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本文引用的文献

1
Stimulus Frequency Otoacoustic Emission Delays and Generating Mechanisms in Guinea Pigs, Chinchillas, and Simulations.豚鼠、毛丝鼠的刺激频率耳声发射延迟及产生机制与模拟研究
J Assoc Res Otolaryngol. 2015 Dec;16(6):679-94. doi: 10.1007/s10162-015-0543-7. Epub 2015 Sep 15.
2
On the spatial distribution of the reflection sources of different latency components of otoacoustic emissions.关于耳声发射不同潜伏期成分反射源的空间分布。
J Acoust Soc Am. 2015 Feb;137(2):768-76. doi: 10.1121/1.4906583.
3
Generation place of the long- and short-latency components of transient-evoked otoacoustic emissions in a nonlinear cochlear model.在非线性耳蜗模型中,瞬态诱发耳声发射的长潜伏期和短潜伏期成分的产生部位。
J Acoust Soc Am. 2013 Jun;133(6):4098-108. doi: 10.1121/1.4802940.
4
Input/output functions of different-latency components of transient-evoked and stimulus-frequency otoacoustic emissions.瞬态诱发耳声发射和刺激频率耳声发射不同潜伏期成分的输入/输出功能。
J Acoust Soc Am. 2013 Apr;133(4):2240-53. doi: 10.1121/1.4794382.
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Time-frequency domain filtering of evoked otoacoustic emissions.诱发性耳声发射的时频域滤波。
J Acoust Soc Am. 2012 Oct;132(4):2455-67. doi: 10.1121/1.4751537.
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Measuring distortion product otoacoustic emissions using continuously sweeping primaries.使用连续扫频的原始信号测量畸变产物耳声发射。
J Acoust Soc Am. 2008 Sep;124(3):1613-26. doi: 10.1121/1.2949505.
7
Comparing stimulus-frequency otoacoustic emissions measured by compression, suppression, and spectral smoothing.比较通过压缩、抑制和频谱平滑测量的刺激频率耳声发射。
J Acoust Soc Am. 2007 Dec;122(6):3562-75. doi: 10.1121/1.2793604.
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Modeling otoacoustic emission and hearing threshold fine structures.耳声发射和听力阈值精细结构建模。
J Acoust Soc Am. 1998 Sep;104(3 Pt 1):1517-43. doi: 10.1121/1.424364.
9
Double-evoked otoacoustic emissions. II. Intermittent noise rejection, calibration and ear-canal measurements.双诱发耳声发射。II. 间歇性噪声抑制、校准及耳道测量。
J Acoust Soc Am. 1998 Jun;103(6):3499-508. doi: 10.1121/1.423058.
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Time-frequency distributions of click-evoked otoacoustic emissions.点击诱发耳声发射的时频分布。
Hear Res. 1997 Apr;106(1-2):112-22. doi: 10.1016/s0378-5955(97)00007-5.

刺激频率耳声发射反射源的定位

Localization of the Reflection Sources of Stimulus-Frequency Otoacoustic Emissions.

作者信息

Moleti A, Sisto R

机构信息

Physics Department, University of Roma Tor Vergata, Via della Ricerca Scientifica, 1, 00133, Rome, Italy.

INAIL Research, Via di Fontana Candida 1, 00044, Monteporzio Catone (RM), Italy.

出版信息

J Assoc Res Otolaryngol. 2016 Oct;17(5):393-401. doi: 10.1007/s10162-016-0580-x. Epub 2016 Aug 9.

DOI:10.1007/s10162-016-0580-x
PMID:27506533
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5023541/
Abstract

The generation of stimulus-frequency otoacoustic emission (SFOAE) residuals in humans is analyzed both theoretically and experimentally to investigate the relation between the frequency difference between the probe and the suppressor tone and the localization of the residual source. Experimental measurements of the SFOAE residual were performed using suppressors of increasing frequency to separate the otoacoustic response from the probe stimulus. From the response to the probe alone, the SFOAE response was also estimated, using spectral smoothing, and compared with the residuals obtained for different frequency suppressors. A nonlinear delayed-stiffness active cochlear model was used to compute the spatial distribution of the residual sources according to a recent model of the local reflectivity from roughness, as a function of the suppressor frequency. The simulations clarified the role of high-frequency suppressors, showing that in humans, with increasing suppressor frequency, the generation region of the residual is only slightly basally shifted with respect to the case of a near-frequency suppressor, near the basal edge of the peak of the resonant basilar membrane response. As a consequence, the hierarchy among different-delay components correspondingly changes, gradually favoring short-delay components, with increasing suppressor frequency. Good agreement between the experimental and theoretical dependence of the level of otoacoustic components of different delay on the frequency shift between probe and suppressor confirms the validity of this interpretation.

摘要

对人类中刺激频率耳声发射(SFOAE)残余信号的产生进行了理论和实验分析,以研究探测音与抑制音之间的频率差异与残余信号源定位之间的关系。使用频率不断增加的抑制音来分离探测刺激的耳声响应,从而对SFOAE残余信号进行实验测量。仅根据对探测音的响应,利用频谱平滑法估算出SFOAE响应,并与不同频率抑制音下获得的残余信号进行比较。根据最近提出的粗糙度局部反射率模型,利用非线性延迟-刚度有源耳蜗模型计算残余信号源的空间分布,该分布是抑制音频率的函数。模拟结果阐明了高频抑制音的作用,表明在人类中,随着抑制音频率的增加,残余信号的产生区域相对于近频抑制音的情况仅在基底方向上略有偏移,靠近共振基底膜响应峰值的基底边缘。因此,不同延迟成分之间的层次关系相应地发生变化,随着抑制音频率的增加,逐渐有利于短延迟成分。不同延迟的耳声成分水平对探测音与抑制音之间频率偏移的实验和理论依赖性之间的良好一致性证实了这种解释的有效性。