of its boundary. With the undelayed velocity feedback ∂u/∂ν=−μ1ut\partial u/\partial\nu = -\mu_1 u_t∂u/∂ν=−μ1​ut​, the energy decays exponentially under geometric conditions on the domain; results of this kind go back to Chen (1979, 1981), Lagnese (1983, 1988), Lasiecka and Triggiani (1987), and Komornik and Zuazua (1990).

Real controllers act with a delay, and delays can destroy stability. Datko, Lagnese and Polis (1986) and Datko (1988) showed that an arbitrarily small delay in a boundary feedback that stabilizes the one-dimensional wave equation can make the closed loop unstable. For a feedback made of an undelayed part and a delayed part, μ1ut(t)+μ2ut(t−τ)\mu_1 u_t(t) + \mu_2 u_t(t-\tau)μ1​ut​(t)+μ2​ut​(t−τ), Xu, Yung and Li (2006) proved, by spectral analysis in one space dimension, that the system is stable when μ2<μ1\mu_2 < \mu_1μ2​<μ1​. Nicaise and Pignotti (2006) extended the stability result to bounded domains in any dimension nnn. This mission formalizes that extension: Theorem 1.1 of their paper.

Setting

Let Ω⊂Rn\Omega \subset \mathbb R^nΩ⊂Rn (n≥1n \ge 1n≥1) be a bounded open set whose boundary Γ\GammaΓ is of class C2C^2C2. The boundary is split as Γ=ΓD∪ΓN\Gamma = \Gamma_D \cup \Gamma_NΓ=ΓD​∪ΓN​, with ΓD‾∩ΓN‾=∅\overline{\Gamma_D} \cap \overline{\Gamma_N} = \emptysetΓD​​∩ΓN​​=∅ and ΓD≠∅\Gamma_D \ne \emptysetΓD​=∅. Let ν\nuν be the outer unit normal and dΓd\GammadΓ the surface measure on Γ\GammaΓ. Fix the undelayed gain μ1>0\mu_1 > 0μ1​>0, the delayed gain μ2>0\mu_2 > 0μ2​>0 and the delay τ>0\tau > 0τ>0. The problem is

utt−Δu=0in Ω×(0,∞),(1.1)u=0on ΓD×(0,∞),(1.2)∂u∂ν(x,t)=−μ1ut(x,t)−μ2ut(x,t−τ)on ΓN×(0,∞),(1.3)\begin{aligned} u_{tt} - \Delta u &= 0 && \text{in } \Omega \times (0,\infty), &(1.1)\\ u &= 0 && \text{on } \Gamma_D \times (0,\infty), &(1.2)\\ \tfrac{\partial u}{\partial \nu}(x,t) &= -\mu_1 u_t(x,t) - \mu_2 u_t(x,t-\tau) && \text{on } \Gamma_N \times (0,\infty), &(1.3) \end{aligned}utt​−Δuu∂ν∂u​(x,t)​=0=0=−μ1​ut​(x,t)−μ2​ut​(x,t−τ)​​in Ω×(0,∞),on ΓD​×(0,∞),on ΓN​×(0,∞),​(1.1)(1.2)(1.3)​

with initial data u(⋅,0)=u0u(\cdot,0) = u_0u(⋅,0)=u0​ and ut(⋅,0)=u1u_t(\cdot,0) = u_1ut​(⋅,0)=u1​ in Ω\OmegaΩ, and a history ut=f0u_t = f_0ut​=f0​ on ΓN×(−τ,0)\Gamma_N \times (-\tau, 0)ΓN​×(−τ,0) (1.4)–(1.5).

The geometric hypothesis requires a function v∈C2(Ω‾)v \in C^2(\overline\Omega)v∈C2(Ω) and a constant α>0\alpha > 0α>0 with two properties:

⟨D2v(x)ξ,ξ⟩≥2α∣ξ∣2(x∈Ω‾, ξ∈Rn),(1.6)\langle D^2 v(x)\xi,\xi\rangle \ge 2\alpha|\xi|^2 \quad (x \in \overline\Omega,\ \xi \in \mathbb R^n), \tag{1.6}⟨D2v(x)ξ,ξ⟩≥2α∣ξ∣2(x∈Ω, ξ∈Rn),(1.6) ∇v(x)⋅ν(x)≤0(x∈ΓD).(1.7)\nabla v(x)\cdot\nu(x) \le 0 \quad (x \in \Gamma_D). \tag{1.7}∇v(x)⋅ν(x)≤0(x∈ΓD​).(1.7)

For example, v(x)=∣x∣2v(x) = |x|^2v(x)=∣x∣2 satisfies both on an annulus whose inner sphere is ΓD\Gamma_DΓD​.

Assume the gain condition

μ2<μ1,(1.8)\mu_2 < \mu_1, \tag{1.8}μ2​<μ1​,(1.8)

and fix ξ\xiξ with

τμ2<ξ<τ(2μ1−μ2).(1.10)\tau\mu_2 < \xi < \tau(2\mu_1 - \mu_2). \tag{1.10}τμ2​<ξ<τ(2μ1​−μ2​).(1.10)

The energy of a solution is the standard wave energy plus a term that stores the delayed velocity:

E(t)=12∫Ω{ut2(x,t)+∣∇u(x,t)∣2} dx+ξ2∫ΓN∫01ut2(x,t−τρ) dρ dΓ.(1.9)E(t) = \frac12\int_\Omega \{u_t^2(x,t) + |\nabla u(x,t)|^2\}\,dx + \frac{\xi}{2}\int_{\Gamma_N}\int_0^1 u_t^2(x,t-\tau\rho)\,d\rho\,d\Gamma. \tag{1.9}E(t)=21​∫Ω​{ut2​(x,t)+∣∇u(x,t)∣2}dx+2ξ​∫ΓN​​∫01​ut2​(x,t−τρ)dρdΓ.(1.9)

Formalization targets

Goal: Theorem 1.1 (exponential decay)

There are constants C1,C2>0C_1, C_2 > 0C1​,C2​>0, depending on Ω,ΓD,ΓN,v,α,μ1,μ2,τ,ξ\Omega, \Gamma_D, \Gamma_N, v, \alpha, \mu_1, \mu_2, \tau, \xiΩ,ΓD​,ΓN​,v,α,μ1​,μ2​,τ,ξ but not on the solution, such that every regular solution satisfies

E(t)≤C1E(0) e−C2t∀t≥0.(1.11)E(t) \le C_1 E(0)\, e^{-C_2 t} \qquad \forall t \ge 0. \tag{1.11}E(t)≤C1​E(0)e−C2​t∀t≥0.(1.11)

The constants are existential and are not fixed numerically. Any valid pair proves the goal.

Milestones, in the order the paper's proof uses them

  1. (3.6): the energy identity, which expresses E′(t)E'(t)E′(t) through boundary integrals over ΓN\Gamma_NΓN​ only.
  2. Proposition 3.1: EEE is nonincreasing, and
E′(t)≤−C∫ΓN{ut2(x,t)+ut2(x,t−τ)} dΓ,C=min⁡{μ1−μ22−ξ2τ, −μ22+ξ2τ}>0.E'(t) \le -C\int_{\Gamma_N}\{u_t^2(x,t) + u_t^2(x,t-\tau)\}\,d\Gamma, \qquad C = \min\Big\{\mu_1 - \frac{\mu_2}{2} - \frac{\xi}{2\tau},\ -\frac{\mu_2}{2} + \frac{\xi}{2\tau}\Big\} > 0.E′(t)≤−C∫ΓN​​{ut2​(x,t)+ut2​(x,t−τ)}dΓ,C=min{μ1​−2μ2​​−2τξ​, −2μ2​​+2τξ​}>0.
  1. (3.22): the integrated form E(T)−E(0)≤−C∫0T∫ΓN{ut2(t)+ut2(t−τ)} dΓ dtE(T) - E(0) \le -C\int_0^T\int_{\Gamma_N}\{u_t^2(t) + u_t^2(t-\tau)\}\,d\Gamma\,dtE(T)−E(0)≤−C∫0T​∫ΓN​​{ut2​(t)+ut2​(t−τ)}dΓdt.
  2. Proposition 3.2 (observability): there is T‾>0\overline T > 0T>0 such that for every T>T‾T > \overline TT>T some C0>0C_0 > 0C0​>0 satisfies
E(0)≤C0∫0T∫ΓN{ut2(x,t)+ut2(x,t−τ)} dΓ dt.(3.10)E(0) \le C_0\int_0^T\int_{\Gamma_N}\{u_t^2(x,t) + u_t^2(x,t-\tau)\}\,d\Gamma\,dt. \tag{3.10}E(0)≤C0​∫0T​∫ΓN​​{ut2​(x,t)+ut2​(x,t−τ)}dΓdt.(3.10)
  1. Contraction: there are T>0T > 0T>0 and 0≤C~<10 \le \tilde C < 10≤C~<1 with E(T)≤C~E(0)E(T) \le \tilde C E(0)E(T)≤C~E(0) for every regular solution.

Significance

The theorem shows that adding a delayed component to a stabilizing boundary feedback preserves exponential decay if the delayed gain is dominated by the undelayed gain. It holds in every dimension, under the same geometric condition that governs the undelayed problem. The companion Theorem 1.2 of the same paper shows that the condition μ2<μ1\mu_2 < \mu_1μ2​<μ1​ cannot be removed: when it fails, there are delays for which some solutions keep constant, positive standard energy. The Lyapunov functional (1.9) became a standard device for delayed feedbacks in later work on wave, plate and Timoshenko systems.

The result was proved in 2006. It has no machine-checked proof. This mission produces:

  • a formal statement of the theorem on classical solutions;
  • the energy identity and dissipation inequality with explicit constants;
  • the observability inequality as a separate target, which is the deep analytic input and is reusable by any stabilization argument on the same geometry.

Difficulty

The dissipation inequality (Proposition 3.1) is a calculation: Green's formula, a change of variables in the delay variable ρ\rhoρ, and Young's inequality. The difficulty is entirely in the observability inequality (3.10). The obvious multiplier argument, which multiplies the equation by ∇v⋅∇u\nabla v\cdot\nabla u∇v⋅∇u and integrates, leaves a lower-order term ∥u∥\|u\|∥u∥ that the boundary observation does not control.

The paper removes that term in two steps. The first is a Carleman-type estimate of Lasiecka, Triggiani and Yao (1999), which is where hypotheses (1.6)–(1.7) enter. The second is a compactness–uniqueness argument closed by Holmgren's uniqueness theorem. None of these tools exists in Mathlib, and neither does Green's formula on a curved domain. The final step from a one-period contraction to exponential decay uses time-translation invariance and monotonicity of EEE.

Formalization scope

  • Domain. A MixedDomain n bundles the following:

    • a bounded open set given by a global C2C^2C2 defining function ψ\psiψ (Ω={ψ<0}\Omega = \{\psi < 0\}Ω={ψ<0}, ∂Ω={ψ=0}\partial\Omega = \{\psi = 0\}∂Ω={ψ=0}, ∇ψ≠0\nabla\psi \ne 0∇ψ=0 on ∂Ω\partial\Omega∂Ω);
    • the split ΓD∪ΓN=∂Ω\Gamma_D \cup \Gamma_N = \partial\OmegaΓD​∪ΓN​=∂Ω with disjoint closures and ΓD≠∅\Gamma_D \ne \emptysetΓD​=∅;
    • a finite measure σ\sigmaσ carried by ∂Ω\partial\Omega∂Ω satisfying the Gauss–Green formula for every C1C^1C1 vector field.

    The outer normal is ν=∇ψ/∣∇ψ∣\nu = \nabla\psi/|\nabla\psi|ν=∇ψ/∣∇ψ∣. The Gauss–Green requirement determines σ\sigmaσ uniquely as the surface measure, so the normalization of dΓd\GammadΓ in (1.9) and (1.10) is the paper's.

  • Solutions are real-valued and classical: uuu is one C2C^2C2 function on Rn×R\mathbb R^n \times \mathbb RRn×R. It satisfies (1.1)–(1.3) for t>0t > 0t>0, and its values at t≤0t \le 0t≤0 are the initial data and the history. Time derivatives are one-variable derivatives in ttt, and ∂u/∂ν=∇u⋅ν\partial u/\partial\nu = \nabla u \cdot \nu∂u/∂ν=∇u⋅ν. This is a subclass of the paper's solutions, so the formal theorems are the paper's restricted to smooth, compatible data.

  • Added hypothesis. In Proposition 3.2, the contraction step and the goal, every connected component of Ω\OmegaΩ has a boundary point in ΓD\Gamma_DΓD​ (true whenever Ω\OmegaΩ is connected). The paper's uniqueness step ("−Δw=0-\Delta w = 0−Δw=0, w=0w = 0w=0 on ΓD\Gamma_DΓD​, ∂w/∂ν=0\partial w/\partial\nu = 0∂w/∂ν=0 on ΓN\Gamma_NΓN​, so w≡0w \equiv 0w≡0") needs every component of Ω\OmegaΩ to meet ΓD\Gamma_DΓD​.

  • Strengthened statements. The identity (3.6) and Propositions 3.1 and (3.22) omit hypotheses they do not use. Proposition 3.1 states the explicit constant CCC from the end of its proof.

  • Conventions. Condition (1.10) is strict. The energy is EEE of (1.9), with the delay term, and not the standard energy. Derivatives of EEE are asserted with HasDerivAt.

  • Excluded trivializations. Three things would make the statements empty or different, and none of them is allowed:

    • a free measure in place of the surface measure;
    • the standard energy in place of EEE;
    • replacing (1.11) by E(t)→0E(t) \to 0E(t)→0.

    The degenerate case ΓN=∅\Gamma_N = \emptysetΓN​=∅ is already excluded by (1.6), (1.7) and Gauss–Green together.

  • Infrastructure needed and welcome:

    • Gauss–Green and Green's first identity on MixedDomain;
    • differentiation under the integral over Ω\OmegaΩ and ΓN\Gamma_NΓN​;
    • a Carleman or multiplier observability estimate for the wave equation with mixed boundary conditions;
    • unique continuation (Holmgren) for the wave equation;
    • the elementary lemma turning a one-period contraction plus monotonicity into exponential decay.

    The last lemma and Gauss–Green on C2C^2C2 domains are reusable far beyond this mission.

Selected references

  • S. Nicaise, C. Pignotti, Stability and instability results of the wave equation with a delay term in the boundary or internal feedbacks, SIAM J. Control Optim. 45(5) (2006), 1561–1585. https://doi.org/10.1137/060648891
  • G. Q. Xu, S. P. Yung, L. K. Li, Stabilization of wave systems with input delay in the boundary control, ESAIM Control Optim. Calc. Var. 12 (2006), 770–785. https://doi.org/10.1051/cocv:2006021
  • R. Datko, J. Lagnese, M. P. Polis, An example on the effect of time delays in boundary feedback stabilization of wave equations, SIAM J. Control Optim. 24 (1986), 152–156. https://doi.org/10.1137/0324007
  • R. Datko, Not all feedback stabilized hyperbolic systems are robust with respect to small time delays in their feedbacks, SIAM J. Control Optim. 26 (1988), 697–713. https://doi.org/10.1137/0326040
  • I. Lasiecka, R. Triggiani, P. F. Yao, Inverse/observability estimates for second-order hyperbolic equations with variable coefficients, J. Math. Anal. Appl. 235 (1999), 13–57. https://doi.org/10.1006/jmaa.1999.6348
  • V. Komornik, E. Zuazua, A direct method for the boundary stabilization of the wave equation, J. Math. Pures Appl. 69 (1990), 33–54.
  • J. Lagnese, Decay of solutions of wave equations in a bounded region with boundary dissipation, J. Differential Equations 50 (1983), 163–182. https://doi.org/10.1016/0022-0396(83)90073-6
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Stabilization for a Perturbed Chain of Integrators in Prescribed Time II: Fixed-Time and Prescribed-Time Stability of the Varying-Degree Homogeneous FeedbackResearch Paper

Motivation

Many control tasks come with a deadline: a consensus protocol or a regulation task must reach its target by a time fixed in advance, whatever the initial condition. Prescribed-time stabilization asks for a feedback law that brings every trajectory of a control system to the equilibrium by a user-chosen time TTT. The basic test case is the chain of integrators x1(n)=ux_1^{(n)}=ux1(n)​=u, the normal form of every single-input feedback-linearizable system.

Two routes to prescribed-time stabilization exist. Time-varying gains that blow up as t→Tt\to Tt→T (Song, Wang, Holloway and Krstić, Automatica 2017) are fragile under measurement noise. Fixed-time stabilization gives a settling time bounded uniformly over all initial conditions, and a time rescaling then turns the uniform bound into any prescribed TTT. Chitour, Ushirobira and Bouhemou (SIAM J. Control Optim. 2020) follow the second route with an explicit, continuous feedback. It combines Hong's backstepping homogeneous controller (Systems Control Lett. 2002) with a degree of homogeneity that depends on the state (Harmouche, Laghrouche, Chitour and Hamerlain, Int. J. Control 2017). A continuity device of Lopez-Ramirez, Efimov, Polyakov and Perruquetti (Int. J. Robust Nonlinear Control 2018) makes that degree a continuous function of the state. This mission formalizes the construction and its main results, §4.1–4.2 of the paper.

Setting

Fix n≥1n\ge1n≥1 and write x=(x1,…,xn)∈Rnx=(x_1,\dots,x_n)\in\mathbb R^nx=(x1​,…,xn​)∈Rn with the Euclidean norm. Let JnJ_nJn​ be the nnn-th Jordan block (Jnei=ei−1J_ne_i=e_{i-1}Jn​ei​=ei−1​, e0=0e_0=0e0​=0). The pure chain of integrators (31) is

x˙=Jnx+u en.\dot x=J_nx+u\,e_n .x˙=Jn​x+uen​.

For y∈Ry\in\mathbb Ry∈R and a>0a>0a>0 write ⌈y⌋a=sign⁡(y)∣y∣a\lceil y\rfloor^a=\operatorname{sign}(y)|y|^a⌈y⌋a=sign(y)∣y∣a. Given gains ℓ1,…,ℓn>0\ell_1,\dots,\ell_n>0ℓ1​,…,ℓn​>0 and κ∈[−12n,12n]\kappa\in[-\tfrac1{2n},\tfrac1{2n}]κ∈[−2n1​,2n1​], set rj=1+(j−1)κr_j=1+(j-1)\kapparj​=1+(j−1)κ and βj=(2+κ)/rj+1−1\beta_j=(2+\kappa)/r_{j+1}-1βj​=(2+κ)/rj+1​−1. Define v0=0v_0=0v0​=0 and

vj=−ℓj⌈⌈xj⌋βj−1−⌈vj−1⌋βj−1⌋rj+κrjβj−1.v_j=-\ell_j\Big\lceil\lceil x_j\rfloor^{\beta_{j-1}}-\lceil v_{j-1}\rfloor^{\beta_{j-1}}\Big\rfloor^{\frac{r_j+\kappa}{r_j\beta_{j-1}}} .vj​=−ℓj​⌈⌈xj​⌋βj−1​−⌈vj−1​⌋βj−1​⌋rj​βj−1​rj​+κ​.

The homogeneous feedback is ωκH(x)=vn(x)\omega^H_\kappa(x)=v_n(x)ωκH​(x)=vn​(x) (Definition 23). The associated Lyapunov function is

Vκ(x)=∑j=1n∣xj∣βj−1+1−∣vj−1∣βj−1+1βj−1+1−⌈vj−1⌋βj−1(xj−vj−1),V_\kappa(x)=\sum_{j=1}^n\frac{|x_j|^{\beta_{j-1}+1}-|v_{j-1}|^{\beta_{j-1}+1}}{\beta_{j-1}+1}-\lceil v_{j-1}\rfloor^{\beta_{j-1}}(x_j-v_{j-1}),Vκ​(x)=j=1∑n​βj−1​+1∣xj​∣βj−1​+1−∣vj−1​∣βj−1​+1​−⌈vj−1​⌋βj−1​(xj​−vj−1​),

and (36) is the decay inequality V˙κ≤−CVκ1+α(κ)\dot V_\kappa\le-CV_\kappa^{1+\alpha(\kappa)}V˙κ​≤−CVκ1+α(κ)​, with α(κ)=κ/(2+κ)\alpha(\kappa)=\kappa/(2+\kappa)α(κ)=κ/(2+κ) and one constant CCC for all κ\kappaκ in the range.

For m∈(0,1)m\in(0,1)m∈(0,1) and κ0∈(0,12n)\kappa_0\in(0,\tfrac1{2n})κ0​∈(0,2n1​), the state-dependent degree κ(x)\kappa(x)κ(x) of (49) equals κ0\kappa_0κ0​ where V0(x)>1+mV_0(x)>1+mV0​(x)>1+m and −κ0-\kappa_0−κ0​ where V0(x)<1−mV_0(x)<1-mV0​(x)<1−m, and it interpolates linearly in V0V_0V0​ in between. The closed-loop controller is ωκ(x)H(x)\omega^H_{\kappa(x)}(x)ωκ(x)H​(x). With B<aκ={Vκ<a}B^\kappa_{<a}=\{V_\kappa<a\}B<aκ​={Vκ​<a}, let r(m,κ0)r(m,\kappa_0)r(m,κ0​) be the largest rrr with B<rκ0⊆B<1+m0B^{\kappa_0}_{<r}\subseteq B^0_{<1+m}B<rκ0​​⊆B<1+m0​, and r(m,−κ0)r(m,-\kappa_0)r(m,−κ0​) the smallest rrr with B<r−κ0⊇B<1−m0B^{-\kappa_0}_{<r}\supseteq B^0_{<1-m}B<r−κ0​​⊇B<1−m0​. Set

T∗(m,κ0)=1C(r(m,κ0)−α(κ0)α(κ0)−2ln⁡(2m)+r(m,−κ0)−α(−κ0)−α(−κ0)).T^\ast(m,\kappa_0)=\frac1C\Big(\frac{r(m,\kappa_0)^{-\alpha(\kappa_0)}}{\alpha(\kappa_0)}-2\ln(2m)+\frac{r(m,-\kappa_0)^{-\alpha(-\kappa_0)}}{-\alpha(-\kappa_0)}\Big).T∗(m,κ0​)=C1​(α(κ0​)r(m,κ0​)−α(κ0​)​−2ln(2m)+−α(−κ0​)r(m,−κ0​)−α(−κ0​)​).

Finally Dλr=diag⁡(λn−i+1)D^{\mathbf r}_\lambda=\operatorname{diag}(\lambda^{n-i+1})Dλr​=diag(λn−i+1) is the dilation of (5).

A system is globally fixed-time stable with settling time at most TTT if the origin is an equilibrium, solutions exist from every initial state, it is Lyapunov stable, and every solution vanishes for all t≥Tt\ge Tt≥T (Definition 1 with Ω=Rn\Omega=\mathbb R^nΩ=Rn).

Formalization targets

Goal: Theorem 30 (p. 1038)

Let the gains and C>0C>0C>0 satisfy (36). There are m∈(0,1)m\in(0,1)m∈(0,1) and κ0∈(0,12n)\kappa_0\in(0,\tfrac1{2n})κ0​∈(0,2n1​) such that, for every T>0T>0T>0 and every λ>0\lambda>0λ>0 with

λ ≥ T∗(m,κ0)/T,\lambda\ \ge\ T^\ast(m,\kappa_0)/T,λ ≥ T∗(m,κ0​)/T,

the feedback u=ωκ(Dλrx)H(Dλrx)u=\omega^H_{\kappa(D^{\mathbf r}_\lambda x)}(D^{\mathbf r}_\lambda x)u=ωκ(Dλr​x)H​(Dλr​x) makes (31) globally fixed-time stable with settling time at most TTT.

Milestones

  • Proposition 24 (p. 1034): gains exist for which (36) holds uniformly in κ\kappaκ, VκV_\kappaVκ​ is C1C^1C1, positive definite and r(κ)\mathbf r(\kappa)r(κ)-homogeneous of degree 2+κ2+\kappa2+κ, and ωκH\omega^H_\kappaωκH​ is globally asymptotically stabilizing.
  • Lemma 31 (p. 1038): on the shell B1−m,1+mκB^\kappa_{1-m,1+m}B1−m,1+mκ​, ∣xj∣|x_j|∣xj​∣ and ∣vj∣|v_j|∣vj​∣ are bounded uniformly in κ\kappaκ.
  • Lemma 32 (p. 1039): on that shell, ∣ωκH−ω0H∣|\omega^H_\kappa-\omega^H_0|∣ωκH​−ω0H​∣ and ∣Vκ−V0∣|V_\kappa-V_0|∣Vκ​−V0​∣ are at most a constant times ∣κ∣min⁡(1,rn)|\kappa|^{\min(1,r_n)}∣κ∣min(1,rn​).
  • Proposition 33 (p. 1040): for every mmm there is κ0(m)>0\kappa_0(m)>0κ0​(m)>0 below which the closed loop is fixed-time stable, with an explicit settling-time bound that coincides with (52) for m≤(17−3)/4m\le(\sqrt{17}-3)/4m≤(17​−3)/4.
  • Theorem 28 (pp. 1036–1037): with an input gain b(t)∈[b‾,bˉ]b(t)\in[\underline b,\bar b]b(t)∈[b​,bˉ] and the feedback ωκ(x)H(x)/b‾\omega^H_{\kappa(x)}(x)/\underline bωκ(x)H​(x)/b​, the closed loop is globally fixed-time stable with settling time at most T∗(m,κ0)T^\ast(m,\kappa_0)T∗(m,κ0​).

Significance

The result gives a static, continuous state feedback for the chain of integrators with an explicit settling-time bound. It is robust to a bounded uncertain input gain, and the rescaled controller meets any prescribed deadline. Unlike time-varying designs, the gains stay bounded, which is what the paper's ISS analysis in §4.3 builds on. The constants in (52) are explicit in terms of CCC and the radii r(m,±κ0)r(m,\pm\kappa_0)r(m,±κ0​), so the rescaling factor λ\lambdaλ is computable.

The results are proved on paper; no machine-checked proof is known. A formalization would check the parameter bookkeeping of the construction: index shifts, exponents, the three-phase settling-time estimate, and the interplay of two different dilations. It would also produce reusable definitions of Carathéodory solutions and of finite-, fixed- and prescribed-time stability, which the platform does not yet have.

Difficulty

The obvious argument uses the Lyapunov function Vκ(x)V_{\kappa(x)}Vκ(x)​ for the varying-degree controller. That fails: κ\kappaκ depends on xxx, so Vκ(x)(x)V_{\kappa(x)}(x)Vκ(x)​(x) acquires a term from the derivative of κ\kappaκ. The proof instead handles three regions separately, with Vκ0V_{\kappa_0}Vκ0​​ outside B1+m0B^0_{1+m}B1+m0​, V0V_0V0​ on the shell B1−m,1+m0B^0_{1-m,1+m}B1−m,1+m0​, and V−κ0V_{-\kappa_0}V−κ0​​ inside B1−m0B^0_{1-m}B1−m0​. On the shell the controller is a perturbation of the linear one, and bounding that perturbation needs uniform Hölder estimates in κ\kappaκ (Lemmas 31–32). The closed loop is only continuous, so solutions need not be unique and every stability claim is about all solutions. Proposition 24 itself is a recursive gain construction whose constants must be uniform in κ\kappaκ.

Formalization scope

States are EuclideanSpace ℝ (Fin n); the paper's index j∈{1,…,n}j\in\{1,\dots,n\}j∈{1,…,n} is j.val + 1. Solutions are Carathéodory solutions on [0,∞)[0,\infty)[0,∞) in integral form, with integrability stated. Every stability property quantifies over all solutions, and existence of a solution from each initial state is part of Lyapunov stability. ⌈y⌋a\lceil y\rfloor^a⌈y⌋a is read as sign⁡(y)∣y∣a\operatorname{sign}(y)|y|^asign(y)∣y∣a; the paper never defines it. V˙\dot VV˙ is the Fréchet derivative applied to the vector field. r(m,κ0)r(m,\kappa_0)r(m,κ0​) and r(m,−κ0)r(m,-\kappa_0)r(m,−κ0​) are the supremum and infimum of the admissible radii.

Hypotheses and readings that differ from the page:

  • The gains and CCC in Theorems 28 and 30 and Proposition 33 are data satisfying (36), not existentially chosen. An unconstrained ∃C\exists C∃C would make (52) false, and Proposition 24 shows (36) is satisfiable.
  • bbb is assumed measurable in Theorem 28.
  • "Adapted" is the feedback divided by b‾\underline bb​, as the page says.
  • Corrected printed slips:
    • (51) lacks ene_nen​.
    • Theorem 30 writes κ0∈(0,1/n)\kappa_0\in(0,1/n)κ0​∈(0,1/n); Theorem 28's (0,12n)(0,\tfrac1{2n})(0,2n1​) is used.
    • Proposition 33 prints κ0(m)∈[−12n,−12n]\kappa_0(m)\in[-\tfrac1{2n},-\tfrac1{2n}]κ0​(m)∈[−2n1​,−2n1​]; the value is positive and at most 12n\tfrac1{2n}2n1​.
    • (37) prints βi−1\beta_{i-1}βi−1​ for βj−1\beta_{j-1}βj−1​.
    • The proof of Lemma 32 prints the exponent of (33) as (rj+1)/(rjβj−1)(r_j+1)/(r_j\beta_{j-1})(rj​+1)/(rj​βj−1​); (33) is used.
  • Lemma 32's maxima are read pointwise, with rn=rn(κ)r_n=r_n(\kappa)rn​=rn​(κ).
  • In Proposition 33 the middle term −2ln⁡(2m)-2\ln(2m)−2ln(2m) of (52) is replaced by max⁡(−2ln⁡(2m), 2ln⁡1+m1−m)\max(-2\ln(2m),\,2\ln\frac{1+m}{1-m})max(−2ln(2m),2ln1−m1+m​): the page's crossing-time estimate −2ln⁡(2m)/C-2\ln(2m)/C−2ln(2m)/C is justified only for m≤(17−3)/4m\le(\sqrt{17}-3)/4m≤(17​−3)/4, where the two bounds coincide.
  • "Explicit" constants are stated as existing.

A formalization in which (36) is dropped, or CCC is chosen freely, or a trajectory is only required to exist, would be trivial or false. Any trivializing reading of this kind is ruled out: stability is required of every solution, and CCC is tied to (36).

Needed infrastructure: signed powers and their Hölder estimates (42), differentiability of VκV_\kappaVκ​, weighted homogeneity, Carathéodory existence for continuous right-hand sides, and comparison lemmas for V˙≤−cV1+α\dot V\le-cV^{1+\alpha}V˙≤−cV1+α. The stability definitions and the comparison lemmas are reusable beyond this mission. Contributions of any of these are welcome.

Selected references

  • Y. Chitour, R. Ushirobira, H. Bouhemou, Stabilization for a Perturbed Chain of Integrators in Prescribed Time, SIAM J. Control Optim. 58(2), 1022–1048, 2020. https://doi.org/10.1137/19M1285937
  • Y. Hong, Finite-time stabilization and stabilizability of a class of controllable systems, Systems Control Lett. 46, 231–236, 2002. https://doi.org/10.1016/S0167-6911(02)00119-6
  • M. Harmouche, S. Laghrouche, Y. Chitour, M. Hamerlain, Stabilisation of perturbed chains of integrators using Lyapunov-based homogeneous controllers, Int. J. Control 90, 2631–2640, 2017. https://doi.org/10.1080/00207179.2016.1262967
  • F. Lopez-Ramirez, D. Efimov, A. Polyakov, W. Perruquetti, Fixed-time output stabilization and fixed-time estimation of a chain of integrators, Int. J. Robust Nonlinear Control 28, 4647–4665, 2018. https://doi.org/10.1002/rnc.4275
  • Y. Song, Y. Wang, J. Holloway, M. Krstić, Time-varying feedback for regulation of normal-form nonlinear systems in prescribed finite time, Automatica 83, 243–251, 2017. https://doi.org/10.1016/j.automatica.2017.06.008
  • S. P. Bhat, D. S. Bernstein, Geometric homogeneity with applications to finite-time stability, Math. Control Signals Systems 17, 101–127, 2005. https://doi.org/10.1007/s00498-005-0151-x
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Dynamical SystemsOperations ResearchProbability+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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Operations ResearchOptimization·Captain: mikedeng1

Optimizing Static Linear Feedback: Gradient Method II: The Gradient Flow Stays in the Sublevel Set and Converges Exponentially under State FeedbackResearch Paper

Motivation

The linear-quadratic regulator (LQR) is the basic problem of optimal control: steer a linear system x˙=Ax+Bu\dot x = Ax + Bux˙=Ax+Bu so as to minimize an integrated quadratic cost of state and input. When the full state is measured, the optimal law is a static linear feedback u=−Kxu = -Kxu=−Kx obtained from an algebraic Riccati equation. When only an output y=Cxy = Cxy=Cx is measured, the optimal static output feedback u=−Kyu = -Kyu=−Ky has no closed form, and the problem is nonconvex. In both cases the cost can be written as a function f(K)f(K)f(K) of the gain alone, which makes it natural to minimize fff by gradient methods directly in the space of gains. This view goes back to Levine and Athans (1970) for output feedback and was revived in reinforcement learning by Fazel, Ge, Kakade and Mesbahi (2018), who proved global convergence of policy gradient for discrete-time state-feedback LQR.

Fatkhullin and Polyak (arXiv:2004.09875v2, SIAM J. Control Optim. 2021) carry out this program for the continuous-time problem. They show that fff is coercive, that it is LLL-smooth on every sublevel set, and that under state feedback it satisfies a gradient-domination (Łojasiewicz–Polyak) inequality. From these properties they derive convergence of the continuous gradient flow and of the discrete gradient method. This mission formalizes the continuous part, Theorem 4.1.

Setting

Fix real matrices A∈Rn×nA\in\mathbb R^{n\times n}A∈Rn×n, B∈Rn×mB\in\mathbb R^{n\times m}B∈Rn×m, C∈Rr×nC\in\mathbb R^{r\times n}C∈Rr×n and symmetric positive definite weights Q∈Rn×nQ\in\mathbb R^{n\times n}Q∈Rn×n, R∈Rm×mR\in\mathbb R^{m\times m}R∈Rm×m and covariance Σ∈Rn×n\Sigma\in\mathbb R^{n\times n}Σ∈Rn×n. A gain is K∈Rm×rK\in\mathbb R^{m\times r}K∈Rm×r, and the closed-loop matrix is AK=A−BKCA_K = A - BKCAK​=A−BKC. A square matrix is Hurwitz if all its eigenvalues have negative real part. The stabilizing set is

S={K:AK is Hurwitz}.\mathcal S = \{K : A_K \text{ is Hurwitz}\}.S={K:AK​ is Hurwitz}.

For K∈SK\in\mathcal SK∈S, let X(K)X(K)X(K) and Y(K)Y(K)Y(K) be the unique solutions of the Lyapunov equations

AK⊤X+XAK+C⊤K⊤RKC+Q=0,AKY+YAK⊤+Σ=0.A_K^\top X + XA_K + C^\top K^\top RKC + Q = 0,\qquad A_KY + YA_K^\top + \Sigma = 0 .AK⊤​X+XAK​+C⊤K⊤RKC+Q=0,AK​Y+YAK⊤​+Σ=0.

The LQR cost is f(K)=Tr(X(K)Σ)f(K) = \mathrm{Tr}(X(K)\Sigma)f(K)=Tr(X(K)Σ). It equals the expected infinite-horizon quadratic cost when the initial state has covariance Σ\SigmaΣ. Its gradient with respect to the Frobenius inner product ⟨M,N⟩=Tr(M⊤N)\langle M,N\rangle = \mathrm{Tr}(M^\top N)⟨M,N⟩=Tr(M⊤N) is

∇f(K)=2 (RKC−B⊤X(K)) Y(K) C⊤.\nabla f(K) = 2\,(RKC - B^\top X(K))\,Y(K)\,C^\top .∇f(K)=2(RKC−B⊤X(K))Y(K)C⊤.

Given a known stabilizing gain K0∈SK_0\in\mathcal SK0​∈S, the sublevel set is S0={K∈S:f(K)≤f(K0)}\mathcal S_0 = \{K\in\mathcal S : f(K)\le f(K_0)\}S0​={K∈S:f(K)≤f(K0​)}. The gradient flow is the ODE

K˙(t)=−∇f(K(t)),K(0)=K0.\dot K(t) = -\nabla f(K(t)),\qquad K(0) = K_0 .K˙(t)=−∇f(K(t)),K(0)=K0​.

State feedback (SLQR) is the case C=IC = IC=I; there fff is written fSf_SfS​, and K∗K_*K∗​ denotes a minimizer of fSf_SfS​ on S\mathcal SS. Norms: ∥⋅∥F\|\cdot\|_F∥⋅∥F​ is the Frobenius norm and ∥⋅∥\|\cdot\|∥⋅∥ the spectral norm. λ1(M)\lambda_1(M)λ1​(M) is the smallest eigenvalue of a symmetric MMM.

Formalization targets

Goal: Theorem 4.1 for state feedback

For C=IC=IC=I, let L>0L>0L>0 be a Lipschitz constant of ∇f\nabla f∇f on S0\mathcal S_0S0​ and let μ\muμ be the constant (3.11),

μ=λ1(R)λ12(Σ)λ1(Q)8fS(K∗)(∥A∥+∥B∥2fS(K0)/(λ1(Σ)λ1(R)))2.\mu = \frac{\lambda_1(R)\lambda_1^2(\Sigma)\lambda_1(Q)}{8f_S(K_*)\big(\|A\| + \|B\|^2 f_S(K_0)/(\lambda_1(\Sigma)\lambda_1(R))\big)^2}.μ=8fS​(K∗​)(∥A∥+∥B∥2fS​(K0​)/(λ1​(Σ)λ1​(R)))2λ1​(R)λ12​(Σ)λ1​(Q)​.

Then the flow has a solution on [0,∞)[0,\infty)[0,∞), and every solution stays in S0\mathcal S_0S0​, has f(Kt)f(K_t)f(Kt​) nonincreasing, has ∇f(Kt)→0\nabla f(K_t)\to0∇f(Kt​)→0 and min⁡0≤t≤T∥∇f(Kt)∥F2≤f(K0)/T\min_{0\le t\le T}\|\nabla f(K_t)\|_F^2\le f(K_0)/Tmin0≤t≤T​∥∇f(Kt​)∥F2​≤f(K0​)/T, and

∥Kt−K∗∥F≤2L(f(K0)−f(K∗))μ e−μt(t≥0).\|K_t - K_*\|_F \le \frac{\sqrt{2L(f(K_0)-f(K_*))}}{\mu}\,e^{-\mu t}\qquad(t\ge0).∥Kt​−K∗​∥F​≤μ2L(f(K0​)−f(K∗​))​​e−μt(t≥0).

Milestones

In attack order:

  1. Existence of a minimizer (Corollary 3.10).
  2. The gradient formula (Lemma 3.11).
  3. Existence of a Lipschitz constant of ∇f\nabla f∇f on S0\mathcal S_0S0​ (Theorem 3.15, qualitative).
  4. The gradient-domination inequality 12∥∇fS(K)∥F2≥μ(fS(K)−fS(K∗))\tfrac12\|\nabla f_S(K)\|_F^2\ge\mu(f_S(K)-f_S(K_*))21​∥∇fS​(K)∥F2​≥μ(fS​(K)−fS​(K∗​)) on S0\mathcal S_0S0​ (Theorem 3.17).
  5. The energy identity ddtf(Kt)=−∥∇f(Kt)∥F2\tfrac{d}{dt}f(K_t) = -\|\nabla f(K_t)\|_F^2dtd​f(Kt​)=−∥∇f(Kt​)∥F2​.
  6. The integral bound of Appendix D.1.
  7. The output-feedback part of Theorem 4.1 (general CCC with rank⁡C=r\operatorname{rank} C = rrankC=r): existence, invariance of S0\mathcal S_0S0​, monotonicity and (4.2).

Significance

The theorem certifies a simple, model-based procedure: start from any stabilizing gain and follow the negative gradient of the cost. The iterate never loses stability, and it converges exponentially to the optimal gain. The same happens for state feedback even though neither fff nor S\mathcal SS is convex. For output feedback it guarantees convergence to stationarity with an explicit O(1/T)O(1/T)O(1/T) rate. The continuous-time result is the template for the discrete gradient method of the same paper (Theorem 4.2) and for policy-gradient analyses of LQR in learning-based control.

The result is proved in the paper. The paper writes out the proof of (4.2) in Appendix D.1. It describes the whole proof as a replica of Theorems 8 and 9 of Polyak 1963, which treat functions satisfying the Łojasiewicz–Polyak inequality on the whole space. No machine-checked version of any of these statements is known. A formal proof would give the first verified treatment of LQR as an optimization problem over gains. It needs Lyapunov equations, the stabilizing set and the cost, together with the analytic facts on which the policy-gradient literature rests: coercivity, smoothness on sublevel sets, and gradient domination.

Difficulty

The obvious argument is the textbook convergence proof for gradient flows of smooth functions satisfying the Łojasiewicz–Polyak inequality. That proof assumes the function is defined and smooth on the whole space. Here fff lives only on the open set S\mathcal SS, blows up at its boundary, is unbounded on S\mathcal SS and is not globally LLL-smooth. The Łojasiewicz–Polyak inequality holds only on S0\mathcal S_0S0​, with a constant that depends on K0K_0K0​. The work therefore lies in keeping the trajectory inside S0\mathcal S_0S0​ and showing it exists for all time. This requires compactness of S0\mathcal S_0S0​ (coercivity of fff) and a positive distance from S0\mathcal S_0S0​ to the boundary of S\mathcal SS. Local ODE existence alone gives neither. The explicit constant μ\muμ additionally requires lower bounds on solutions of Lyapunov equations and an upper bound on ∥K∥F\|K\|_F∥K∥F​ over S0\mathcal S_0S0​.

Formalization scope

Matrices are Matrix (Fin p) (Fin q) ℝ. Hurwitz means every complex eigenvalue of the complexified matrix has negative real part. X(K)X(K)X(K) and Y(K)Y(K)Y(K) are the unique solutions of their Lyapunov equations. Where the solution is not unique (possible only off S\mathcal SS) they take the value 000, and no statement uses these off-S\mathcal SS values. ∇f\nabla f∇f is defined by formula (3.3), and Lemma 3.11 states that it is the Fréchet derivative with respect to the Frobenius inner product. A solution of the flow is a curve with K(0)=K0K(0)=K_0K(0)=K0​ that stays in S\mathcal SS for t≥0t\ge0t≥0. Its entries have the prescribed derivative within [0,∞)[0,\infty)[0,∞). Global existence and invariance of S0\mathcal S_0S0​ are conclusions, never hypotheses. Assuming a global solution, or a solution confined to S0\mathcal S_0S0​, would trivialize the theorem, and that encoding is excluded. The case C=IC=IC=I is a matrix argument CCC with C=1C=1C=1. λ1\lambda_1λ1​ is the minimum of the (unsorted) eigenvalues, and the spectral norm is λmax⁡(M⊤M)\sqrt{\lambda_{\max}(M^\top M)}λmax​(M⊤M)​. "Monotone decreasing" is rendered as nonincreasing. min⁡0≤t≤T\min_{0\le t\le T}min0≤t≤T​ is rendered as the existence of a point of [0,T][0,T][0,T] where the bound holds.

The standing assumptions of p. 3 are hypotheses wherever they apply: K0∈SK_0\in\mathcal SK0​∈S, Q,R,Σ≻0Q,R,\Sigma\succ0Q,R,Σ≻0, rank⁡C=r\operatorname{rank}C=rrankC=r, and B≠0B\ne0B=0. Deviations from the printed paper:

  • The paper's explicit Lipschitz constant (3.8) is false as printed; the planning notes record counterexamples for both output and state feedback. The goal therefore takes LLL as any Lipschitz constant of ∇f\nabla f∇f on S0\mathcal S_0S0​, which is the paper's own definition of LLL-smoothness (§3.6). Theorem 3.15 enters only in its qualitative form, as the existence of such an LLL.
  • The set-builder for S\mathcal SS on p. 3 writes Rm×n\mathbb R^{m\times n}Rm×n; gains are m×rm\times rm×r.
  • The optimal gain K∗K_*K∗​ is a hypothesis (its existence is Corollary 3.10), and f(K∗)>0f(K_*)>0f(K∗​)>0 is not assumed.

A complete development needs the following: Lyapunov equations and their solution theory (uniqueness, positivity, integral representation), continuity and differentiability of K↦X(K)K\mapsto X(K)K↦X(K) on S\mathcal SS, coercivity of fff, global existence for ODEs confined to a compact invariant set, and the Łojasiewicz–Polyak argument for flows on a subset. The Lyapunov and stabilizing-set layer is reusable across control missions. Proofs of any milestone, and of auxiliary lemmas such as Lemmas 3.8, A.5, C.1–C.3, are welcome.

Selected references

  • I. Fatkhullin, B. Polyak, Optimizing Static Linear Feedback: Gradient Method, SIAM J. Control Optim. 59 (2021); preprint arXiv:2004.09875v2. https://arxiv.org/abs/2004.09875
  • M. Fazel, R. Ge, S. Kakade, M. Mesbahi, Global Convergence of Policy Gradient Methods for the Linear Quadratic Regulator, ICML 2018. https://arxiv.org/abs/1801.05039
  • W. S. Levine, M. Athans, On the determination of the optimal constant output feedback gains for linear multivariable systems, IEEE Trans. Automat. Control 15 (1970). https://doi.org/10.1109/TAC.1970.1099363
  • H. Karimi, J. Nutini, M. Schmidt, Linear Convergence of Gradient and Proximal-Gradient Methods Under the Polyak–Łojasiewicz Condition, ECML PKDD 2016. https://arxiv.org/abs/1608.04636
  • B. T. Polyak, Gradient methods for the minimisation of functionals, USSR Comput. Math. Math. Phys. 3 (1963), 864–878. https://doi.org/10.1016/0041-5553(63)90382-3
11 thms1 active userReviewed
Dynamical SystemsOperations ResearchProbability+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
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Operations ResearchOptimizationProbability+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
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