Starting from the bosonic commutation relations [ai,aj†]=δij, derive the commutation relations for the field operators
[ψ(x),ψ†(x′)]=δ(3)(x−x′)
and similarly for fermions (anticommutator). Use the definition ψ(x)=∑iφi(x)ai where {φi(x)} is a complete orthonormal set.