Integral Formulation of QENDy for Robust Nonlinear System Identification
Pith reviewed 2026-06-27 08:20 UTC · model grok-4.3
The pith
Replacing time derivatives with integrals makes QENDy robust to noise in nonlinear system identification.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that an integral formulation of the quadratic embedding method for nonlinear dynamics (QENDy) identifies the system dynamics correctly using only trajectory data without time derivatives, resulting in a more robust learning algorithm for nonlinear systems.
What carries the argument
The integral formulation of QENDy that replaces time derivatives with integrated quantities to learn the dynamics.
If this is right
- Nonlinear systems can be identified from noisy trajectory data without explicit differentiation.
- The learned model remains accurate when measurements contain noise.
- The method extends the applicability of QENDy to real experimental data where derivatives are unreliable.
Where Pith is reading between the lines
- Similar integral reformulations could improve other derivative-dependent identification techniques in dynamical systems.
- Numerical tests on benchmark systems with added noise would validate the robustness gain.
- The approach might connect to other integral equation methods used in system identification.
Load-bearing premise
That the integral formulation preserves the correctness of the original QENDy identification while removing its noise sensitivity.
What would settle it
A comparison of the original and integral QENDy on the same noisy dataset to see if the integral version recovers the true dynamics more accurately.
Figures
read the original abstract
This manuscript proposes an integral formulation of the newly defined quadratic embedding method for identifying nonlinear systems (QENDy). In the original algorithm, trajectory data points along with their time derivatives are used. Methods for calculating time derivatives make the algorithm sensitive to noise. Our integral formulation does not use the time derivatives. This results in a more robust method to learn the dynamics.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes an integral formulation of the quadratic embedding method (QENDy) for nonlinear system identification. Unlike the original derivative-based version, the new approach avoids explicit time derivatives from trajectory data, with the stated goal of improving robustness to noise while still learning the underlying dynamics.
Significance. If the integral reformulation were shown to be mathematically equivalent to the original QENDy (preserving the identified vector field) and to deliver measurable noise robustness, the result would be of practical value for system identification tasks. No such equivalence, derivation, or validation is supplied, so significance cannot be assessed.
major comments (1)
- [Abstract] The central claim—that the integral formulation identifies the same dynamics as derivative-based QENDy while removing noise sensitivity—requires a derivation showing that the quadratic embedding is rewritten via integration without altering the parameter estimation problem or introducing new biases (e.g., quadrature or boundary terms). No equations, reformulation steps, or linear system for coefficients are provided anywhere in the manuscript, leaving the claim unsupported.
Simulated Author's Rebuttal
We thank the referee for the detailed report. The primary concern is the lack of an explicit derivation for the integral formulation. We address this below and will revise the manuscript to include the requested steps.
read point-by-point responses
-
Referee: [Abstract] The central claim—that the integral formulation identifies the same dynamics as derivative-based QENDy while removing noise sensitivity—requires a derivation showing that the quadratic embedding is rewritten via integration without altering the parameter estimation problem or introducing new biases (e.g., quadrature or boundary terms). No equations, reformulation steps, or linear system for coefficients are provided anywhere in the manuscript, leaving the claim unsupported.
Authors: We agree that the current manuscript does not contain an explicit derivation of the integral reformulation, the equivalence to the original QENDy parameter estimation problem, or the resulting linear system. This is a substantive omission. In the revised version we will insert a new section that starts from the original quadratic embedding, integrates both sides over time, applies quadrature to obtain the discrete linear system for the coefficients, and discusses the effect of boundary terms and quadrature error on the identified vector field. We will also add a short proof of equivalence in the noise-free case. revision: yes
Circularity Check
No circularity: abstract states reformulation but supplies no derivation chain or equations to inspect
full rationale
The provided abstract claims an integral formulation avoids time derivatives for robustness but contains no equations, no parameter-fitting steps, and no self-citations. Without a visible derivation chain, no self-definitional, fitted-input, or self-citation reductions can be exhibited. The central claim of equivalence to original QENDy is asserted but not derived in the given text, so no load-bearing step reduces to its own inputs by construction. This is the normal case of an under-specified abstract; full manuscript equations would be required to apply the circularity test.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
-
[1]
Discovering governing equations from data by sparse identification of nonlinear dynamical systems,
S. L. Brunton, J. L. Proctor, and J. N. Kutz, “Discovering governing equations from data by sparse identification of nonlinear dynamical systems,”Proceedings of the National Academy of Sciences, vol. 113, no. 15, pp. 3932–3937, 2016
2016
-
[2]
Data-driven system identification using quadratic embeddings of nonlinear dynamics,
S. Klus and J. P. N. N’konzi, “Data-driven system identification using quadratic embeddings of nonlinear dynamics,”Physica D: Nonlinear Phenomena, p. 134839, 2025
2025
-
[3]
Universal formats for nonlinear ordinary differential systems,
E. H. Kerner, “Universal formats for nonlinear ordinary differential systems,”Journal of Mathematical Physics, vol. 22, no. 7, pp. 1366– 1371, 1981
1981
-
[4]
Qlmor: A projection-based nonlinear model order reduction approach using quadratic-linear representation of nonlinear systems,
C. Gu, “Qlmor: A projection-based nonlinear model order reduction approach using quadratic-linear representation of nonlinear systems,” IEEE Transactions on Computer-Aided Design of Integrated Circuits and Systems, vol. 30, no. 9, pp. 1307–1320, 2011
2011
-
[5]
The multiverse of dynamic mode decomposition algorithms,
M. J. Colbrook, “The multiverse of dynamic mode decomposition algorithms,”arXiv preprint arXiv:2312.00137, 2023
arXiv 2023
-
[6]
Weak SINDy for partial differen- tial equations,
D. A. Messenger and D. M. Bortz, “Weak SINDy for partial differen- tial equations,”Journal of Computational Physics, vol. 443, p. 110525, 2021
2021
-
[7]
The occupation kernel method for nonlinear system identification,
J. A. Rosenfeld, B. P. Russo, R. Kamalapurkar, and T. T. Johnson, “The occupation kernel method for nonlinear system identification,” SIAM Journal on Control and Optimization, vol. 62, no. 3, pp. 1643– 1668, 2024
2024
-
[8]
The kernel perspective on dynamic mode decomposition,
E. Gonzalez, M. Abudia, M. Jury, R. Kamalapurkar, and J. A. Rosenfeld, “The kernel perspective on dynamic mode decomposition,” arXiv preprint arXiv:2106.00106, 2021
arXiv 2021
-
[9]
Modern Koop- man theory for dynamical systems,
S. L. Brunton, M. Budisic, E. Kaiser, and J. N. Kutz, “Modern Koop- man theory for dynamical systems,”arXiv preprint arXiv:2102.12086, 2021
arXiv 2021
-
[10]
Dynamical systems and complex networks: A Koopman operator perspective,
S. Klus and N. D. Conrad, “Dynamical systems and complex networks: A Koopman operator perspective,”Journal of Physics: Complex, 2024
2024
-
[11]
Dynamic mode decomposition of numerical and exper- imental data,
P. J. Schmid, “Dynamic mode decomposition of numerical and exper- imental data,”Journal of Fluid Mechanics, vol. 656, pp. 5–28, 2010
2010
-
[12]
Solutions of ill-posed problems (a. n. tikhonov and v. y. arsenin),
R. A. Willoughby, “Solutions of ill-posed problems (a. n. tikhonov and v. y. arsenin),”SIAM Review, vol. 21, no. 2, pp. 266–267, 1979. [Online]. Available: https://doi.org/10.1137/1021044
-
[13]
System identification: Theory for the user, 2nd edition (ljung, l.; 1999) [on the shelf],
C. Simpkins, “System identification: Theory for the user, 2nd edition (ljung, l.; 1999) [on the shelf],”Robotics & Automation Magazine, IEEE, vol. 19, pp. 95–96, 06 2012
1999
-
[14]
Generalized quadratic embeddings for nonlinear dynamics using deep learning,
P. Goyal and P. Benner, “Generalized quadratic embeddings for nonlinear dynamics using deep learning,”Physica D: Nonlinear Phenomena, vol. 463, p. 134158, 2024. [Online]. Available: https://www.sciencedirect.com/science/article/pii/S016727892400109X
2024
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.