2014
DOI: 10.1186/1475-925x-13-95
|View full text |Cite
|
Sign up to set email alerts
|

An in-situ calibration method and the effects on stimulus frequency otoacoustic emissions

Abstract: BackgroundThe interference between the incoming sound wave and the acoustic energy reflected by the tympanic membrane (TM) forms a standing wave in human ear canals. The existence of standing waves causes various problems when measuring otoacoustic emissions (OAEs) that are soft sounds closely related with the functional status of the inner ear. The purpose of this study was to propose an in-situ calibration method to overcome the standing-wave problem and to improve the accuracy of OAE measurements.MethodsIn … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
10
0

Year Published

2016
2016
2024
2024

Publication Types

Select...
6
1

Relationship

1
6

Authors

Journals

citations
Cited by 10 publications
(10 citation statements)
references
References 37 publications
0
10
0
Order By: Relevance
“…Experiment 2 mainly focused on the use of chirp stimuli that could be presented without system distortion at higher relative levels than was possible with click stimuli. Including chirps with slower sweep rates traversed the qualitative divide between sweep rates used in swept-tone studies of SFOAEs (Chen et al, 2014; Kalluri & Shera, 2013) and the relatively faster sweep rates typically used with chirp OAE measurements. Experiment 2 used a smaller set of test ears than Exp.…”
Section: Methodsmentioning
confidence: 99%
“…Experiment 2 mainly focused on the use of chirp stimuli that could be presented without system distortion at higher relative levels than was possible with click stimuli. Including chirps with slower sweep rates traversed the qualitative divide between sweep rates used in swept-tone studies of SFOAEs (Chen et al, 2014; Kalluri & Shera, 2013) and the relatively faster sweep rates typically used with chirp OAE measurements. Experiment 2 used a smaller set of test ears than Exp.…”
Section: Methodsmentioning
confidence: 99%
“…seen here reflects the combined effects of ear-canal acoustics on both the evoking stimuli and on the emission itself. For instance, the SPL-calibration overcompensates the stimuli level near the quarter-wave null, resulting in stronger stimulation of the cochlea (e.g., Siegel and Hirohata, 1994;Scheperle et al, 2008;Chen et al, 2014). This may explain the increase in DPOAE levels near 2-4 kHz at the deep probe placement, where the f 1 frequency (2.6-5.2 kHz) was near f k/4 (shifted from 2.6 to 3.4 kHz; see Sec.…”
Section: Changes In Ear-canal Acoustics With Probe Insertion Depthmentioning
confidence: 99%
“…1(B) ;Siegel, 1994;Siegel and Hirohata, 1994]. These effects manifest themselves most simply when stimulus and response are at the same frequency; for example, as reduced behavioral thresholds or increased SFOAE amplitudes near f k/4 (Lewis et al, 2009;Chen et al, 2014;Souza et al, 2014). Interpretation of the effects of quarter-wave nulls on DPOAE measurements is more complicated, since DPOAE levels depend on both the absolute and the relative levels of the two evoking tones (L 1 and L 2 ), which are altered differently when either f 1 and/or f 2 approach f k/4 (Whitehead et al, 1995).…”
Section: A Effects Of Ear-canal Acoustics On Stimulus and Emissionmentioning
confidence: 99%
“…Estimating an equivalent pressure at the TM Swept-tone stimulus-frequency (SF) OAEs have been measured using a procedure with constant equivalent pressure level at the TM under the assumptions that the ear canal has a cylindrical geometry and an immobile TM (Chen et al, 2014). The latter assumption allows estimation of the ear-canal length from a "quarter-length frequency" in the measured sound pressure level.…”
Section: à18mentioning
confidence: 99%
“…In contrast to Chen et al (2014), this technique allows for the presence of TM mobility. A cylindrical model of ear-canal acoustics is used for a lossfree acoustic wave number k 0 ¼ 2pf =k for sound of frequency f and wavelength k traveling in a canal of length x, in which a time dependence e j2pft is assumed.…”
Section: à18mentioning
confidence: 99%