# Pauli's exclusion principle

## Pauli's exclusion principle[edit | edit source]

We've already mentioned the Pauli's exclusion principle:*each individual state can be occupied by a single fermion*. We have seen that it holds for two fermions.The introduction of Slater determinant allows us to see that this principle is valid for an arbitrary number of identical fermions: since the antisymmetric ket is a slater determinant, if two states are the same then the matrix has two identical columns and the determinant is 0.
This is not true for bosons since every has been changed into a .

## Occupation numbers[edit | edit source]

If we have a system of identical particles, with each particle allowed to stay in one of the individual states, we can define the *occupation number* as the number of particles being in the state . Occupation numbers are subjected to the restriction that . Clearly two mathematical state

- If the particle under study are bosons occupation numbers are arbitrary
- If the particle under study are fermions occupation numbers can only be 1 or 0, since a state can be empty or occupied by a single fermion

## Statistical implications of Pauli's exclusion principle[edit | edit source]

Since statistical description of macroscopic properties is based on the number of microscopic states that corresponds to the same macroscopic state, the difference between bosons and fermions, the second being subjected to Pauli's exclusion principle, leads to different statistics:

- bosons are described by Bose-Einstein statistics,which takes into account the possibility of having an arbitrary number of particles in each individual state
- fermions are described by Fermi-Dirac statistics,which takes into account the restriction in the occupation numbers