This study was conducted to explore the hypothesis that the N1-P2 component of the auditory evoked potential reflects exclusively the stimulus intensity around 30 msec after sound onset rather than the stimulus intensity immediately after sound onset or the simple integrated value of sound energy. In Experiment 1, subjects were presented randomly with three kinds of brief noise bursts which differed in temporal locations of the plateau intensity. The amplitude of the N1-P2 component was significantly larger in the condition in which the plateau intensity appeared 30 msec after the noise onset than it was in the condition in which it appeared immediately after the onset, and it disappeared less than 30 msec after the onset. Furthermore, the results in Experiment 2 suggest that the N1-P2 component was little influenced by the fall time of noise bursts at approximately 40 msec after the onset. These results, taken together, seem to support the hypothesis stated above.It has been suggested that the auditory system acts as a temporal integrator of sound energy (Olsen & Carhart, 1966;Zwislocki, 1960Zwislocki, , 1969. Onishi and Davis (1968) reported that the amplitUde of the NI-P2 component of the auditory evoked potentials recorded from the vertex increased in proportion to the sound duration when it was shorter than 30 msec. Furthermore, several researchers found that lengthening the sound duration over about 30 msec did not cause any increase in the amplitude of the NI-P2 component (McCandless & Best, 1966;Picton, Woods, & Proulx, 1978). These results, taken together, suggest that the vertex potentials reflect the temporal integration of sound energy within about 30 msec after the stimulus onset.A close examination of Onishi and Davis' (1968) results, however, reveals that their data cannot be consistently interpreted by the view stated above. For instance, the amplitUde of the NI-P2 component of the evoked potential to a sound with a 3-msec rise time and a 30-msec plateau duration was not larger than it was to a sound with a 30-msec rise time and a 3-msec plateau duration. If sound energy is simply integrated over the 33 msec after the stimulus onset, the integrated value in the former sound would be over twice as great as that in the latter sound. Therefore, it is difficult to interpret this result in terms of simple integration of sound energy. Furthermore, the concept of ceiling effect cannot explain the result satisfactorily.On the other hand, if it is hypothesized that the stimulus intensity around 30 msec after stimulus onset is more effective for evoking the NI-P2 component than is the stimulus intensity immediately after the stimulus onset, Onishi and Davis' data seem to be easily interpreted.
EXPERIMENT 1 MethodThe subjects were II paid male college students between the ages of 18 and 22 years. All subjects reported that they had no hearing difficulty.The stimuli were bursts of white noise generated by an NF, WF-711 noise generator. The noise bursts were shaped and temporally controlled by a computer and ...