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Perceptual Coherence : Hearing and Seeing

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40 <strong>Perceptual</strong> <strong>Coherence</strong><br />

Figure 2.6. Representation of a simple on-off cell. The maximum excitation would<br />

occur if the white bar of the grating falls completely on the on-center <strong>and</strong> the black<br />

bars fall completely on the off-surrounds, as shown in (B). Simple on-off cells are<br />

phase sensitive, as illustrated in (B). The excitation would be maximum in (B1), close<br />

to baseline in (B2), maximally inhibited in (B3), <strong>and</strong> equal to baseline in (B4). If<br />

the frequency of the grating decreases as in (A) or triples as in (C), the firing would be<br />

close to baseline because the white <strong>and</strong> black bars fall in the on- <strong>and</strong> off-regions.<br />

are integrated by the bipolar <strong>and</strong> horizontal cells (the orientation of the bars<br />

does not matter because the receptive fields are circular). 2 The optimal grating<br />

frequencies will be those in which the widths of the black-<strong>and</strong>-white bars<br />

equal the widths of the center <strong>and</strong> surround. As shown figure 2.6, the maximum<br />

increase in firing shown in (B1) will occur when the width of a white<br />

bar (representing an increase in intensity) completely falls within the center<br />

on-region <strong>and</strong> the flanking black bars (representing a decrease in intensity)<br />

fall in the surround off-regions. By the same reasoning, the maximum<br />

2. Typically, spatial gratings are described in terms of frequency: the number of black<strong>and</strong>-white<br />

cycles per degree of visual angle. This provides a convenient metric that is independent<br />

of the distance from the viewer. For a constant frequency, the black-<strong>and</strong>-white bars must<br />

increase in width as the grating moves away from the viewer.

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