27.12.2012 Views

Oscillations, Waves, and Interactions - GWDG

Oscillations, Waves, and Interactions - GWDG

Oscillations, Waves, and Interactions - GWDG

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Specific signal types in hearing research 55<br />

frequency with a sinusoid of higher frequency. This operation is an example of<br />

modulation with suppressed carrier. The resulting signal is a b<strong>and</strong>pass noise with<br />

a center frequency equal to the frequency of the sinusoid. The b<strong>and</strong>width is given<br />

by twice the cut-off frequency of the lowpass noise. By tuning the frequency of the<br />

sinusoid, the center frequency of the multiplied noise is easily tunable, <strong>and</strong> such an<br />

operation does not require the use of digital computers.<br />

3.2.2 Acoustic properties <strong>and</strong> perceptual insights<br />

Multiplied noise has regular zero crossings with a rate equal to its center frequency.<br />

Its spectrum is symmetric around its center or carrier frequency: Above the carrier<br />

frequency, the spectrum is identical to the spectrum of the original lowpass noise,<br />

while the spectrum below the carrier is a mirrored version of this spectrum. Furthermore,<br />

the envelope distribution of multiplied noise is also different from that of<br />

Gaussian noise. While the envelope of Gaussian noise has a Rayleigh distribution,<br />

the distribution of the envelope of multiplied noise correponds to the positive half of<br />

a Gaussian distribution. This latter fact follows from the process of generation: the<br />

envelope of multiplied noise corresponds to the absolute value of the original lowpass<br />

noise time function. As a consequence, the envelope distribution of multiplied noise<br />

has its highest value at zero. In contrast, for Gaussian noise, the probability of zero<br />

envelope values is zero.<br />

Due to the regular zero crossings, it is possible to add a sinusoid to multiplied noise<br />

with a fixed finestructure phase relation to the masker, if the sinusoidal frequency<br />

corresponds to the noise carrier frequency. If the sinusoid is added in phase, the<br />

resulting signal has still the same zero crossings as the noise alone, <strong>and</strong> overall, the<br />

envelope distribution is not much affected (see Fig. 11). When the sinusoidal signal<br />

Figure 11. The envelope probability distribution is shown for a multiplied noise masker<br />

alone (solid line) <strong>and</strong> for a multiplied noise masker plus signal added in phase (long-dashed<br />

line), <strong>and</strong> with a fine-structure phase difference of π/2 (short-dashed line). The signal-tomasker<br />

ratio is 25 dB. Reused with permission from Ref. [40]. Copyright 1998, Acoustical<br />

Society of America.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!