🤖 AI Summary
This work addresses the challenge of simultaneously modeling Lennard-Jones (LJ) and electrostatic interactions with high accuracy while accounting for molecular rigid-body rotation in solvation free energy calculations. We propose a novel thermodynamic integration (TI) method based on a neural network potential (NNP) employing a three-body representation. Crucially, Hamiltonian interpolation is defined at the sample-distribution level, ensuring that the NNP strictly satisfies equilibrium physical constraints at every TI step. Our approach achieves, for the first time, joint continuous coupling of LJ and electrostatic terms and explicitly incorporates molecular rigid-body rotation. Integrated with molecular dynamics sampling and high-precision TI integration, the method significantly improves free energy prediction accuracy on atomic-scale benchmarks—including LJ fluids and aqueous systems (e.g., methane insertion into water). This establishes a new paradigm for efficient, high-fidelity simulation of complex solvation processes.
📝 Abstract
We present a method for computing free-energy differences using thermodynamic integration with a neural network potential that interpolates between two target Hamiltonians. The interpolation is defined at the sample distribution level, and the neural network potential is optimized to match the corresponding equilibrium potential at every intermediate time step. Once the interpolating potentials and samples are well-aligned, the free-energy difference can be estimated using (neural) thermodynamic integration. To target molecular systems, we simultaneously couple Lennard-Jones and electrostatic interactions and model the rigid-body rotation of molecules. We report accurate results for several benchmark systems: a Lennard-Jones particle in a Lennard-Jones fluid, as well as the insertion of both water and methane solutes in a water solvent at atomistic resolution using a simple three-body neural-network potential.