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Perceptual Coherence : Hearing and Seeing

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192 <strong>Perceptual</strong> <strong>Coherence</strong><br />

This process creates a new set of delayed traces that in turn are compared<br />

to the next signal. Over time, the relative signal strength of the delay line<br />

at the period of the signal would increase due to a high number of coincidence<br />

spikes, <strong>and</strong> the strength of the other delay lines would decrease.<br />

These sorts of models seem to capture our implicit underst<strong>and</strong>ing of<br />

how we make sense of repeating patterns. To provide an equivalent sort of<br />

visual stimulus, we could construct a r<strong>and</strong>om dot kinematogram similar to<br />

the ones shown in figure 1.1. The observer would see a streaming pattern of<br />

dots <strong>and</strong> would have to judge each time the pattern recycled. A similar twodimensional<br />

recurrent delay line model would work.<br />

Moreover, it seems that models based on the timings among the spikes<br />

can also account for the change in perceived periodicity <strong>and</strong> pitch for alternating<br />

r<strong>and</strong>om noise segments. As described above, a sequence such as<br />

ABABAB is perceived as repeating AB units. But, as the number of repeats<br />

is increased from<br />

AABBAABB to AAAAAAAABBBBBBBBAAAAAAAABBBBBBBB<br />

the perception shifts to repeating A <strong>and</strong> B units. The perceived pitch doubles<br />

<strong>and</strong> the timbre of the noise shifts back <strong>and</strong> forth from As to Bs. The sequence<br />

is not perceived as repeating AAAAAAAABBBBBBBB units,<br />

even though this 16-segment unit is a perfect repeat. We can speculate that<br />

there are limits to the ability to find periodicities at long intervals, so that<br />

perceptual strength would decrease for the repeating units based on 16<br />

noise segments. If the noise segment were 2 ms (a frequency of 500 Hz),<br />

the duration of 8 As followed by 8 Bs would be 32 ms (31 Hz), close to the<br />

lower limit for tonal perception.<br />

All of these models depend on the existence of neurons capable of detecting<br />

the coincidence of incoming excitations. In the auditory pathway,<br />

octopus cells fit the requirements for a coincidence detector (Oertel, Bal,<br />

Gardner, Smith, & Joris, 2000). The octopus cells are found in the mammalian<br />

cochlear nucleus <strong>and</strong> cross the bundle of auditory fibers. Several<br />

features of the octopus cells make them superbly suited to detecting spike<br />

coincidences. First, each octopus cell spans about one third of the frequency<br />

array of the auditory fibers <strong>and</strong> therefore can integrate the firings<br />

across a wide range of frequencies. In mice, a single octopus cell could be<br />

expected to receive inputs from auditory nerve cells that span two to three<br />

octaves. Anywhere from 60 to 240 fibers would converge on a single cell,<br />

<strong>and</strong> roughly one tenth to one third of the fibers seem to be necessary to trigger<br />

the octopus cell. Second, the summation of synaptic potentials from<br />

many fibers within 1 ms is required to cause a firing. Third, octopus cells<br />

can fire rapidly with exceptionally well-timed spikes to periodic broadb<strong>and</strong><br />

sounds like clicks. Fourth, octopus cells can phase-lock at very high rates,<br />

between 800 <strong>and</strong> 1,000 spikes per second <strong>and</strong> respond to tones above

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