Paper:
Initial value problems, i.e. differential equations with specific, initial conditions, represent a classic problem within the field of ordinary differential equations (ODEs). While the simplest types of ODEs may have closed-form solutions, most interesting cases typically rely on iterative schemes for numerical integration such as the family of Runge-Kutta methods. They are, however, sensitive to the strategy the step size is adapted during integration, which has to be chosen by the experimenter. Here, we show how the design of a step size controller can be cast as a learning problem, allowing deep networks to learn to exploit structure in the initial value problem at hand in an automatic way. The key ingredients for the resulting Meta-Learning Runge-Kutta (MLRK) are the development of a good performance measure and the identification of suitable input features. Traditional approaches suggest the local error estimates as input to the controller. However, by studying the characteristics of the local error function we show that including the partial derivatives of the initial value problem is favorable. Our experiments demonstrate considerable benefits over traditional approaches. In particular, MLRK is able to mitigate sudden spikes in the local error function by a faster adaptation of the step size. More importantly, the additional information in the form of partial derivatives and function values leads to a substantial improvement in performance. The source code can be found at https://www.dropbox.com/sh/ rkctdfhkosywnnx/AABKadysCR8-aHW_0kb6vCtSa?dl=0

Review:
## Summary ##
The authors present a method for learning a step-size adaptation strategy for Runge-Kutta methods. The principal contributions of the paper are:
1. They define a loss function that better captures global performance of the controller, rather than just local behavior.
2. They propose a set of input features to a step size controller. It includes the intermediate Runge-Kutta evaluation values, which allow the controller to approximate the derivatives of the Jacobian function $g$.
3. They describe a recurrent architecture for adapting step size over time.
Runge-Kutta methods are a workhorse of ordinary differential equations and choosing step size is one of the central challenges involved in their application. Better methods for step size selection would definitely be of broad interest. As the authors point out, existing methods often consist of hand-tuned heuristics---a feature that often suggests machine learning could provide significant improvements.
While the premise of the paper is very promising, I don't think it is ready to be accepted to ICLR at this time. Most significantly, the experimental results are not particularly compelling. I believe the authors should refine their method, aim for better experimental results and resubmit. I have included more specific comments below.
## Specific Comments ##
1. I think the paper would benefit from a clearer description of the RK step-size selection problem. For instance, for a p^th order RK solver, at each time step,
   * Inputs: t, y(t), g  # Also possibly intermediate values from previous time steps.
   * Select a step size h(t)
   * Evaluate g at p different points based on h(t).
   * Use these evaluations to compute a value of y_(t + h_t)
   For those that aren't familiar with these methods (at ICLR there will be many!) I think this would help explain where the authors' method (and the other methods your describe) fits into the larger algorithm.
2. I think a short explanation of error estimation would be helpful in addition to the reference to Butcher. This estimation is critical to step size adaptation. In particular I think this would be clearer if the authors expanded the paragraph at the bottom of page 4, where they describe error in a polynomial in (t_n, h) whose coefficients are derivatives of g.
3.  The authors' proposed loss function (Eq. 5) includes the true value of y at t_n, y(t_n). They acknowledge that this may make it computationally prohibitive, but I think this point warrants further discussion. Does this mean that their loss function can only be used on problems for which we have a closed form solution (such as harmonic oscillators)? I noticed that in their van der Pol experiments, the authors switch to a more standard loss (Eq. 6). Is this because Eq. 5 is intractable in this example? Is there a reasonable approximation to Eq. 5 that could be used when a closed form solution is not known?
4. There are a number of issues with the experiments that I think could use clarification or improvement:
  (a) The authors compare to a 'baseline' but I don't believe this baseline is defined anywhere. Is it one of the adaptation methods described in Section 2?
  (b) In Table 1, the baseline method achieves lower error, while MLRK uses fewer steps. It is difficult to assess if this is an improvement since this this cost-accuracy tradeoff is at the heart of the Lagrangian formulation. Ideally, shouldn't we be able to adjust 'tol' to trace out some Pareto frontier for the cost-accuracy tradeoff? In this case, wouldn't we hope for MLRK to be able to achieve better accuracy given the same computational budget?
  (c) In the van der Pol experiments, the authors switch to local L1 loss (Eq. 6). Was the intention to experiment with local L1 loss and van der Pol provided an interesting class of examples? Or was the reasoning that Eq. 5 is intractable for van der Pol so they had to use local L1 loss? If Eq. 5 can still be evaluated on these experiments, this might be a more convincing comparison.
  (d) The number of steps required was provided for the harmonic oscillator experiments, but not the van der Pol ones. This would be helpful for comparing the methods.
  (e) What is the computational overhead of running an RNN alongside your solver? Although it doesn't tell the whole story, it would be informative to report wall clock time along with the number of steps required for each method.