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Journal ArticleDOI

Observations of the Vibration of the Basilar Membrane in Squirrel Monkeys using the Mössbauer Technique

William S. Rhode
- 01 Apr 1971 - 
- Vol. 49, Iss: 4, pp 1218-1231
TLDR
The amplitude and the phase of vibration of the basilar membrane and the bony limbus of the cochlea were measured in living squirrel monkeys using the Mossbauer technique.
Abstract
The amplitude and the phase of vibration of the basilar membrane and the bony limbus of the cochlea were measured in living squirrel monkeys using the Mossbauer technique. In the middle ear, the vibration of the malleus (and occasionally the incus) was measured. The Mossbauer technique makes possible the measurement of very small velocities, e.g., 0.2 mm/sec. This sensitivity permits measurement of the motion of the malleus at sound‐pressure levels (SPLs) of 90 to 110 dB and measurement of the motion of the basilar membrane at 70 to 120 dB SPL, depending on the frequency. The basilar membrane vibrates nonlinearly for frequencies which produce the largest deflections at the spot on the basilar membrane under observation. The ratio of the displacement of the basilar membrane to that of the malleus was observed to have the following characteristics: (1) As the frequency is increased from a low value, its amplitude increases at 6 dB/oct until just below the maximum ratio where the slope increases to about 24 dB/oct; (2) the maximum ratio was about 24 dB for the SPLs used; (3) for frequencies above that producing the maximum ratio, the drop‐off rate was approximately 100 dB/oct; (4) the amplitude ratio did not drop off indefinitely but tended to level off; (5) the motion of the basilar membrane differs from the motion of the malleus by 90° at very low frequencies; (6) for frequencies below that producing the maximum ratio, the phase differences between the motion of the basilar membrane and that of the malleus is a linear function of frequency; (7) near the frequency corresponding to the maximum ratio, the phase difference decreases at a faster rate; and (8) the phase difference approaches a constant value (7π 8π or 9π) for high frequencies. Anatomical constraints allowed only a small portion of the basal turn to be studied (6.5–7.5 kHz produced maximum deflection of the basilar membrane in this region).

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Journal ArticleDOI

Mechanics of the Mammalian Cochlea

TL;DR: The high sensitivity and sharp-frequency tuning, as well as compression and other nonlinearities (two-tone suppression and intermodulation distortion), are highly labile, indicating the presence in normal cochleae of a positive feedback from the organ of Corti, the "cochlear amplifier."
Journal ArticleDOI

Stable propagation of synchronous spiking in cortical neural networks

TL;DR: The results indicate that a combinatorial neural code, based on rapid associations of groups of neurons co-ordinating their activity at the single spike level, is possible within a cortical-like network.
Journal ArticleDOI

Basilar-membrane responses to tones at the base of the chinchilla cochlea

TL;DR: Basilar-membrane responses to single tones were measured, using laser velocimetry, at a site of the chinchilla cochlea located 3.5 mm from its basal end, and compressive growth of responses to tones with frequency near CF is accompanied by intensity-dependent phase shifts.
Journal ArticleDOI

Evoked otoacoustic emissions arise by two fundamentally different mechanisms: A taxonomy for mammalian OAEs

TL;DR: Two broad classes of emissions--reflection-source and distortion-source emissions--are distinguished based on the mechanisms of their generation, and the implications of this OAE taxonomy for the measurement, interpretation, and clinical use of otoacoustic emissions as noninvasive probes of cochlear function are discussed.
Journal ArticleDOI

Phase-locking in the cochlear nerve of the guinea-pig and its relation to the receptor potential of inner hair-cells.

TL;DR: The high-frequency limit of phase-locking has been measured in fibres of the auditory nerve in the guinea-pig and it is shown that phase- locking begins to decline at about 600 Hz and is no longer detectable above 3.5 kHz.
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