In addition to breaking spin symmetry, a single LAS state omits all entanglement between fragments; fragments interact exclusively via a mean-field potential. This approximation is obviously quantitatively inaccurate, and can also be qualitatively inaccurate in certain cases. However, interaction and entanglement between fragments, as well as global Ŝ2 symmetry, can be restored by constructing a linear combination of multiple states of the LAS type, which we refer to as LASSI. The LASSI wave functions are linear combinations of the LAS states |⃗ n⟩ P :