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Extremum and Nash Equilibrium Seeking with Delays and PDEs: Designs & Applications

T0 review · 3 major / 5 minor · reviewed 2026-08-12 · deepseek-v4-flash

Pith's one-line read Boundary-control extremum seeking drives games whose players act through delays or heat PDEs to a small neighborhood of the Nash equilibrium.

desk verdict A useful consolidation of the authors' ES/NES results for PDE-constrained games, but the central stability claims rest on asserted small-gain verifications that the appendices do not actually carry out. read the letter →

arxiv 2411.13234 v1 pith:WAZVDRYU submitted 2024-11-20 math.OC cs.SYeess.SY

classification math.OCcs.SYeess.SY MSC 93C2091A1093C23
keywords extremumseekingNashequilibriumpartialdifferentialequationstimedelaysboundarycontrolsmall-gainanalysisaveragingtheorynoncooperativegames
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

Extremum seeking is a model-free way to optimize an unknown map in real time using only output measurements; Nash equilibrium seeking extends it to games where competing players each maximize their own payoff. This paper claims that the method keeps working when a player's action reaches the payoff function through infinite-dimensional dynamics: a time delay, a heat (diffusion) equation, or a mixed pair of one transport and one heat equation. For quadratic noncooperative games with weak coupling and a diagonally dominant Hessian, the proposed decentralized boundary-control laws make the closed-loop system locally exponentially converge to a small neighborhood of the Nash equilibrium, with propagated actions within $O(|a|+1/\omega)$ of the optimum. The significance is that real-time, model-free optimization can be applied to physical and networked systems where actuation is blurred by transport or diffusion, such as traffic bottlenecks, thermal manufacturing, and source seeking.

What carries the argument

The load-bearing object is the averaged infinite-dimensional closed loop: a finite-dimensional ODE for the estimated gradient $\hat{G}$ coupled through its boundary condition to a transport or heat PDE that represents the compensated actuator error. A reduction-like transformation, the finite-spectrum assignment in equations (65) and (132)-(133), rewrites the loop so that the ODE sees the boundary control signal directly, and the boundary laws (58), (27), and (122) use only the player's own Hessian diagonal estimate plus an integral of the PDE state. Exponential stability of the average system is established by checking an input-to-state small-gain condition for the PDE-ODE interconnection, where the game coupling $\epsilon$ appears in the interconnection gains, and an averaging theorem for infinite-dimensional systems then converts that stability into convergence of the original periodic closed loop.

What would settle it

Compute the input-to-state gains $\gamma_0$ and $b_3$ for the averaged two-player heat-PDE loop (70)-(73) from the variation-of-constants formula and the integral bounds in Appendix A, for example with $D_1=1$, $D_2=2$, and diagonal-dominant Hessian entries, and test the small-gain inequalities (283) along a sequence $\epsilon\to 0$. If the gain product fails to stay below one, or if a direct simulation of the averaged loop for those parameters shows no exponential decay, the asserted verification is wrong and Theorem 1's conclusion is unsupported.

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Extended reading notes

Core claim

On the paper's own terms, the central discovery is a design-and-stability statement: in an $N$-player quadratic game where each player measures only its own payoff and knows only its own delay or diffusion domain, a boundary controller that compensates that player's actuation PDE lets all players collectively find the Nash equilibrium. Theorem 1 covers arbitrary distinct heat PDEs, Theorem 2 covers arbitrary distinct delays, and Theorem 3 covers a duopoly with one transport player and one heat player. In each case, the closed-loop error system has a unique locally exponentially stable periodic solution, and the propagated action vector satisfies $\limsup_{t\to\infty}|\Theta(t)-\Theta^*|=O(|a|+1/\omega)$, with the finer bounds $|\theta_1(t)-\theta_1^*|=O(a_1+1/\omega)$ and $|\theta_2(t)-\theta_2^*|=O(a_2e^{D_2\sqrt{\omega}/2}+1/\omega)$ in the heterogeneous duopoly. The paper also shows that scalar extremum seeking with PDE actuation is a corollary of the Nash results, and it catalogues a broad set of PDE types for which the same template, trajectory-generated probing signals plus boundary control, applies.

Load-bearing premise

The whole theorem rests on the claim, stated but not fully derived in the appendices, that the averaged PDE-ODE loop satisfies the small-gain condition needed for exponential stability for sufficiently small coupling $\epsilon$; if that verification fails, the convergence result collapses.

Editorial extensions

If this is right

  • Theorem 1: in the heat-PDE game, $\limsup_{t\to\infty}|\Theta(t)-\Theta^*|=O(|a|+1/\omega)$ while the boundary inputs satisfy $\limsup_{t\to\infty}|\theta(t)-\theta^*|=O(|a|e^{\max_i D_i\sqrt{\omega}/2}+1/\omega)$, so the exponential probing amplification is confined to the input side.
  • Theorem 2: with arbitrary distinct input delays, the predictor feedback (27) gives $\limsup_{t\to\infty}|\theta(t)-\theta^*|=O(|a|+1/\omega)$, the same residual order as a delay-free game.
  • Theorem 3: in the transport-heat duopoly, the transport player converges to $O(a_1+1/\omega)$ and the heat player to $O(a_2e^{D_2\sqrt{\omega}/2}+1/\omega)$ of their Nash actions, despite each player compensating only its own PDE.
  • Scalar extremum seeking with PDE actuation follows as a corollary (Remark 1), so every single-agent result in the paper's PDE catalogue inherits the same stability template.
  • The boundary-control-plus-probing template is listed for reaction-advection-diffusion, wave, variable-delay, and distributed-delay actuation (Table I), indicating the design is not tied to heat or transport equations specifically.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The numerical example uses $\epsilon=1$, outside the theorem's stated $0<\epsilon<1$ range, and still converges; I take this as evidence that the small-coupling assumption is conservative, though the paper does not promote this observation to a theorem.
  • The residual bound for a heat-PDE player contains $e^{D\sqrt{\omega}/2}$, so a long diffusion domain forces a practical trade-off: to keep the Nash neighborhood tight one must shrink the probing amplitude, which in turn weakens the gradient estimate. I expect this trade-off to be the practical bottleneck in thermal and diffusion applications.
  • The small-gain framework used for two PDE classes is generic enough that the same proof structure should cover games with more than two heterogeneous players, or mixtures involving wave and reaction-advection-diffusion dynamics, once the missing gain verifications are supplied.
  • Since the payoffs are quadratic, a standard local-quadratic approximation argument suggests the theorems extend to smooth strictly concave payoffs in a neighborhood of the equilibrium; checking this explicitly would be a natural follow-up.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 5 minor

Summary. The paper presents boundary-control extremum seeking (ES) and Nash equilibrium seeking (NES) algorithms for quadratic noncooperative games in which players' actions are filtered through delays, heat PDEs, or a heterogeneous transport-heat PDE pair. The main theoretical results, Theorems 1-3, assert that with sufficiently large filter gains and frequencies and sufficiently small coupling ε, the closed-loop system has a locally exponentially stable periodic solution and converges to an O(|a|+1/ω) neighborhood of the Nash equilibrium (with additional exponentially growing amplitude factors in the input-side bounds). The paper also reviews applications to traffic, drilling, source seeking, additive manufacturing, bioreactors, and neuromuscular stimulation, and includes a duopoly simulation.

Significance. If fully proven, the results would be a significant extension of model-free ES/NES to infinite-dimensional actuator dynamics, providing constructive boundary controllers and explicit residual bounds. The paper is well organized, connects to a large body of prior work, and the simulation illustrates the proposed laws. The main limitations are in the proof apparatus: the central stability theorems are reduced to small-gain verifications that are asserted rather than demonstrated, and at least one parameter mapping appears inconsistent with the plant boundary condition. The survey and application sections are informative, but the technical contribution is not yet fully supported.

major comments (3)
  1. [Appendix A (Theorem 1), Eqs. (278)-(281)] The verification of assumptions (A1)-(A7) of [34, Theorem 8.2] is not carried out. In particular, the plant's boundary at x=0 is the homogeneous Neumann condition ∂x u_i^av(0,t)=0 (Eq. (280)), while the parameter list assigns φ0(0,u_i^av,¯G_i^av)=b1 u_i^av(0,t) with b1<0. Since the small-gain condition (8.3.24) and the asserted O(ε) scaling of γ0 and b3 depend on the boundary operator at x=0, the current text does not establish the exponential stability of the averaged system (70)-(73). Please provide the correct parameter mapping for a Neumann boundary or show directly that the resulting ISS gains scale as claimed.
  2. [Appendices B and C (Theorems 2 and 3)] The proofs of Theorems 2 and 3 rely on the same pattern: the average closed-loop systems (286)-(288) and (292)-(296) are claimed to satisfy the hypotheses (H1)-(H2) or (A1)-(A7) of [34, Theorems 8.1 and 8.2], and the small-gain condition is asserted to hold for sufficiently small ε. No explicit verification of the gains (b3, γ0, γ1) or of the small-gain inequality is given; phrases such as 'can be readily verified' (after Eq. (297)) and 'it is not difficult to see' (Eqs. (66) and (134)) are not sufficient for a journal publication. Because local exponential stability of the average system is the load-bearing premise for the subsequent averaging argument and residual bounds, these steps must be supplied or replaced by precise pointers to the corresponding theorems in [60].
  3. [Theorems 1 and 3, Eqs. (76) and (148)] The residual bounds for the input-side estimates contain factors e^{max(D_i)√ω/2} and e^{D2√ω/2}, which grow with ω. The theorems state existence of sufficiently large ω while simultaneously using bounds that deteriorate as ω grows. Without an explicit scaling of the dither amplitudes a_i with ω (e.g., a_i = o(e^{-D_i√ω/2})), the assertion that θ(t) converges to a small neighborhood of θ* is not justified for the claimed parameter regime. Please state the admissible parameter scaling or reformulate the residual bound as a trade-off.
minor comments (5)
  1. [Section I] The word 'dealts' in the opening sentence should be 'deals'.
  2. [Section IV] The symbol D is overloaded: it denotes the delay matrix, the vector of domain lengths, the diffusion operator, and the spatial domain length. This causes confusion in equations such as (33) and (62); please use distinct notation or explicitly disambiguate.
  3. [Section X] In the sentence defining the low-pass filter, 'steads for convolution' should be 'stands for convolution'.
  4. [Appendix H] The heading 'THE BASIC IDEA OF NASH EQULIBRIUM SEEKING' contains a typo; it should be 'EQUILIBRIUM'.
  5. [Section VII] The simulation uses ε=1, which is outside the theorem's stated 0<ε<1. The text acknowledges that this suggests the analysis may be conservative, but the simulation should not be read as validation of the theorem's assumptions; this limitation should be stated more prominently.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the convergence theorems are not forced by construction; the main proof gaps are omitted small-gain verifications, not circular reductions.

full rationale

None of the load-bearing steps reduces to its own inputs by construction. Theorems 1–3 assert existence of design parameters (sufficiently large c and ω, sufficiently small ε) and derive exponential convergence of an averaged PDE–ODE loop to a residual set of size O(|a|+1/ω); the residual bounds are obtained via the general infinite-dimensional averaging theorem [25] after exponential stability of the average system is established, not by fitting parameters to the claimed Nash equilibrium. The stability verification in Appendices A–C relies on the Karafyllis–Krstić ISS small-gain theorems [34] and contains genuine omissions, e.g., the assertions that conditions “can be readily verified” (Appendix A, after Eq. (281)) and that “with some mathematical manipulations, it is not difficult to see” (Eq. (66) and Eq. (134)). There is also a possible correctness concern in Appendix A, where the listed mapping φ0(0,u_i,¯G_i)=b_1 u_i(0,t) is asserted while the plant boundary condition is the homogeneous Neumann condition ∂_x u_i(0,t)=0 (Eq. (280)); these are incomplete or mismatched verifications, but they are not circularity, because [34] is an external mathematical theorem and the paper does not define its target result into its assumptions. Self-citations to [18], [61], [62], [63], [65] supply design templates and conference versions of related games, but the central convergence claims are argued from the averaged closed loop and independent small-gain/averaging theorems rather than being justified solely by those citations. Therefore the paper is not circular, though its proof completeness is imperfect.

Assumptions & free parameters 0 free parameters · 6 assumptions · 0 invented entities

The central claims rest on standard results in averaging and small-gain theory, plus domain assumptions about quadratic games and information structure. The key unverified premise is the satisfaction of the small-gain theorem hypotheses for the averaged PDE-ODE loops, which the paper asserts but does not demonstrate.

assumptions (6)
  • standard math Averaging theorem for infinite-dimensional systems (Hale and Lunel 1990) applies to the closed-loop parabolic/hyperbolic PDE-ODE systems.
    Used in Appendices D and E to conclude that exponential stability of the average system implies existence of a unique locally exponentially stable periodic solution and O(1/ω) closeness for the time-varying system.
  • standard math Small-gain theorems for ODE-PDE loops (Karafyllis and Krstic 2018, Theorems 8.1, 8.2, 11.5) are applicable to the averaged closed-loop system.
    Invoked in Appendices F, A, B, C to prove exponential stability of the origin of the average system via small-gain conditions.
  • standard math Levy-Desplanques theorem: strictly diagonally dominant matrices are nonsingular.
    Used in Section II to guarantee existence and uniqueness of the Nash equilibrium theta* = -H^{-1}h under Assumption 1.
  • domain assumption Payoff functions are quadratic, strictly concave in each player's own action, with diagonal dominance of the Hessian and equal coupling weights (Assumptions 1-3).
    Restricts the game class; the convergence results are local to the Nash equilibrium of such quadratic approximations.
  • domain assumption Players only know their own payoff, their own constant delay or domain length D_i, and the parameters of their own probing signals; no information sharing.
    Defines the decentralized model-free setting; the control laws (58) and (122) require the distributed state u_i of the player's own PDE error system.
  • ad hoc to paper The averaged PDE-ODE closed-loop systems satisfy the assumptions (A1)-(A7) and (H1)-(H2) of the small-gain theorems with the specific gains stated in Appendices A-C.
    The paper asserts this 'can be readily verified' but does not actually carry out the verification. This is the load-bearing unproven premise of Theorems 1-3.

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Cite this review

Pith. "Pith review of Extremum and Nash Equilibrium Seeking with Delays and PDEs: Designs & Applications." pith.science (2026). https://pith.science/paper/WAZVDRYU

@misc{pith2026241113234,
  author       = {Pith},
  title        = {Pith review of: Extremum and Nash Equilibrium Seeking with Delays and PDEs: Designs & Applications},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/WAZVDRYU}},
  note         = {Machine review of arXiv:2411.13234}
}
read the original abstract

The development of extremum seeking (ES) has progressed, over the past hundred years, from static maps, to finite-dimensional dynamic systems, to networks of static and dynamic agents. Extensions from ODE dynamics to maps and agents that incorporate delays or even partial differential equations (PDEs) is the next natural step in that progression through ascending research challenges. This paper reviews results on algorithm design and theory of ES for such infinite-dimensional systems. Both hyperbolic and parabolic dynamics are presented: delays or transport equations, heat-dominated equation, wave equations, and reaction-advection-diffusion equations. Nash equilibrium seeking (NES) methods are introduced for noncooperative game scenarios of the model-free kind and then specialized to single-agent optimization. Even heterogeneous PDE games, such as a duopoly with one parabolic and one hyperbolic agent, are considered. Several engineering applications are touched upon for illustration, including flow-traffic control for urban mobility, oil-drilling systems, deep-sea cable-actuated source seeking, additive manufacturing modeled by the Stefan PDE, biological reactors, light-source seeking with flexible-beam structures, and neuromuscular electrical stimulation.

Figures

Figures reproduced from arXiv: 2411.13234 by the authors.

Figure 2
Figure 2. Block diagram illustrating the Nash Equilibrium seeking strategy [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 1
Figure 1. Nash equilibrium seeking schemes applied by two players ( [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 3
Figure 3. Nash equilibrium seeking in a duopoly (N = 2) noncooperative game with players acting through heat PDE dynamics. As in (1), we consider games where the payoff function yi(t)=Ji(D[θ(t)])=Ji(Θ(t)) of each player is quadratic [8], [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figures from the paper (31 more)
Figure 4
Figure 4. Figure 4: Block diagram illustrating the Nash Equilibrium seeking strategy [PITH_FULL_IMAGE:figures/full_fig_p006_4.png]
Figure 5
Figure 5. Figure 5: Nash equilibrium seeking in a heterogeneous noncooperative game [PITH_FULL_IMAGE:figures/full_fig_p009_5.png]
Figure 6
Figure 6. Figure 6: Block diagram illustrating the Nash Equilibrium seeking strategy [PITH_FULL_IMAGE:figures/full_fig_p010_6.png]
Figure 7
Figure 7. Figure 7: (a) actions’ time histories and (b) payoffs’ time histories for [PITH_FULL_IMAGE:figures/full_fig_p013_7.png]
Figure 8
Figure 8. Figure 8: Actions’ time histories for P1 and P2 for distinct values of the coupling coefficient (ϵ = 0.75, ϵ = 0.5 and ϵ = 0.25). For maximization problems, the unknown nonlinear map is assumed to be locally quadratic, such that Q(Θ) = y ∗ + H 2 (Θ − Θ ∗ ) 2 , (153) where Θ∗ , y…
Figure 9
Figure 9. Figure 9: Evolution of the infinite-dimensional states [PITH_FULL_IMAGE:figures/full_fig_p014_9.png]
Figure 10
Figure 10. Figure 10: Fig. 11 shows the structure of the proof, divided into [PITH_FULL_IMAGE:figures/full_fig_p015_10.png]
Figure 10
Figure 10. Figure 10: A general block diagram for implementation of ES control design for PDE connections ( [PITH_FULL_IMAGE:figures/full_fig_p016_10.png]
Figure 11
Figure 11. Figure 11: Structure of the stability proof for the closed-loop system. capacity drop can be caused by lane-drop, hills, tunnel, bridge or curvature on the road. If incoming traffic flow remains unchanged, traffic congestion forms upstream of the bottleneck because the upstream …
Figure 12
Figure 12. Figure 12: Traffic on a freeway segment with lane-drop. [PITH_FULL_IMAGE:figures/full_fig_p017_12.png]
Figure 13
Figure 13. Figure 13: Quadratic fundamental diagram for the clear Zone C and the [PITH_FULL_IMAGE:figures/full_fig_p018_13.png]
Figure 14
Figure 14. Figure 14: Block diagram for implementation of ES control design for the nonlinear LWR PDE model. [PITH_FULL_IMAGE:figures/full_fig_p020_14.png]
Figure 15
Figure 15. Figure 15: Picture showing the topside of a drilling rig. [PITH_FULL_IMAGE:figures/full_fig_p020_15.png]
Figure 16
Figure 16. Figure 16: Cascade of wave PDE with a static map y(Θ(t)) = Q(Θ(t)). The extremum y(t) = y ∗ is achieved for Θ(t) = Θ∗. Wave PDEs are used generally to model different sort of processes such as mechanical, acoustics, electromagnetic and fluid dynamics. formation and it is the dow…
Figure 17
Figure 17. Figure 17: Motivating example - underwater search: xe represents the relative linear position of the source signal with respect to the sensor. The control task aims to drive the sensor to the source signal, meaning that xe(t) → 0 (or to a small neighborhood of zero) as t → +∞. T…
Figure 18
Figure 18. Figure 18: Gradient extremum seeking control loop. B. Trajectory Generation for the Probing Signal The perturbation S(t) is adapted from the basic ES scheme in order to accommodate actuation dynamics. The trajectory generation problem, as described in [44, Chapter12], is out￾lin…
Figure 19
Figure 19. Figure 19: The cascade of the PDE dynamics and the ODE integrator. [PITH_FULL_IMAGE:figures/full_fig_p023_19.png]
Figure 20
Figure 20. Figure 20: Schematic of one-phase Stefan problem [40], [41]. The temperature [PITH_FULL_IMAGE:figures/full_fig_p023_20.png]
Figure 21
Figure 21. Figure 21: Control objective of the Stefan problem. We aim to design a heat flux input [PITH_FULL_IMAGE:figures/full_fig_p024_21.png]
Figure 23
Figure 23. Figure 23: Extremum seeking control loop applied to the one-phase Stefan [PITH_FULL_IMAGE:figures/full_fig_p024_23.png]
Figure 24
Figure 24. Figure 24: Extremum seeking scheme for tubular bioreactors. [PITH_FULL_IMAGE:figures/full_fig_p026_24.png]
Figure 25
Figure 25. Figure 25: Basic gradient ES scheme for tubular bioreactors modeled by RAD-PDEs. [PITH_FULL_IMAGE:figures/full_fig_p026_25.png]
Figure 26
Figure 26. Figure 26: Light-source seeking with a coupled flexible beam [PITH_FULL_IMAGE:figures/full_fig_p027_26.png]
Figure 27
Figure 27. Figure 27: Mechanical apparatus for NMES experimental tests. The point [PITH_FULL_IMAGE:figures/full_fig_p027_27.png]
Figure 28
Figure 28. Figure 28: Open-loop responses for different step-current-inputs of a stroke patient with delays of order 300ms. Extracted from [67]. limitation is that a PID controller is designed for linear sys￾tems, but the neuromuscular plant, which is being controlled, is nonlinear, time-v…
Figure 29
Figure 29. Figure 29: Block diagram of the closed-loop system for NMES using discrete [PITH_FULL_IMAGE:figures/full_fig_p028_29.png]
Figure 30
Figure 30. Figure 30: The graphic portrays the angular elbow joint movement performed by the stroke patient without the help of the proposed NMES controller. It can be seen that the stroke subject is not able to actively contract his arm to the final flexion position. 0 40 80 120 140 180 2…
Figure 31
Figure 31. Figure 31: Output responses for a stroke patient: PID with fixed gains (Kp = 1 , Ki = 1 , Kd = 1) not guaranteeing an acceptable trajectory tracking after 120 seconds. APPENDIX A PROOF OF THEOREM 1 The proof of Theorem 1 follows steps similar to those employed to prove the resul…
Figure 32
Figure 32. Figure 32 [PITH_FULL_IMAGE:figures/full_fig_p031_32.png]
Figure 33
Figure 33. Figure 33: Deterministic Nash seeking schemes applied by players in a duopoly [PITH_FULL_IMAGE:figures/full_fig_p035_33.png]
Figure 34
Figure 34. Figure 34: The simplest perturbation-based extremum seeking scheme for a [PITH_FULL_IMAGE:figures/full_fig_p036_34.png]

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Lie-Bracket Nash Equilibrium Seeking with Bounded Update Rates for Noncooperative Games

    math.OC 2025-01 accept novelty 5.0 of 10

    A bounded-update-rate extremum seeking controller drives players in quadratic noncooperative games to a small neighborhood of the Nash equilibrium, with local exponential convergence shown via Lie-bracket averaging.

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Pith tools

Reviewed August 12, 2026 · model on record in the stance chip above.