Non perturbative analogues of the Gaussian effective potential (GEP) a
re defined for quantum oscillators obeying q-or (qp)-deformed commutat
ion relations. These are called the non perturbative q-effective poten
tial (NP(q)EP) and the non perturbative qp effective potential (NP(qp)
EP), in the respective cases. A system-specific effective potential (S
SEP) is also introduced by means of an additional minimization with re
spect to the q or q and p parameters. The method is applied to q and (
qp) oscillators of the quartic and sextic types. The SSEP in the case
of ground states of the q-oscillators corresponds to q = 1, which is t
he ordinary bosonic limit. A potential shape transition that involves
the conversion of a double well to a single well or vice versa, is see
n to exist in the case of quantum oscillators sitting in a double well
potential.