van de Par S, Kohlrausch A
IPO Center for Research on User-System Interaction, Eindhoven, The Netherlands.
J Acoust Soc Am. 1998 Apr;103(4):2100-10. doi: 10.1121/1.421356.
Detection thresholds were measured with a multiplied-noise masker that was in phase in both ears and a sinusoidal signal which was either in phase or out of phase (NoSo and NoS pi conditions). The masker was generated by multiplying a low-pass noise with a sinusoidal carrier. The signal was a sinusoid with the same frequency as the carrier and a constant phase offset, theta, with respect to the carrier. By adjusting the phase offset, the stimulus properties were varied in such a way that only interaural time delays (theta = pi/2) or interaural intensity differences (theta = 0) were present within the NoS pi stimulus. Thresholds were measured at a center frequency of 4 kHz as a function of bandwidth for theta = pi/2 and for theta = 0. In a second experiment thresholds were measured for a bandwidth of 25 Hz as a function of the center frequency. The results show that narrow-band BMLDs at 4 kHz can amount to 30 dB for the theta = 0 condition. For this condition, narrow-band BMLDs are also reasonably constant across frequency, in contrast to results obtained with standard Gaussian-noise maskers. For theta = pi/2, BMLDs are restricted to the frequency region below 2 kHz provided that the masker is narrow band, but BMLDs of up to 15 dB are found at 4 kHz if the masker is 50 Hz or wider. The frequency dependence of the binaural thresholds seems to be best explained by assuming that the stimulus waveforms are compressed before binaural interaction.
使用双耳同相的乘法噪声掩蔽器和同相或异相的正弦信号(NoSo和NoS π条件)测量检测阈值。掩蔽器通过将低通噪声与正弦载波相乘生成。信号是与载波频率相同且相对于载波具有恒定相位偏移θ的正弦波。通过调整相位偏移,刺激特性以这样的方式变化,即NoS π刺激中仅存在双耳时间延迟(θ = π/2)或双耳强度差异(θ = 0)。在中心频率为4 kHz时,根据带宽测量θ = π/2和θ = 0时的阈值。在第二个实验中,根据中心频率测量带宽为25 Hz时的阈值。结果表明,对于θ = 0条件,4 kHz处的窄带双耳掩蔽级差(BMLD)可达30 dB。对于该条件,与使用标准高斯噪声掩蔽器获得的结果相比,窄带BMLD在频率上也相当恒定。对于θ = π/2,如果掩蔽器是窄带的,则BMLD限于2 kHz以下的频率区域,但如果掩蔽器为50 Hz或更宽,则在4 kHz处可发现高达15 dB的BMLD。双耳阈值的频率依赖性似乎最好通过假设刺激波形在双耳相互作用之前被压缩来解释。