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组合音与掩蔽

Combination tones and unmasking.

作者信息

Tyler R S

出版信息

Hear Res. 1980 Jun;2(3-4):357-68. doi: 10.1016/0378-5955(80)90070-2.

Abstract

Some important relationships between two auditory nonlinearities, unmasking and combination tone (CT) production, are described. An example of unmasking is provided by using a forward-masking paradigm where a baseline is first obtained by determining the threshold of a 2000 Hz signal preceded by a 2000 Hz masker. When a second tone (the suppressor) is then added concurrently with the masker, the signal can be easier to hear. At a suppressor level of 80 dB SPL, this unmasking occurs for suppressor frequencies around 2300 Hz. At a suppressor level of 55 dB SPL, the unmasking effect occurs at suppressor frequencies closer to the masker frequency. An example of CT production is provided by presenting two sinusoids (f1 and f2) as maskers in a forward-masking experiment. The threshold of the 2000 Hz signal is shown to decrease as f2/f1 is increased keeping 2f1 - f2 = 2000 Hz. This is consistent with the notion that the magnitude of the CR decreases as f2/f1 increases. We then provide evidence that CTs can produce ummasking effects similar to acoustic tones. Again a baseline was determined with a 2000 Hz signal amd masker (f1). Two higher-frequency sinusoids (f2 and f3) were added simultaneously to the masker, neither of which produced unmasking when presented individually. When 2f2 - f3 or f3 - f2 was approximately 2300 Hz, unmasking was observed. Next was explored 2f2 - f3 unmasking as a function of f3/f2, keeping 2f2 - f3 frequency fixed at 2300 Hz. As f3/f2 increases, the magnitude of the unmasking decreases. These CT unmasking effects suggest that the generation of CTs must be at the same site or peripheral to the site of suppression.

摘要

描述了两种听觉非线性现象——掩蔽和组合音(CT)产生之间的一些重要关系。通过使用前掩蔽范式提供了一个掩蔽的例子,其中首先通过确定在2000 Hz掩蔽音之前的2000 Hz信号的阈值来获得基线。然后,当第二个音调(抑制音)与掩蔽音同时添加时,信号可能会更容易被听到。在抑制音声压级为80 dB SPL时,对于2300 Hz左右的抑制音频率会出现这种掩蔽解除现象。在抑制音声压级为55 dB SPL时,掩蔽解除效应出现在更接近掩蔽音频率的抑制音频率处。通过在前掩蔽实验中呈现两个正弦波(f1和f2)作为掩蔽音,提供了一个CT产生的例子。结果表明,在保持2f1 - f2 = 2000 Hz的情况下,随着f2/f1的增加,2000 Hz信号的阈值会降低。这与CR的幅度随着f2/f1增加而降低的观点一致。然后我们提供证据表明,CT可以产生与纯音类似的掩蔽解除效应。同样,用一个2000 Hz信号和掩蔽音(f1)确定了一个基线。将两个更高频率的正弦波(f2和f3)同时添加到掩蔽音中,单独呈现时它们都不会产生掩蔽解除现象。当2f2 - f3或f3 - f2约为2300 Hz时,观察到了掩蔽解除现象。接下来研究了在2f2 - f3频率固定为2300 Hz时,2f2 - f3掩蔽解除效应随f3/f2的变化情况。随着f3/f2的增加,掩蔽解除的幅度会减小。这些CT掩蔽解除效应表明,CT的产生必定发生在抑制部位的同一位置或其周边。

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