Remember that a notch filter must have transfer function zeros on the unit circle $z=e^{j\omega}$, i.e., there are certain frequencies that are completely attenuated. But note that zeros on the unit circle are not sufficient to characterize a filter as a notch filter (even though any frequency with perfect attenuation is called a notch frequency). E.g., most frequency-selective filters will have most, if not all, of their zeros on the unit circle (to get a good stop band attenuation). However, they are no notch filters. So for IIR filters you also have to consider the pole locations. And for notch filters, the pole angles are identical to or at least very close to the angles of the zeros. So for each zero on the unit circle you get a pole at the same or a similar angle, just with a smaller radius, because for causal and stable filters the poles need to be inside the unit circle.
That's why the filter in your example qualifies as a notch filter. All its zeros are on the unit circle and its poles are at the same angle as the zeros. The notch frequencies are simply the angles at which the zeros occur:
$$z_{01}=e^{j\omega_{01}}=e^{j\pi /4},\qquad
z_{02}=e^{j\omega_{02}}=-e^{j\pi/4}=e^{-j3\pi /4}$$
