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Perceptual Coherence : Hearing and Seeing

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80 <strong>Perceptual</strong> <strong>Coherence</strong><br />

Figure 2.28. The spectral-temporal receptive fields of four representative<br />

auditory cells. Nearly all neurons had multiple excitation <strong>and</strong> inhibitory regions<br />

<strong>and</strong> seem tuned to auditory characteristics that define objects. Adapted from “Optimizing<br />

Sound Features for Cortical Neurons,” by R. C. DeCharms, D. T. Blake, <strong>and</strong><br />

M. M. Merzenich, 1998, Science, 280, 1439–1444.<br />

surface, finding stimulus edges (onsets) in time, finding stimulus movements,<br />

<strong>and</strong> finding feature conjunctions.”<br />

Shamma (2001) <strong>and</strong> Shamma <strong>and</strong> Klein (2000) measured the receptive<br />

fields in A1 using sounds made up of many harmonics across a five-octave frequency<br />

range. The amplitudes of the harmonics are modulated across the logarithmic<br />

frequency axis by a sine wave that drifts either up or down in<br />

frequency. The sine wave creates an amplitude envelope across the frequency<br />

range that gradually shifts in frequency, as shown in figure 2.29. By varying<br />

the frequency, rate of drift, <strong>and</strong> amplitude (depth of modulation) of the sine<br />

wave, it is possible to measure the spectral-temporal response field from the<br />

resulting firing pattern. Examples of rippled spectra are shown in figure 2.29. 5<br />

Researchers (Depireaux, Simon, Klein, & Shamma, 2001; Kowalski,<br />

Depireaux, & Shamma, 1996) investigated whether the spectral <strong>and</strong> temporal<br />

components of the neural response were separable <strong>and</strong> independent. In<br />

5. The ripple stimuli are modeled after drifting sinusoidal gratings, discussed in chapter 5,<br />

used to investigate second-order motion.

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