Fermions need to satisfy the Pauli exclusion principle: no two can be in th
e same state. This restriction is most compactly expressed in a second quan
tization formalism by the requirement that the creation and annihilation op
erators of the electrons satisfy anti-commutation relations. The usual clas
sical limit of quantum mechanics corresponds to creation and annihilation o
perators that satisfy commutation relations, as for a harmonic oscillator.
We discuss a simple classical limit for Fermions. This limit is shown to co
rrespond to an anharmonic oscillator, with just one bound excited state. Th
e vibrational quantum number of this anharmonic oscillator, which is theref
ore limited to the range 0 to 1, is the classical analog of the quantum mec
hanical occupancy. This interpretation is also true for Bosons, except that
they correspond to a harmonic oscillator so that the occupancy is from 0 u
p. The formalism is intended to be useful for simulating the behavior of hi
ghly correlated Fermionic systems, so the extension to many electron states
is also discussed.