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Oscillations, Waves, and Interactions - GWDG

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

Figure 4. Simultaneous masked thresholds of a 260-ms, 1100-Hz signal as a function of<br />

the fundamental frequency f0 of the harmonic complex masker. Thresholds are expressed<br />

relative to the level of a single masker component. The maskers were presented at a level of<br />

75 dB SPL. Squares: zero-phase complex; right-pointing triangles: negative Schroeder-phase<br />

complex; left-pointing triangles: positive Schroeder-phase complex. Reused with permission<br />

from Ref. [9]. Copyright 1995, Acoustical Society of America.<br />

results obtained at 1100 Hz would allow a direct prediction for the phase characteristic<br />

in the range of three octaves around 1100 Hz. The comparison with the results at<br />

550 Hz indeed revealed the expected relation, while towards higher frequencies, the<br />

curvature changed somewhat less with center frequency than expected for a system,<br />

in which the amplitude <strong>and</strong> phase characteristics of the filters remain constant on a<br />

logarithmic frequency scale.<br />

One final important observation from these initial Schroeder-phase studies needs<br />

to be mentioned. The view on the shape of the auditory filters was in the 1980’s<br />

strongly influenced by the work of Patterson, Moore <strong>and</strong> colleagues, who had used<br />

the notched-noise technique to estimate the amplitude characteristic of the auditory<br />

filter. The best characterization was possible with a so-called rounded exponential<br />

filter shape [17]. A time-domain implementation of a filter with such an amplitude<br />

characteric was possible based on so-called gamma-tone filters [18,19]. Due to the<br />

large amount of studies supporting this concept of auditory filters, we were interested<br />

to analyze the Schroeder-phase stimuli with such a filter.<br />

Figure 5 presents, in a similar format as Figs. 1 <strong>and</strong> 3, four periods of the waveform<br />

for harmonic complexes with fundamental frequency 100 Hz. The analysis shows the<br />

output of the gamma-tone filter tuned to 1100 Hz, <strong>and</strong> the three subpanels are for the<br />

three different phase choices. It is apparant that this filter does not lead to differences<br />

in the modulation depth between the three stimuli, <strong>and</strong> based on this simulation<br />

one would expect quite similar masking behaviour of all three complex tones, in<br />

contrast to the experimental data. The major reason for the similar treatment of the<br />

two Schroeder-phase maskers by the gamma-tone filter is its antisymmetric phase

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