Fine structure of the intracochlear potential field. II. Tone-evoked waveforms and cochlear microphonics
M. Zidanic and W. E. Brownell Department of Otolaryngology, Head and Neck Surgery, Johns Hopkins University, Baltimore, Maryland 21205-2195. 1. Extracellular evoked potentials to low-frequency pure-tone stimuli were recorded in the second cochlear turn of the anesthetized guinea pig. Spatial variati...
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Veröffentlicht in: | Journal of neurophysiology 1992-01, Vol.67 (1), p.108-124 |
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Zusammenfassung: | M. Zidanic and W. E. Brownell
Department of Otolaryngology, Head and Neck Surgery, Johns Hopkins University, Baltimore, Maryland 21205-2195.
1. Extracellular evoked potentials to low-frequency pure-tone stimuli were
recorded in the second cochlear turn of the anesthetized guinea pig.
Spatial variations of the field potentials were characterized by advancing
and withdrawing micropipettes along radial tracks in scala tympani (ST) and
scala vestibuli (SV). Compound action potentials (CAPs) and cochlear
microphonics (CM) are the major components of the evoked responses to 50-
to 1,600- Hz stimuli. The relative contribution of CM and CAP to the evoked
potentials varies with cochlear scala and location within the scala as well
as with stimulus frequency and intensity. 2. In the 50- to 800-Hz frequency
range, the largest CM in the second turn was recorded from scala media
(SM). Below 500 Hz the CM in SV is larger than in ST, whereas above 500 Hz
a larger CM is present in ST. The CM in SV is nearly in phase with the CM
in SM, although it is smaller by a factor of two to four. The CM diminishes
by another factor of two over a 100-microns depth range as an electrode is
withdrawn out of SV through the spiral ligament. While the electrode is in
SV or in the fluid outside the spiral ligament, the CM magnitude does not
change by greater than 10%. The shape of the radial CM magnitude profile
along tracks in SV shows little or no dependence on intensity in the 65- to
105-dB SPL range or on frequency in the 50- to 800-Hz range. 3. Unlike the
CM profiles in SV, the shape of the CM magnitude and phase profiles in ST
are a complex function of frequency and intensity. Below 500 Hz, the CM
goes through a 140-180 degree radial phase shift over a 100-microns
distance near the spiral ligament bordering ST. Concomitant with the large
radial phase shift is a local minimum of the CM magnitude. The location of
this "virtual ground point" can shift radially by as much as 100 microns
over a 30-dB intensity range. The CM magnitude deep in ST is always larger
than the CM outside the spiral ligament bordering ST. However, the ratio of
the CM magnitudes at these two locations can vary from 0.1 to 0.8, the
ratio tending to increase with intensity in the 200- to 800-Hz
range. |
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ISSN: | 0022-3077 1522-1598 |
DOI: | 10.1152/jn.1992.67.1.108 |