Gorga Michael P, Neely Stephen T, Dierking Darcia M, Kopun Judy, Jolkowski Kristin, Groenenboom Kristin, Tan Hongyang, Stiegemann Bettina
Boys Town National Research Hospital, 555 North 30th Street, Omaha, Nebraska 68131, USA.
J Acoust Soc Am. 2008 Apr;123(4):2172-90. doi: 10.1121/1.2839138.
Distortion product otoacoustic emission suppression (quantified as decrements) was measured for f(2)=500 and 4000 Hz, for a range of primary levels (L(2)), suppressor frequencies (f(3)), and suppressor levels (L(3)) in 19 normal-hearing subjects. Slopes of decrement-versus-L(3) functions were similar at both f(2) frequencies, and decreased as f(3) increased. Suppression tuning curves, constructed from decrement functions, were used to estimate (1) suppression for on- and low-frequency suppressors, (2) tip-to-tail differences, (3) Q(ERB), and (4) best frequency. Compression, estimated from the slope of functions relating suppression "threshold" to L(2) for off-frequency suppressors, was similar for 500 and 4000 Hz. Tip-to-tail differences, Q(ERB), and best frequency decreased as L(2) increased for both frequencies. However, tip-to-tail difference (an estimate of cochlear-amplifier gain) was 20 dB greater at 4000 Hz, compared to 500 Hz. Q(ERB) decreased to a greater extent with L(2) when f(2)=4000 Hz, but, on an octave scale, best frequency shifted more with level when f(2)=500 Hz. These data indicate that, at both frequencies, cochlear processing is nonlinear. Response growth and compression are similar at the two frequencies, but gain is greater at 4000 Hz and spread of excitation is greater at 500 Hz.
在19名听力正常的受试者中,测量了f(2)=500和4000 Hz时,一系列初级水平(L(2))、抑制频率(f(3))和抑制水平(L(3))下的畸变产物耳声发射抑制(以衰减量量化)。在两个f(2)频率下,衰减与L(3)函数的斜率相似,且随f(3)增加而减小。由衰减函数构建的抑制调谐曲线用于估计:(1)对同频和低频抑制器的抑制;(2)首尾差异;(3)Q(ERB);(4)最佳频率。对于500和4000 Hz,根据与失谐抑制器的抑制“阈值”相关的函数斜率估计的压缩情况相似。对于两个频率,首尾差异、Q(ERB)和最佳频率均随L(2)增加而减小。然而,与500 Hz相比,4000 Hz时的首尾差异(耳蜗放大器增益的估计值)大20 dB。当f(2)=4000 Hz时,Q(ERB)随L(2)下降的幅度更大,但在倍频程尺度上,当f(2)=500 Hz时,最佳频率随声级的变化更大。这些数据表明,在两个频率下,耳蜗处理都是非线性的。两个频率下的反应增长和压缩情况相似,但4000 Hz时的增益更大,500 Hz时的兴奋扩散更大。