We introduce a
τ
\tau
-dependent Wigner representation,
Wig
τ
\operatorname {Wig}_\tau
,
τ
∈
[
0
,
1
]
\tau \in [0,1]
, which permits us to define a general theory connecting time-frequency representations on one side and pseudo-differential operators on the other. The scheme includes various types of time-frequency representations, among the others the classical Wigner and Rihaczek representations and the most common classes of pseudo-differential operators. We show further that the integral over
τ
\tau
of
Wig
τ
\operatorname {Wig}_\tau
yields a new representation
Q
Q
possessing features in signal analysis which considerably improve those of the Wigner representation, especially for what concerns the so-called “ghost frequencies”. The relations of all these representations with respect to the generalized spectrogram and the Cohen class are then studied. Furthermore, a characterization of the
L
p
L^p
-boundedness of both
τ
\tau
-pseudo-differential operators and
τ
\tau
-Wigner representations are obtained.