where 𝑠 is the CV, 𝜔 ! is the height of each Gaussian, 𝜏 ! is the size of the time interval between successive Gaussian depositions and 𝛿𝑠 is the Gaussian width. These repulsive Gaussians are centered at the explored points in the CV-space with a deposition rate 𝜔 = 𝜔 ! 𝜏 ! ⁄ . The biasing energy terms are repeatedly added to the potential to discourage the system from visiting again the already explored configurations, thus ensuring a homogeneous sampling of the CV-space.