~~NOTOC~~ ====== Pair Potentials ====== ---- The most simple interaction that can be used are pair potentials. They are assumed to be isotropic, i.e. they only depend on the pair distance $r_{ij}=|\boldsymbol{r}_j-\boldsymbol{r}_i|$ of the two atoms $i$ and $j$. The potential energy for a system described by pair interactions is given as $$ E_\text{total} = \frac{1}{2} \sum_{i\neq j}V_2(\boldsymbol{r}_i,\boldsymbol{r}_j) = \sum_{i #F 0 3 #C Mg Zn #I 0 0 0 #E cp_Mg -1 -10 0 cp_Zn -1 -10 0 There has to be one line per element, starting with ''cp_'', the rest of the name will be replaced by the element name (if the ''#C'' line is available) or the element number. The following three values are the starting value, the minimum and maximum for that parameter. **This feature is only available for analytic pair potentials.** ===== Number of potential functions ===== To describe a system with $N$ atom types you need $N(N+1)/2$ potentials. ^ $N$ ^ $N(N+1)/2$ ^ | 1 | 1 | | 2 | 3 | | 3 | 6 | ===== Order of potential functions ===== The potential table is assumed to be symmetric, i.e. the potential for the atom types 1-0 is the same as the potential 0-1. The order of the pair potentials in the potential file for $N$ atom types is: $\Phi_{00}, \ldots, \Phi_{0N}, \Phi_{11}, \ldots, \Phi_{1N}, \ldots, \Phi_{NN}$