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Oscillations, Waves, and Interactions - GWDG

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Specific signal types in hearing research 47<br />

Noise signals have been extensively used to study auditory masking where they<br />

often serve as masker signals. For example, in the early experiments related to critical<br />

b<strong>and</strong>width by Hawkins <strong>and</strong> Stevens [27], white Gaussian noise maskers were used<br />

to measure the dependence of masked thresholds of a tonal signal as a function of<br />

frequency. Probably the preference for using noise signals as a masker is related to its<br />

uniform energy distribution across time <strong>and</strong> frequency <strong>and</strong> the fact that it is a well<br />

defined signal. The inherently stochastic nature of noise, however, has implications<br />

for its masking behavior as was demonstrated in studies that employed reproducible<br />

noise for which the stochastic uncertainties in the noise are effectively removed. Generally,<br />

reproducible noise produces lower masked thresholds than running noise [28].<br />

3.1 Low-noise noise<br />

3.1.1 Definition<br />

In the previous section we discussed that a filtering operation on white Gaussian<br />

noise causes the autocorrelation function to change from a delta function at lag zero,<br />

to a pattern that reflects predictability of successive time samples of such noise. This<br />

predictability is reflected in a smooth development of the envelope of the time domain<br />

noise waveform 1 . The rate of fluctuation in the temporal envelope is proportional to<br />

the b<strong>and</strong>width of the filtered noise signal. The spectrum of the envelope has a large<br />

DC component <strong>and</strong> a downward tilting slope that leaves very little spectral power<br />

beyond frequencies equal to the b<strong>and</strong>width of the b<strong>and</strong>pass noise. Interestingly, the<br />

degree of fluctuation is independent of the b<strong>and</strong>width, which is reflected in the probability<br />

density function of the temporal envelope values which is Rayleigh distributed.<br />

Thus, there is an inherently high degree of fluctuation in Gaussian noise.<br />

The inherent fluctuations that are present in Gaussian noise have prompted the<br />

development of so-called low-noise noise [29]. This special type of noise has the same<br />

spectral envelope as Gaussian noise, but a much lower degree of inherent fluctuations<br />

in its temporal envelope, hence the name low-noise noise. This allowed the study of<br />

the contribution of envelope fluctuations to auditory masking phenomena by comparing<br />

the masking effect of Gaussian <strong>and</strong> low-noise noise. The first to pursue this<br />

idea where Pumplin <strong>and</strong> Hartmann [30].<br />

3.1.2 Stimulus generation<br />

The original manner to generate low-noise, such as promoted by Ref. [29] was via a<br />

special optimization algorithm. First a b<strong>and</strong>-pass noise was digitally generated in<br />

the frequency domain by setting amplitudes in a restricted spectral range to some<br />

specific values, e. g., one constant value, <strong>and</strong> r<strong>and</strong>omizing the phases. Such a noise<br />

will approximate all the properties of a b<strong>and</strong>pass Gaussian noise when the product of<br />

time <strong>and</strong> frequency is sufficiently large. Via a steepest descent algorithm, the phase<br />

spectrum was modified step-by-step in the direction which made the temporal enve-<br />

1 There are alternative manners to determine the envelope of a signal which lead to<br />

somewhat different envelopes. We will consider here the Hilbert envelope.

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