Two types of operators (I, II) are constructed in terms of bosonic qua
ntum (q-)oscillator operators. These operators satisfy a relation anal
ogous to the q-commutation relation for fermionic quantum (q-)oscillat
ors. Both types of operators (I, II) can be identified with the fermio
nic harmonic oscillator in the limit q --> 1 by exploiting the presenc
e of certain arbitrary functions of the deformation parameter q. For I
they may be identified as parameters of U(1) transformations while fo
r II they correspond to parameters of GL(2,R) transformations. Appropr
iate fermionic number operators in the limit q --> 1 are also construc
ted.