The data in Table show that, for instance, in the dissociation limit, the edge and center fragments would respectively would be measured to have 4 + (∆N = 0) = 4 and 2 + (∆N = 0) = 2 electrons with about a 90% probability, with the remaining probability split roughly evenly between the fragment gaining one electron and losing one electron. The most important observation from the data of Table is that model states in which any one fragment gains or loses more than one electron compared to the reference, or which acquires a local spin magnitude of more than 1, does not contribute to the final wave function at all at either the equilibrium geometry or at the dissociation limit. That is, the model states in which any one fragment is highly charged or has a high spin compared to the reference are all deadwood.