“…From the above analysis, it could be said that the structure of the interface has reached a stationary state in this simulation time, and the structural and energetic analysis could be performed during the final 500 ps of the simulation time. Moreover, during this simulation time, the local solvent densities of the interfacial models fluctuate weakly and approach the bulk solvent density, while the water solvent molecules move away from the crystal faces, as shown in Figure S11. ,, The mean solvent densities which are along the normal to the crystal faces at its plateau of (1 0 1̅)/solvent, (1 0 1)/solvent, (0 0 2)/solvent, (0 1 1)/solvent, (0 1̅ 1)/solvent, (1 1̅ 0)/solvent, (1 1 0)/solvent models are 0.986, 0.985, 0.981, 0.987, 0.989, 0.979, and 0.980 g/cm 3 , respectively, which are close to the simulated bulk density of the water solvent bulk (0.989 g/cm 3 ). Therefore, the behaviors of the simulations are physically consistent.…”