Riedel Helmut, Kollmeier Birger
Medizinische Physik, Carl von Ossietzky Universität Oldenburg, D-26111 Oldenburg, Germany.
Hear Res. 2006 Aug;218(1-2):5-19. doi: 10.1016/j.heares.2006.03.018. Epub 2006 Jun 9.
Binaural difference potentials (BDs) are thought to be generated by neural units in the brain stem responding specifically to binaural stimulation. They are computed by subtracting the sum of monaural responses from the binaural response, BD = B - (L + R). BDs in dependency on the interaural time difference (ITD) have been measured and compared to the Jeffress model in a number of studies with conflicting results. The classical Jeffress model assuming binaural coincidence detector cells innervated by bilateral excitatory cells via two delay lines predicts a BD latency increase of ITD/2. A modification of the model using only a single delay line as found in birds yields a BD latency increase of ITD. The objective of this study is to measure BDs with a high signal-to-noise ratio for a large range of ITDs and to compare the data with the predictions of some models in the literature including that of Jeffress. Chirp evoked BDs were recorded for 17 ITDs in the range from 0 to 2 ms at a level of 40 dB nHL for four channels (A1, A2, PO9, PO10) from 11 normal hearing subjects. For each binaural condition 10,000 epochs were collected while 40,000 epochs were recorded for each of the two monaural conditions. Significant BD components are observed for ITDs up to 2 ms. The peak-to-peak amplitude of the first components of the BD, DP1-DN1, is monotonically decreasing with ITD. This is in contrast with click studies which reported a constant BD-amplitude for ITDs up to 1 ms. The latency of the BD-component DN1 is monotonically, but nonlinearly increasing with ITD. In the current study, DN1 latency is found to increase faster than ITD/2 but slower than ITD incompatible with either variant of the Jeffress model. To describe BD waveforms, the computational model proposed by Ungan et al. [Hearing Research 106, 66-82, 1997] using ipsilateral excitatory and contralateral inhibitory inputs to the binaural cells was implemented with only four parameters and successfully fitted to the BD data. Despite its simplicity the model predicts features which can be physiologically tested: the inhibitory input must arrive slightly before the excitatory input, and the duration of the inhibition must be considerably longer than the standard deviations of excitatory and inhibitory arrival times to the binaural cells. With these characteristics, the model can accurately describe BD amplitude and latency as a function of the ITD.
双耳差异电位(BDs)被认为是由脑干中的神经单元产生的,这些神经单元对双耳刺激有特异性反应。它们通过从双耳反应中减去单耳反应的总和来计算,即BD = B - (L + R)。在许多研究中,已经测量了依赖双耳时间差(ITD)的BDs,并与杰弗里斯模型进行了比较,但结果相互矛盾。经典的杰弗里斯模型假设双耳重合检测细胞由双侧兴奋性细胞通过两条延迟线支配,预测BD潜伏期增加ITD/2。在鸟类中发现的仅使用一条延迟线的模型修改版本,预测BD潜伏期增加ITD。本研究的目的是在大范围的ITD下测量具有高信噪比的BDs,并将数据与文献中包括杰弗里斯模型在内的一些模型的预测进行比较。在11名听力正常的受试者的四个通道(A1、A2、PO9,、PO10)上,以40 dB nHL的水平记录了17个在0到2 ms范围内的ITD的啁啾诱发BDs。对于每个双耳条件,收集了10000个epoch,而对于两个单耳条件中的每一个,则记录了40000个epoch。观察到ITD高达2 ms时存在显著的BD成分。BD的第一个成分DP1 - DN1的峰峰值幅度随ITD单调递减。这与点击研究相反,点击研究报告了ITD高达1 ms时BD幅度恒定。BD成分DN1的潜伏期随ITD单调但非线性增加。在当前研究中,发现DN1潜伏期的增加速度比ITD/2快,但比ITD慢,这与杰弗里斯模型的任何一个变体都不相符。为了描述BD波形,实施了Ungan等人[《听觉研究》106, 66 - 82, 1997]提出的计算模型,该模型使用对双耳细胞同侧兴奋性和对侧抑制性输入,仅用四个参数并成功拟合了BD数据。尽管该模型很简单,但它预测了可以进行生理测试的特征:抑制性输入必须比兴奋性输入稍早到达,并且抑制的持续时间必须比兴奋性和抑制性到达双耳细胞的时间标准差长得多。具有这些特征,该模型可以准确地将BD幅度和潜伏期描述为ITD的函数。