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Oscillations, Waves, and Interactions - GWDG

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58 A. Kohlrausch <strong>and</strong> S. van de Par<br />

types. Higher values of the threshold indicate a stronger effect of the masker on the<br />

audibility of the signal.<br />

The data for the sinusoidal masker (circles, continuous line) indicate a highly<br />

nonlinear growth of masking. When the masker level is changed by 12 dB from 66 to<br />

78 dB SPL, the threshold increases by 30.3 dB, corresponding to a slope of 2.5 dB/dB.<br />

The sinusoidal masker produces more masking than any of the other maskers. From<br />

all noise maskers, the least masking is obtained for the 20-Hz-wide multiplied noise<br />

masker (open triangles), while the strongest masking effect is seen for the 100-Hzwide<br />

Gaussian masker. These data show thus the effect of two stimulus parameters<br />

on spectral masking: The more envelope minima occur in the masker, the lower<br />

the masked threshold (compare the three open symbols in Fig. 13). And, given a<br />

specific envelope distribution, faster fluctuations in the envelope, i. e., an increased<br />

b<strong>and</strong>width, lead to higher thresholds (compare open <strong>and</strong> filled symbols of the same<br />

type in Fig. 13).<br />

Van der Heijden <strong>and</strong> Kohlrausch [45] emphasized in their conclusion the relevance<br />

of noise statistics for the interpretation of experimental data: “In summary, our data<br />

show that, particularly with high masker levels, attention should be paid to the exact<br />

nature of narrow-b<strong>and</strong> stimuli used to mask a target at a frequency above the<br />

masker frequency [...] . These differences are by no means restricted to extremely<br />

slowly fluctuating maskers. On the contrary, masker fluctuations are relevant under<br />

many common experimental conditions, such as the ‘low-frequency tail’ of the psychoacoustic<br />

tuning curves. Unfortunately, in many published papers the influence of<br />

the type of noise used as masker (particularly multiplication noise versus Gaussian<br />

noise) has generally been neglected” ([45], p. 1806).<br />

The envelope spectra of different noise types, shown in Fig. 12, suggested a critical<br />

test of the concept of modulation filter banks, which was developed in the Ph. D.<br />

thesis by Torsten Dau [36,46,47]. This concept provided a new view on modulation<br />

detection, <strong>and</strong> emphasized the role of the intrinsic envelope fluctuations of the carrier<br />

on the ability to detect sinusoidal amplitude modulations applied to this carrier.<br />

While for noise carriers, modulation detection is limited by intrinsic modulations of<br />

the carrier, for sinusoidal carriers, the limitation in detecting amplitude modulations<br />

comes from intrinsic properties of the auditory system [48]. An important element in<br />

this concept are modulation filters: a certain range of modulation frequencies falls<br />

into the same modulation filter, <strong>and</strong> modulation detection is possible if the applied<br />

modulation is sufficiently strong compared to the intrinsic modulations within the<br />

modulation filter centered on the test modulation.<br />

In such a framework, one would expect very different modulation detection thresholds<br />

for noise carriers with different envelope spectra. For example, the modulation<br />

spectrum of low-noise noise has very little energy at low modulation frequencies <strong>and</strong><br />

therefore, modulation detection should be much better at these modulation rates<br />

than, e. g., for Gaussian or also for multiplied noise. Dau et al. [41] tested this<br />

expectation by measuring modulation detection for the three noise types shown in<br />

Fig. 12.<br />

In the left panel of Fig. 14, experimentally determined modulation thresholds are<br />

shown for the three noise types, all with a b<strong>and</strong>width of 50 Hz. First of all, we see<br />

that Gaussian <strong>and</strong> multiplied noises have the highest thresholds at low modulation

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