In recent experiments the build-up of acousto-electric flux in CdS platelets was shown to be accompanied by an emission of r. f. oscillation (1 to 4). In these experiments either the transversal geometry (1, 2) with c-axis perpendicular to the platelet normaL o r the longitudinal geometry (3, 4) with c-axis parallel to the platelet normal was used. In contrast, a calculation by Bruun (5) showed that there is a considerably enhanced electromechanical coupling for pseudo-shear waves in a 3 0 ' off-axis direction. In this note it will be shown that for pseudo-shear waves round-trip gain conditions exist, too, and an r. f. oscillation can be observed.Clevite photoconducting CdS was used a s crystal material and the sample preparation was performed as described in ( l ) , except that the platelet was cut in 30 off-axis orientation. The resistivity of the oscillator was balanced by illumination with a He-Ne laser. The r.f. current was analysed with a 1L20 Tektronix spectrum analyser and, after sampling the r. f. puls on a 561A Tektronix oscilloscope, it was displayed on an x-y recorder where either the time or the frequency could be chosen a s the x axis.
0Pulses of duration between 6 0 ps and 1 ms were applied. A s in the case of (1) and (3) a non-ohmic behaviour was observed after a certain incubation time Ti which was strongly field and resistivity dependent (Fig. 1). Though the behaviour of the incubation time is similar to that of (I), no cut-off field could be observed if the pulse was long enough. This is in agreement with the observations in (3).The acousto-electric current always showdd an approximately linear increase with the applied voltage, The spectrum of the r.f. current is shown in Fig. 2. It was taken for a 3.7 kQcm sample 50 p s after the beginning of the pulse which means