In 2009 Shytov et al. described the theory on the long-range interaction between adatoms in graphene with the 1/r asymptotic decay using the tight-binding approximation. It occurs that this interaction of a different type than the standard Friedeloscillation mediated one (for which we know that if it is mediated by the surface-state electrons, then the decay of Friedel spatial oscillations is like 1/r 2 , whereas for the bulk-state mediated interaction, decay is as 1/r 3 ). In graphene, as it is well-known, there are two sub-lattices A and B, and they considered the interaction between adatoms in two cases: (1) when both adatoms reside on the same sub-lattice (case denoted by AA) and ( ) when they reside on different sub-lattices (case denoted by AB). The interaction between them in the first case is described by the following formula