“…By symmetry, an analogous definition holds for θ 2,2i−1 . Here, the short radial extent of the square-well attraction, λ i = 1.1σ [37], and its surface coverage measured by the semiopening angle of its conical segment, δ i = cos −1 (0.89), are chosen to be typical of protein-protein interactions [20,23]. In contrast, the patch position on the surface and the bond energy i are randomly chosen, under the sole constraint that the lattice formed by simply bonding the patches is the orthorhombic P 2 1 2 1 2 1 .…”