There is no "most common use," it is a matter of context. If you're talking about electronics states of an atom, then these are energy eigenstates of the Hamiltonian describing the electrons and their interaction with the nucleus. If you are talking about the vibrations of a diatomic molecule, then they can be as simplified as the energy eigenstates of the Hamiltonian for a Morse potential, without any consideration for electrons (Born-Oppenheimer approximation).
Basically, you have a Hamiltonian ##\hat{H}## describing some quantum system, so the ##\psi_i## such that
$$
\hat{H} \psi_i = E_i \psi_i
$$
are energy eigenstates. The physics being describe basically boil down to what is in ##\hat{H}##.
If this is still not clear, you will have to give a more explicit context for your question.