The discussion focuses on the quantum numbers used to label the eigenfunctions of the helium atom, particularly in the context of its non-perturbative structure. The base Hamiltonian yields quantum numbers that form the term symbol: L, S, J, and MJ. Due to the complexity of the three-body problem, analytical solutions are not available, but variational methods can provide accurate results. References to significant works, such as those by Drake and Yan, highlight high-precision calculations related to helium's eigenfunctions. Overall, understanding these quantum numbers is crucial for characterizing helium atom eigenfunctions effectively.