The ability of human observers to discriminate differences in the amplitude of sinusoids and narrow-band noises was measured by the rating method of detection theory. Although each sinusoid (always 1000 Hz) was presented at a fixed amplitude, its amplitude on any trial was drawn from one of two Rayleigh probability distributions that differed in mean amplitude: a signal distribution and a noise distribution. Similarly, the amplitudes of the narrow-band noises were distributed as the Rayleigh distribution by virtue of the reciprocal relation between their bandwidth (100 Hz centered on 1000 Hz) and duration (10 msec),The obtained psychometric functions showing the area under the ROC as a function of signal-to-noise ratio were similar for both kinds of signals and were displaced, on average, about 4 dB from an ideal observer's function. The slopes of the obtained functions were similar to those of an ideal observer using 1 degree of freedomhalf the number available in Rayleigh noise.When asked to discriminate small differences in the am-. plitude of two sounds, human observers do not perform at the same level as an ideal observer that makes the best possible use of the information available in the waveforms. There is nothing remarkable in this, but the exact nature of the information not used by human observers is an open question. One possibility is that the discrepancy between ideal and human observers depends upon the waveform's bandwidth. For wide-band noise, Green (1960) and Irwin (1989) reported a discrepancy of 5-7 dB between ideal and human observers, but for an approximation to narrow-band noise, Ronken (1969) reported a discrepancy of only 0.7 dB. Ronken's (1969) results are important because he studied a special case of narrow-band noise known as Rayleigh noise. A band-limited noise waveform can be represented by a finite number of equally spaced discrete samples and, according to Shannon's sampling theorem, the number of samples required is equal to 2 WT, where W is the bandwidth of the noise in hertz and T is its duration in seconds. For Rayleigh noise, the duration is the reciprocal of the bandwidth and, therefore, 2WT = 2. This is a limiting case because every additional cycle of the noise's bandwidth requires two additional samples to represent it (Green & McGill, 1970). Furthermore, the energy in such a waveform is distributed as chi square with 2WT = 2 df. The amplitude of the waveform is dis-