A data-driven choice of misfit function for FWI using reinforcement learning
This work addresses the difficulty of making optimal parameter choices in FWI for practitioners, offering an automated solution that could reduce reliance on manual intervention, though it is incremental as it builds on existing hierarchical approaches.
The paper tackles the challenge of manually tuning misfit functions in Full-Waveform Inversion (FWI) to avoid cycle-skipping and improve resolution by proposing a reinforcement learning approach using a deep-Q network to automatically determine optimal switching times between misfit functions, demonstrating improved convergence in simple examples.
In the workflow of Full-Waveform Inversion (FWI), we often tune the parameters of the inversion to help us avoid cycle skipping and obtain high resolution models. For example, typically start by using objective functions that avoid cycle skipping, like tomographic and image based or using only low frequency, and then later, we utilize the least squares misfit to admit high resolution information. We also may perform an isotropic (acoustic) inversion to first update the velocity model and then switch to multi-parameter anisotropic (elastic) inversions to fully recover the complex physics. Such hierarchical approaches are common in FWI, and they often depend on our manual intervention based on many factors, and of course, results depend on experience. However, with the large data size often involved in the inversion and the complexity of the process, making optimal choices is difficult even for an experienced practitioner. Thus, as an example, and within the framework of reinforcement learning, we utilize a deep-Q network (DQN) to learn an optimal policy to determine the proper timing to switch between different misfit functions. Specifically, we train the state-action value function (Q) to predict when to use the conventional L2-norm misfit function or the more advanced optimal-transport matching-filter (OTMF) misfit to mitigate the cycle-skipping and obtain high resolution, as well as improve convergence. We use a simple while demonstrative shifted-signal inversion examples to demonstrate the basic principles of the proposed method.