http://auditorymodels.org/jba
Dr. Jonathan (Jont) B. Allen received a BS in Electrical Engineering from the University of Illinois, Urbana-Champaign in 1966, and MS and PhD from the University of Pennsylvania in 1968 and 1970 respectively. After graduation in 1970 Allen joined Bell Laboratories in Murray Hill NJ, where he was in the Acoustics Research Department (from 1974 to 1997), as a Distinguished member of Technical Staff. Since 1997 he is with the research division of the newly created AT&T Labs. |
|
|
|
|
|
|
|
Title: 'Derecruitment by Multiband compression in hearing aids'
An MPEG version of this talk may be found in:
The Efferent Auditory System ; Ed. C. Berlin,
Chapt. 4., pp 73--86, Singular, 1999,
401 West A St., Suite 325, San Diego, CA 92101
Click here to watch the cochlear model video
This material is discussed in:
Harvey Fletcher's role in the creation of communication acoustics
J. Acoust. Soc. Am., 1996, April, Vol. 99, pp 1825--1839.
This 28 minute video proceeds as follows:
This paper shows that the slope in the basal tail for long-wave cochlear models is 3 dB/mm, whereas neural data have a slope of 0.2 dB/mm. This very shallow slope is consistent with two-tone suppression and upward-spread of masking thresholds, which are independent of masker frequency (Fahey and Allen, JASA 1985, pp 599-612).
This paper discusses the relation between loudness and the intensity JND. We have shown that intensity discrimination may be viewed as the second moment of the loudness decision variable, and that this decision variable is Poisson. These results are consistent with the JND being due to internal (neural) noise.
This paper was present orally at the ARO meeting in Feb. 1997. It discusses why the outer hair cells (OHC) are need by the auditory system to compress the dynamic range of the acoustic signal due to the limited dynamic range of the inner hair cell (IHC). According to this theory, the OHCs tension the basilar membrane, thereby changing its stiffness as a function of signal intensity (Page 9). When the stiffness changes, the basilar membrane cutoff frequency changes accordingly. The gain seen by the IHC is dynamically controlled by sliding the low-pass filter of the cochlear traveling wave across the high pass filtering of the tectorial membrane, which varies the gain at the cross-over frequency. This idea can be used to explain the upward-spread of masking (Page 8).
load FILTERH.MAT loglog(abs(Hw)) zoomThen use the mouse to select the viewable portion from the screen, to scale the frequency range of interest. If you wish to plot the data as a function of place along the basilar membrane, use the command:
semilogy(abs(Hw)')and again use zoom to display the region of interest.