The wave function for an atom simultaneously depends on (describes) all of the electrons in the atom. The Schrödinger equation is much more
complicated for atoms with more than one electron than for a one-electron species such as a hydrogen atom, and an explicit solution to this equation
is not possible even for helium, let alone for more complicated atoms. We must therefore rely on approximations to solutions of the many-electron
Schrödinger equation. We shall use one of the most common and useful, called the orbital approximation. |