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OtoAcoustic Emissions (OAE’s) Phenomenon and applications in audiological diagnostics Measurement procedures TEOAE and DPOAE Physiological backgound, functional models Acknowledgment: several illustrations and diagrams are taken from a tutorial presentation of Prof. Sebastian Hoth, Heidelberg Otoacoustic emissions (Dillier: lecture Medical Acoustics) Differentiation and quantification of hearing disorders Otoacoustic emissions (Dillier: lecture Medical Acoustics) Advantages of OAE measurement in audiology Objective response Response specific for cochlea Sensitive test Short test procedure Only passive cooperation required Otoacoustic emissions (Dillier: lecture Medical Acoustics) Clinical applications Detection of hearing disorder (newborn screening, babies, children, adults with suspected aggravation, functional hearing loss) Monitoring of cochlear function (ototoxic drugs, noise, degenerative processes, intraoperative monitoring) Audiological differential diagnostics: specific for cochlear lesions Otoacoustic emissions (Dillier: lecture Medical Acoustics) Types of otoacoustic emissions Spontaneous otoacoustic emissions (SOAE) Transitory evoked otoacoustic emissions (TEOAE) Distortion product emissions (DPOAE) Stimulus frequency emissions (SFOAE) Otoacoustic emissions (Dillier: lecture Medical Acoustics) Otoacoustic emissions (OAE) Spontaneous otoacoustic emissions (SOAE) Evoked otoacoustic emissions (EOAE) Poststimulatory OAE Transitory evoked OAE (TEOAE) Perstimulatory OAE Stimulus frequency Otoacoustic otoacoustic emissions distortion products (SFOAE) (DPOAE) Otoacoustic emissions (Dillier: lecture Medical Acoustics) Otoacoustic emissions Measurement equipment for OAE recordings Otoacoustic emissions (Dillier: lecture Medical Acoustics) Th. Janssen, in Praxis der Audiometrie (Lehnhardt & Laszig, 2000) Principle of evoked otoacoustic emission measurements (EOAE) Stimulus Response Amplitude Amplitude Frequency Time TEOAE Delayed OAE DPOAE Transitory Evoked OtoAcoustic Emissions Distortion products Distortion Product OtoAcoustic Emissions Otoacoustic emissions (Dillier: lecture Medical Acoustics) TEOAE: Transitory (short stimulus, e.g. click) Evoked OtoAcoustic Emissions Otoacoustic emissions (Dillier: lecture Medical Acoustics) OAE: verification/optimization of stimulus/measurement conditions 1. Probe Cerumen Patency? Orientation Leakage Stability 2. Stimulus Level Ear canal response Remote from tympanic membrane 3. Environment Ambient noise Sound attenuation Room acoustics Ear plugs 4. Patient Respiration Movements Cables Otoacoustic emissions (Dillier: lecture Medical Acoustics) Probe related sources of error Otoacoustic emissions (Dillier: lecture Medical Acoustics) Th. Janssen, in Praxis der Audiometrie (Lehnhardt & Laszig, 2000) Improvement of signal/noise relation by 3-fold summation: Emission Noise Otoacoustic emissions (Dillier: lecture Medical Acoustics) 3-fold test signal amplitude 1,7-fold noise signal amplitude SNR improvement is only dependent on number of averages (n): SNR improvement (Gain G): G = 20 ⋅ log (c ⋅ n ) (c N ⋅ n ) A (n) AN (n) S N ( n) n = 20 ⋅ log S = 20 ⋅ log s = 20 ⋅ log = 10 ⋅ log n S N (1) AS (1) Otoacoustic AN (1) emissions (Dillier: lecture Medical cS cAcoustics) N n TEOAE: documentation of measurement and result Otoacoustic emissions (Dillier: lecture Medical Acoustics) Properties of „true“ OAE? Good measurement conditions Stimulus STABILITY A - B DIFF reproducible response REPRO > 60% SNR > 6 dB Typical response properties: • • • • • Emission amplitude between 0 and 25 dB SPL Emission duration > 6 ms Initially fast, later slower oscillations Amplitude decreases with increasing delay Amplitude decreases for higher frequencies Otoacoustic emissions (Dillier: lecture Medical Acoustics) Polarity averaging and Binomial statistics: What is the percentage of a positive amplitude at a fixed temporal interval of a random signal? Binomial distribution: Polarity average Meas. signal with n>5: Gaussian distribution Polarity average Meas. signal with and If the polarity average reaches a value of α n, the signal is probably not a random process (sig. level 1-α) Polarity average Time Otoacoustic emissions (Dillier: lecture Medical Acoustics) Output (linear) Amplitude Nonlinearity and distortion Time Original signal Linear Amplification Intensity Input (linear) Nonlinear amplification Additional frequencies Frequency Schematic diagram Otoacoustic emissions (Dillier: lecture Medical Acoustics) Effect of cubic terms in the transfer function Input u1(t) Nonlinear system u1 (t ) = c(sin ω1t + sin ω 2t ) Output u2(t) u2 (t ) = a1u1 (t ) + a2u12 (t ) + a3u13 (t ) + ... Quadratic distortions: u12 (t ) = ... cos(ω 2 − ω1 )t + sin 2ω1t + cos(ω1 + ω 2 )t + sin 2ω 2t Cubic distortions: u13 (t ) = ... sin( 2ω 2 − ω1 )t + sin( 2ω1 − ω 2 )t + terms with „Distortion product“ Otoacoustic emissions (Dillier: lecture Medical Acoustics) 3ω1 2ω1 + ω 2 2ω 2 + ω1 3ω 2 Equipment to measure distortion products (DPOAE’s) Otoacoustic emissions (Dillier: lecture Medical Acoustics) Th. Janssen, in Praxis der Audiometrie (Lehnhardt & Laszig, 2000) Stimulation using two sinewaves: Superposition of the primary travelling waves and origin of distortion products stimulus f1 L1 = 70 dB SPL stimulus f2 = 1.2 * f1 L2 = 70 dB SPL DP 2f1-f2 Base f2 Apex Otoacoustic emissions (Dillier: lecture Medical Acoustics) Stimulation using two sinewaves: Superposition of travelling waves f1 f2 Base Apex f2 f1 Base Apex Overlap: maximum very close to f2 Otoacoustic emissions (Dillier: lecture Medical Acoustics) Spectrum of DPOAEsignal Th. Janssen, in Praxis der Audiometrie (Lehnhardt & Laszig, 2000) Otoacoustic emissions (Dillier: lecture Medical Acoustics) Audiological interpretation of OAE: OAE‘s are results of the active cochlear amplification The more effective this amplification is... 1. ... the more sensitive the hearing 2. ... the larger the emissions The OAE amplitude is inversely proportional to the hearing threshold Otoacoustic emissions (Dillier: lecture Medical Acoustics) TEOAE or DPOAE? Advantages of TEOAE Advantages of DPOAE Smaller probe Less measurement noise Up to 30 dB hearing loss Up to 50 dB hearing loss Technical artefacts relatively ease to avoid Automatic interpretation Suitable for screening Systematic inner ear diagnostics If possible both TEOAE and DPOAE! Otoacoustic emissions (Dillier: lecture Medical Acoustics) TEOAE-Measurement at day 2 or 3 „pass“ „refer“ repeat „refer“ ABR etc. „pass“ HI or CI Ok Otoacoustic emissions (Dillier: lecture Medical Acoustics) DPOAE Screening device (BioLogic) Otoacoustic emissions (Dillier: lecture Medical Acoustics) OAE-Echoscreen (Mack GmbH) Otoacoustic emissions (Dillier: lecture Medical Acoustics) OAE Screener Echocheck/Echosensor (Otodynamics Ltd) Otoacoustic emissions (Dillier: lecture Medical Acoustics) GSI 60 DPOAE (Grason Stadler) Otoacoustic emissions (Dillier: lecture Medical Acoustics) What does an alerting screening result mean? development) Hearing loss prevalence (language development)......: 3 : 1000 Sensitivity Sensitivity.......................................................... : 100 % Specifity Specifity............................................................. : 92 % What is the probability that a child with positive screening result at the first OAE test session has indeed a hearing loss? Only in 3 out of 1000 children is a hearing disorder to be expected Out of 1000 tested normal hearing children 80 will show an alerting screening result 3 / 83 = 0,0361 Positive predictive value....................................... value : 3,61 % According to T. Steffens, Regensburg Otoacoustic emissions (Dillier: lecture Medical Acoustics) Nonlinear cochlear mechanics: Sensitivity and frequency selectivity at low stimulation levels Otoacoustic emissions (Dillier: lecture Medical Acoustics) Johnstone BM, Patuzzi R, Yates GK (1986) Basilar membrane measurements and the travelling wave. Hear Res 22: 147-153 Structure and function of outer hair cells Tectorial membrane Fast motility: transversal force on the hair bundle. Active amplification? K+ Cuticular plate Slow motility: longitudinal force under efferent control. Adaptation at high levels? Electrical tuning Deiters cells efferent afferent Otoacoustic emissions (Dillier: lecture Medical Acoustics) After Kim 1986 Cochlear Micromechanics Amplification and sharpening of basilar membrane vibrations through • nonlinearity • electromotility of outer hair cells amplification feedback Preyer 1996 nonlinearity Otoacoustic emissions (Dillier: lecture Medical Acoustics) Cochlear sound processing and generation of OAE Threshold 0 dB Threshold ~ 50 dB Otoacoustic emissions (Dillier: lecture Medical Acoustics) Active filter mechanisms