∆N S 0 0 0.00 0.00 0.00 0.00 0.00 0.00 -1 The deadwood model states with |∆N | > 1 or S > 1 for at least one fragment correspond to 3744 of the LASSI [3,3] model states of this molecule. However, the remaining 900 model states still include more than 600 deadwood states, based on the LASSI eigenvectors at both equilibrium and dissociation. These model states are distinguished by the fragment statelet index, n. Table presents n(I) K (∆N, S) [see Eq. ( ) above], the expectation value of this index after projecting into a given fragment Hilbert space for each fragment. For example, at the dissociation limit, when the left fragment has acquired one electron (∆N = 1), the state of that fragment might consist of, on average, 26% the second root (n = 1) of Eq. ( ), or 13% the third root (n = 2), or some other linear combination of the first (n = 0), second, and third roots that yields the same average n of 0.26. In general, a value of x for this expectation value indicates that at least one statelet with index n ≥ ⌈x⌉ must contribute significantly to the final wave function.