Alternatively, contractions can be denoted by a line joining and .
We shall look in detail at four special cases where and are equal to creation and annihilation operators. For particles we'll denote the creation operators by and the annihilation operators by ().
They satisfy the usual commutation relations , where denotes the Kronecker delta.
We then have
where .
These relationships hold true for bosonic operators or fermionic operators because of the way normal ordering is defined.