SE(3) Equivariant Augmented Coupling Flows
This work addresses the need for efficient and invariant probabilistic models in computational chemistry and physics, offering a novel method for sampling Boltzmann distributions with improved speed.
The paper tackles the problem of probabilistic modeling of physical systems by proposing an SE(3) equivariant coupling flow that preserves fast sampling and density evaluation, achieving competitive performance with equivariant continuous normalizing flows and diffusion models while sampling more than an order of magnitude faster on datasets like DW4, LJ13, and QM9-positional.
Coupling normalizing flows allow for fast sampling and density evaluation, making them the tool of choice for probabilistic modeling of physical systems. However, the standard coupling architecture precludes endowing flows that operate on the Cartesian coordinates of atoms with the SE(3) and permutation invariances of physical systems. This work proposes a coupling flow that preserves SE(3) and permutation equivariance by performing coordinate splits along additional augmented dimensions. At each layer, the flow maps atoms' positions into learned SE(3) invariant bases, where we apply standard flow transformations, such as monotonic rational-quadratic splines, before returning to the original basis. Crucially, our flow preserves fast sampling and density evaluation, and may be used to produce unbiased estimates of expectations with respect to the target distribution via importance sampling. When trained on the DW4, LJ13, and QM9-positional datasets, our flow is competitive with equivariant continuous normalizing flows and diffusion models, while allowing sampling more than an order of magnitude faster. Moreover, to the best of our knowledge, we are the first to learn the full Boltzmann distribution of alanine dipeptide by only modeling the Cartesian positions of its atoms. Lastly, we demonstrate that our flow can be trained to approximately sample from the Boltzmann distribution of the DW4 and LJ13 particle systems using only their energy functions.