In this review we discuss quantum phase transitions and the mapping between
symmetry breaking of electronic structure configurations at the large-dime
nsion limit and mean-held theory of phase transitions. We show that the fin
ite size scaling method can be used for the calculations of the critical pa
rameters of the few-body Schrodinger equation. In this approach, the finite
size corresponds to the number of elements in a complete basis set used to
expand the exact eigenfunction of a given Hamiltonian. The critical parame
ters such as the critical nuclear charges will be used to explain and predi
ct the stability of atomic and molecular negative ions. For N-electron atom
s with 2 less than or equal to N less than or equal to 86, results show tha
t, at most, only one electron can be added to a free atom in the gas phase.
However, doubly charged atomic negative ions might exist in a strong magne
tic held.