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Absolute auditory threshold: testing the absolute
Author(s) -
Heil Peter,
Matysiak Artur
Publication year - 2020
Publication title -
european journal of neuroscience
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.346
H-Index - 206
eISSN - 1460-9568
pISSN - 0953-816X
DOI - 10.1111/ejn.13765
Subject(s) - quiet , amplitude , sound intensity , envelope (radar) , intensity (physics) , absolute threshold of hearing , poisson distribution , acoustics , physics , mathematics , sound (geography) , computer science , statistics , hearing loss , audiology , telecommunications , medicine , radar , quantum mechanics
Abstract The mechanisms underlying the detection of sounds in quiet, one of the simplest tasks for auditory systems, are debated. Several models proposed to explain the threshold for sounds in quiet and its dependence on sound parameters include a minimum sound intensity (‘hard threshold’), below which sound has no effect on the ear. Also, many models are based on the assumption that threshold is mediated by integration of a neural response proportional to sound intensity. Here, we test these ideas. Using an adaptive forced choice procedure, we obtained thresholds of 95 normal‐hearing human ears for 18 tones (3.125 kHz carrier) in quiet, each with a different temporal amplitude envelope. Grand‐mean thresholds and standard deviations were well described by a probabilistic model according to which sensory events are generated by a Poisson point process with a low rate in the absence, and higher, time‐varying rates in the presence, of stimulation. The subject actively evaluates the process and bases the decision on the number of events observed. The sound‐driven rate of events is proportional to the temporal amplitude envelope of the bandpass‐filtered sound raised to an exponent. We find no evidence for a hard threshold: When the model is extended to include such a threshold, the fit does not improve. Furthermore, we find an exponent of 3, consistent with our previous studies and further challenging models that are based on the assumption of the integration of a neural response that, at threshold sound levels, is directly proportional to sound amplitude or intensity.