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Perceptual Coherence : Hearing and Seeing

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Characteristics of Auditory <strong>and</strong> Visual Scenes 111<br />

happens on all time <strong>and</strong> frequency scales. The relationship between<br />

amplitude <strong>and</strong> frequency is invariant. 7<br />

For a r<strong>and</strong>om walk process, the amplitudes of the Fourier waves decrease<br />

at the rate of 1/f 2 so that for each doubling of frequency (an octave),<br />

the amplitude of the wave decreases fourfold. The brightness or pressure of<br />

any next point is equal to the value of the first point plus a r<strong>and</strong>om increment.<br />

Thus, there will be just slow changes in the amplitudes <strong>and</strong> there<br />

will be high correlations between the values of adjacent points. As the distance<br />

between the two points increases, the correlation gradually decreases<br />

due to summing more <strong>and</strong> more r<strong>and</strong>om increments. The autocorrelation<br />

between points separated by a constant distance will always be the same.<br />

The difference between successive values is a series of r<strong>and</strong>om values <strong>and</strong><br />

therefore creates white noise (1/f 0 ).<br />

The most interesting outcomes occur when the amplitudes decrease at<br />

the rate of 1/f. Every time frequency is doubled the amplitude is decreased<br />

by one half, so that the energy in each octave remains identical. Many<br />

physical processes follow this 1/f relationship, including nerve membrane<br />

potentials, traffic flow, sunspot activity, <strong>and</strong> flood levels of the Nile River.<br />

Schroder (1991) pointed out that 1/f functions can be conceptualized as the<br />

combination of several processes with different distances <strong>and</strong> timings <strong>and</strong><br />

that the end result is that there is a varying correlation among the fluctuating<br />

levels across the frequency range. Consider a simple simulation suggested<br />

by Voss (Gardner, 1978) based on the sum of three dice. We start by<br />

throwing all three <strong>and</strong> recording the sum. Then only one die is selected,<br />

rethrown, <strong>and</strong> the new sum recorded. On the next trial two dice are selected,<br />

both are rethrown, <strong>and</strong> the new sum recorded. On the third trial, only one<br />

die is selected, rethrown, <strong>and</strong> the sum recorded. On the fourth trial, all three<br />

dice are selected <strong>and</strong> thrown <strong>and</strong> the sum recorded. All the following trials<br />

follow the identical sequence. In this simulation, the correlation between<br />

adjacent points is not constant. The correlation between points in which<br />

one die changed will be 2/3 because two of the three dice remain the same;<br />

the correlation between adjacent points in which two dice changed will be<br />

1/3; <strong>and</strong> the correlation between adjacent points in which all three dice<br />

changed will be zero. Thus, there will be regions in time or space of correlated<br />

sums. The number of independent processes (i.e., the number of dice)<br />

will determine the size of the correlated regions. All 1/f processes can be<br />

represented by the linear sum of short-range processes that have different<br />

time scales (Wagenmakers, Farrell, & Ratcliff, 2004). For example, heart<br />

7. Power laws have been used to describe an extraordinary range of phenomena: the frequency<br />

of earthquakes of different magnitudes, the distribution of income among individuals,<br />

the energy for metabolism for animals with different body masses, <strong>and</strong> the density of animals<br />

with different body masses (Marquet, 2002).

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