> I believe all of these will require additional rewrite in multiple places.
We thank the reviewer for raising these concerns. We are confident that all of the concerns are addressed in the paper, which we concisely summarize in this response. The reviewer’s comments will be helpful for guiding the final revision of this paper (if accepted) to make our points even clearer.
> it is yet unclear to me how the proposed model improves the results and helps the stabilization of the training as claimed.
We summarize here the reasoning for why "the proposed model improves the results and helps the stabilization of the training", which is also provided in the paper but we will make this clearer in a revision, if the paper gets accepted:
1. **Gauss-Legendre quadrature results in a more accurate estimate of the time integral when compared to Monte Carlo.** This is because it is a higher-order numerical scheme (more precisely, it allows integrating higher-degree polynomials exactly) that leads to lower quadrature errors than Monte Carlo. Besides this theoretic argument, the difference in the quadrature error can be seen empirically in our experiments in, e.g., Figure 2. (See Section 2.3.)
2. **A more accurate estimate of the time integral results in a more stable and accurate estimate of the loss.** This is supported numerically by Figure 2 (left) which shows extremely high variability in the estimates of the loss for AM and low variance estimates of loss for our proposed HOAM. This also agrees with standard results from statistical learning theory where the deviation of the empirical risk (the estimate of the loss function) from the true risk (the true loss function) directly enters in bounds of generalization errors.
3. **A more accurate estimate of the loss makes solving the optimization problem tractable.** This is supported by the numerical results in the paper, explicitly in Figure 2 (middle) and shown to be essential in global response,
All this is also described in detail in the main text of our paper in Section 2.3 and numerically supported by Figure 2 and the global response. For example see line 200: "Plain uniform sampling over the data set for mini-batching can lead to poor estimates of the loss."
> If I understand correctly, the HOAM combines higher order numerical quadrature with MC sampling to solve (7) in the direction of time by employing a Gauss-Legendre quadrature. How can this be achieved numerically?
1. As referenced in the main text of the paper the empirical loss is given in the Appendix in section A. This is written down as a discrete summation which can be easily implemented numerically.
2. For the Gauss-Legendre quadrature, the key algorithmic step is determining the roots of the Legendre polynomials, which is implemented (for example) in scipy (scipy.special.roots_legendre()). We also provide the code of our implementation, but the link is redacted for now per submission policy.
> It would be also useful to motivate the choice of the dynamical systems in the numerical experiments? Why the examples are relevant in this context is unclear.
1. From a surrogate modeling perspective, the systems that we consider are exceedingly challenging because they are high dimensional, chaotic and/or stochastic. Surrogate modeling for such systems is in its infancy because the point-wise approximations of traditional surrogate modeling techniques are meaningless. We reference these attempts in detail in the introduction and literature review.
2. We make careful efforts to choose problem setups which are experimentally meaningful to practitioners (see for example Appendix B.2 that describes that the data are obtained from code that are used by plasma physicists). The physical relevance of our problem setups are detailed in the numerous sources we cite, see [7, 21, 34, 42, 87 Sec 2(b)(i), 58].
> A clear framing of the problem setup and all the assumptions on the model would help the reader to better understand the results.
1. The problem setup is described in the Introduction section on page 1: “Given a data set of samples [...] we aim to learn a dynamical-system reduced model to rapidly predict samples that approximately follow the same law [...]”
2. When we make mathematical statements, we provide assumptions. For example, for the statement of ‘uniqueness’ on page 4 we assume that the density is positive and that the source term integrates to zero.
3. We provide an extensive appendix C-E on the connection to optimal transport and additional literature.
We hope that we have been able to demonstrate that most of these concerns are addressed in the main text of the paper. If the reviewer does not have any additional concerns, we would greatly appreciate it if they would consider revising their score.