Spin vectors are usually represented in terms of their Hermitian cartesian component operators
Sometimes, the non-Hermitian ladder operators
are used. The cartesian operators are then given by
Some common commutators are
and
For a spin S the cartesian and ladder operators are square matrices of
dimension 2S+1. They are always represented in the Zeeman basis with
states
(m=-S,...,S), in short
,
that satisfy
For S=1/2
The state is commonly denoted as
,
the
state as
.
For S=1
For S=3/2
For S=2
For S=5/2