Synopsis from
the chapter on Ipsilateral Suppression in the book Otoacoustic Emissions
and Clinical Applications . M. Robinette & T. Glattke editors
by George A. Tavartkiladze,
Gregory I. Frolenkov, Alexandr V. Kruglov, Serge V. Artamasov
1. Introduction
Many studies have been devoted to the suppression
of transient evoked otoacoustic emissions (TEOAEs) by contralateral
acoustic stimulation starting with the 1993 paper by the Collet
group in France. It is believed that this effect is mediated by
the medial olivocochlear system (Durrant,
1998; Veuillet, Collet & Morgon, 1992), and
it is relatively small. Typically the TEOAE suppression associated
with contralateral stimuli of 70-75 dB SPL is about 1 to 2 dB (Veuillet
et al., 1991). In contrast to contralateral stimulation,
ipsilateral masking can result in more pronounced suppression of
TEOAE (Kemp & Chum, 1980; Tavartkiladze
et al., 1993; Wilson, 1980). The mechanisms underlying
this effect seem to be twofold. From one view, the suppression results
from intracochlear masking processes; from another view, it appears
to be mediated through the olivocochlear system. This chapter describes
various aspects of TEOAE masking properties under simultaneous and
forward masking conditions that have been investigated for several
years (Frolenkov et al., 1995; Tavartkiladze,
et al., 1991, 1996).
2. Ipsilateral
Simultaneous Masking of TEOAEs
Since the first description by Kemp (1978),
the measurements of TEOAEs have progressed from laboratory research
to clinical application. Today it is universally accepted that OAE
phenomena are of cochlear origin (Probst,
1991; Zurek, 1985). Nevertheless, the particular
segments of the cochlear partition generate TEOAE in response to
a stimulus with given frequency composition remain unresolved (Hilger
et al., 1995; Kemp 1986; Tavartkiladze et al., 1993).
This situation is due to the very complex structure of the TEOAE
frequency spectrums and to the fact that not all frequencies evoke
TEOAEs (Probst et al., 1986).
Constructing TEOAE tuning curves under simultaneous tonal masking
conditions can reveale information about the location of the cochlear
partition vibration maximum. Unfortunately, only a few researchers
have described the results of TEOAE simultaneous masking investigations
(Kemp & Chum, 1980; Wilson, 1980).
3. Simultaneous-Masking
Procedures
All our simultaneous masking experiments were
performed with subjects who were 21 to 33 years of age, with audiometric
thresholds less than 20 dB HLwithin the frequency range of 125-8000
Hz, with type A tympanograms, and no signs of otologic diseases
during the investigation. Because spontaneous otoacoustic emissions
(SOAEs) could modify TEOAE responses (Probst
et al., 1986), the existence of SOAE or (synchronized)
quasi-SOAEs was tested using an ILO 88 system (Otodynamics, Hatfield,
UK).
TEOAEs were recorded with a custom-designed acoustic
probe, consisting of a microphone (EA-1842) and two Knowles (Itasca,
IL) electroacoustic transducers (ED-1913) (Fig. 1).
The free field calibration of the probe microphone was carried out
by short broadband clicks with initial rarefaction wave. The probe
under calibration was placed close to the measuring microphone (4676,
Bruel & Kjaer, Nram, Denmark) connected to a measuring amplifier
(2235 noisemeter, Bruel & Kjaer). Output of the measuring amplifier
was used for calibration of the probe. (The frequency response of
the probe-microphone channel is presented in the left bottom panel
of Fig. 1).
During the experiments, probe-microphone output
was amplified and fed to a Medelec "Sensor-3" clinical averager
using an effective filter bandwidth of 300 Hz (6 dB per octave)
to 6000 Hz (12 dB per octave). One of the electroacoustical transducers
was used to deliver test stimuli, which were 60 and 500 microsecond
clicks, and tone bursts of different frequencies with trapezoidal
envelope: 1 cycle rise/fall, 1 cycle plateau for frequencies less
than 1 kHz, and 2 cycles rise and fall, 3 cycles plateau for frequencies
more than 1 kHz. To reduce intersubject variability of TEOAE amplitude,
the stimulus intensity was related to the subject's sensation level
and set at 20 dB SL to provide selective excitation of the limited
segment of cochlear partition. Test stimuli repetition rate was
20 Hz.
TEOAE-response waveforms were obtained with synchronous
averaging of 2000 consecutive responses to test stimuli. The signal
was then routed into two independent channels of averaging system.
Thus, averaged responses to even and odd stimuli were obtained.
The sum of these curves formed the TEOAE record, and the difference
between them was used for noise-level estimation. The second electroacoustical
transducer was employed to deliver masking tones of different frequencies.
First, the subjective threshold of tone perception was determined
for each frequency. After that, masking was continued with constant
intensity during the averaging process. Any intensity changes were
performed at least 1-2 min before the start of averaging. For masker-artifact
cancellation, the reference masker was attenuated, phase-corrected,
and electrically added to the probe-microphone output (Fig.1)
before leading it to the averager. The degree of attenuation and
phase correction angle were manually adjusted in such a way as to
minimize amplitude of the signal at the averager input. The adjustment
was necessary each time when the frequency or intensity of the masker
tone were changed.
The results obtained were used for the construction
of iso-suppression tuning curves. For each frequency of masking
tone, the relation between the masker intensity (5-60 dB SL) and
TEOAE amplitude was determined. Then the masking tone intensity
necessary for 50% reduction of TEOAE amplitude was approx20uation
was less than 50%, even under the highest levels of masking tone
(50-60 dB SL), the masking tone of this frequency was not considered
to produce TEOAE reduction and this intensity was marked by the
arbitrary value of 180 dB.

Fig 1: Schematic drawing of the
simultaneous masking experiments setup. Left bottom panel represents
the probe-microphone frequency response
4. TEOAE-Amplitude
Calculation
Linear component cancellation (Bray
& Kemp, 1987; Kemp,et al., 1986) was not suitable
for these experiments, because the method dramatically reduced the
amplitude of TEOAE evoked by stimuli of a relatively low intensity
(Frolenkov et al., 1995; Grandori
& Ravazzani, 1993; Tavartkiladze et al., 1994).
Instead, TEOAEs were recoeded by ordinary averaging. However, the
linear component cancellation was used for the determination of
time window of analysis. For this purpose, the control TEOAE recordings
were made at different click intensities (0-46 dB SL), and for each
subject the difference was obtained between TEOAE records to 30
dB SL click and to 20 dB SL click after multiplying the latter record
by a 10 dB correction coefficient (Fig. 2). The
difference consisted of non-linear TEOAE components only and was
used to determine the analysis window (Fig. 2).
Additionally, the appropriateness of the time window estimate was
determined by the construction of input/output curves for the RMS
amplitude of TEOAE in time intervals shorter than window chosen.
Any time intervals that did not include non-linear TEOAE components
were excluded from consideration. Hamming window function and Fast
Fourier Transform (FFT) was performed. The amplitude of the TEOAE
was calculated as the square root of the difference between the
signal power and noise power in the frequency range where the spectrum
of signal exceeded that of noise more than 3 dB.
Fig.2. - Analysis time determination. A, B:
TEOAE responses evoked by 50 s clicks with intensity of 30 dB
SL and 20 dB SL correspondingly. C: The difference of the
above recordings after multiplying of the record by the 10 dB
correction coefficient. This difference consists of non-linear
TEOAE components only and was used to determine the analysis window
(indicated by horizontal line). The zero point on the time scale
corresponds to the stimuli onsets. Stimulus artifact on record
C was not completely cancelled due to the signal
limitation by the ADC converter.
5. TEOAE Tuning
Properties
The TEOAEs were suppressed in all the experiments
with simultaneous tonal masking. Fig. 3 shows typical
TEOAEs recorded in response to 1.5-kHz tone bursts without masking
and with masking tone of various intensities. In the experiments,
the masking effect increased directly with the sensation level of
the masking tone. With the tone at 40 dB SL, almost total suppression
of TEOAE was observed. Such significant response suppression was
found only at the masking-tone frequency equal or close to that
of the tone burst (Fig. 3).

Fig.3 : TEOAE reduction under simultaneous masking
by 1.5-kHz tone of increasing intensity (indicated on the records).
OAEs were evoked by 1.5-kHz, 20-dB SL tone bursts.
Fig. 4 shows typical iso-suppression tuning curves of tone-burst
and click-evoked OAEs. In all subjects and for all stimuli the tuning
curve corresponded to the TEOAE frequency spectrum. In the case
of tone-burst stimulation, locations of the maxima of the TEOAE
and stimulus spectrum and tuning-curve tip were the same. The tuning
properties of click-evoked OAE were different, and TEOAE spectral
maxima, as well as TEOAE tuning-curves tips, did not correspond
to the stimulus spectra. Indeed, clicks of various duration (60
microseconds and 500 microseconds) had quite different spectra .
Irrespective of the click-stimuli spectra, the spectra of TEOAE
were practically identical, and correspondingly similar TEOAE tuning-curves
were obtained. In addition, the smaller difference between the tip
and the low-frequency segment of the tuning curve with the 500 microseconds
stimulus closely correlated to the existence of low-frequency TEOAE
components which were not observed for the 60 microseconds click
stimulation. In this subject tone burst stimulation with a frequency
of 1.5 kHz was the most effective for the TEOAE excitation . The
TEOAE evoked by this stimulus had in its spectrum essentially the
same peaks that dominated in the spectra of TEOAE to broad-band
stimulation . As a result, the tuning curve of the TEOAE to the
1.5 kHz tone burst was similar to the tuning curves of click-evoked
OAEs. TEOAE spectra of all test subjects were characterized by the
dominant peaks within the 1 to 2 kHz range, and the peaks strictly
determined the tuning curves of both OAEs evoked by clicks of different
duration and TEOAE to the tone burst of the most effective frequency.
Nevertheless, this apparent independence of TEOAE-frequency composition
and iso-suppression tuning curves from the stimuli spectra was only
relative. When the stimulus energy was concentrated within the frequency
range which did not comprise the frequencies of the dominant peaks
of TEOAE to broad-band stimulation, the TEOAE with different frequency
composition was observed . For example, OAEs evoked by 2.5 kHz tone
bursts had the spectral peaks within the range of 1.8 to 2.6 kHz
and the tuning curve with the tip located around 2.5 kHz (Fig.
4). Comparison of the tone-evoked OAE tuning curves showed
that OAEs evoked with 2.5 kHz tone burst was characterized by a
somewhat wider tuning curve than the TEOAEs to 1.5 kHz stimulation.
This difference was not surprising considering the wider spectrum
of TEOAE to the 2.5 kHz tone burst (Fig. 4). The
tuning-curves shape with typical flat low frequency "plateau" and
steep high frequency rise (Fig. 4) was observed
in all subjects.

Fig. 4. Iso-suppression tuning
curves (top) of OAEs evoked by clicks of different durations
(A) and by tone bursts of different frequencies (B).
Bottom records show from top to bottom: the spectra of stimuli and
the spectra of corresponding TEOAEs. Stimuli intensity was 20 dB
SL. Dashed lines indicate noise level.
The relation of TEOAE simultaneous-masking properties
to the TEOAE-frequency composition was further explored by construction
of tuning curves of the separate TEOAE frequency components (Fig.
5). It was found that the components were suppressed independently
and had individual tuning curves with the typical shape (Fig.
4). The tips of the tuning curves were closely related
to the frequency of separate components (Fig. 5).
The intensities of masking tones that corresponded to the tuning
curves tips tended to be higher for dominant peaks (Fig.
5). Usually the amplitudes of the TEOAE frequency components
differed, and the tuning curve constructed from total TEOAE spectrum
was determined by the contribution of TEOAE dominant spectral peaks
(Fig. 5). Finally, the the independent suppression
of the TEOAE frequency components was observed in all the subjects.
Unfortunately, neither subjects had SOAEs, and it could not be determined
how the presence of SOAEs could modify the suppression of TEOAE
spectral constituents.
Fig.5 - Iso-suppression tuning curves of the
separate frequency components of 500 m
s-click evoked OAE (left) and of the overall TEOAE
response (right). The tuning curves were constructed for
the frequency ranges indicated above the TEOAE spectrum (bottom
records). Dashed lines indicate noise level.
6. Ipsilateral
Forward Masking of TEOAE
Neurons of the medial olivocochlear system (MOCS)
can be effectively activated with both contralateral and ipsilateral
sound (Liberman & Brown, 1986).
Direct electrical stimulation of the crossed olivocochlear bundle
(the subsystem of the MOCS presumably consisting of the ipsilaterally
activating efferent fibers (Warren
& Liberman, 1989) at the floor of the IV ventricle)
has resulted in bilateral desensitization of the cochleas (Rajan,
1988, 1990), as well as in the suppression of the
DPOAEs (Mountain, 1980).
Therefore, it is reasonable to suggest some functional significance
of the ipsilaterally activated olivocochlear feedback. Nevertheless,
the latter reflex arc has received little attention in the literature.
Evidence was presented for the involvement of efferent system in
the ipsilateral forward-masking of the compound-action potential
(Bonfils & Puel, 1987),
and in the ipsilateral forward masking of TEOAE, demonstrated by
the comparison between ipsilateral, contralateral, and binaural
forward masking of TEOAE (Berlin et
al., 1995). Nevertheless, the majority of the data
related to the cochlear efferent physiology were obtained in experiments
on the anesthetized animals, which may have changed reflex properties
of the efferent neurons (Liberman
& Brown, 1986). As a result, in an awake human
being even the question about the latency of the contralateral activation
of MOCS is still disputable (Lind,
1994). There are indications for the existence of
the ipsilaterally activated efferent suppression of TEOAE in normal
hearing subjects (Tavartkiladze et
al., 1996). Comparison of the ipsilateral and contralateral
efferent-mediated TEOAE suppressions in the same subject could be
useful for the clinical testing of MOCS functioning.
7. Forward-Masking
Experiment
As in the simultaneous-masking studies, subjects
investigated were normal-hearing subjects with no history of otologic
disease, with audiometric thresholds less than 20 dB within the
frequency range of 125-8000 Hz, and type-A tympanograms. Absence
of the spontaneous OAEs was proved by the ILO 88 analyzer (Otodynamics).
Suppression of TEOAE by the continuous contralateral-noise stimulation
is known to be of the same order of magnitude as the TEOAE spontaneous
changes (Berlin et al., 1993)
and slightly more than the TEOAE changes with directed attention
(Froehlich et al., 1993).
The TEOAE suppression by relatively short acoustic stimuli (clicks
or broad-band noise no more than 30 ms duration) was investigated.
This effect was expected to be somewhat smaller than the suppression
associated with continuous noise presented contralaterally. To minimize
baseline changes all TEOAE recordings were performed in one lengthy
recording session without change of the probe’s position in the
test ear.
The ILO88 system (with software version 3.94L)
was set up with uniform (80-microseconds) linear clicks as stimulus
1 and quad-spaced clicks as stimulus 2. Stimulus 1 was routed to
channel A as the ipsilateral acoustic stimulus. Stimulus 2 was fed
to channel B. In click-to-click forward masking experiments, the
latter stimulus was delivered ipsilaterally through the second electroacoustic
transducer of ILO probe and was used as a masker. In noise-to-click
forward masking experiments, output of the channel B triggered the
general-purpose digital generator (HP33120A, Hewlett Packard). After
appropriate attenuation (output attenuator of the Midimate 602 audiometer,
Madsen Electronics) digitally generated broadband (bandwidth: 50-8000
Hz) noise bursts of 10 or 30 milliseconds duration were delivered
ipsilaterally to the second electroacoustic transducer of the ILO
probe or contralaterally to the TDH-39 headphone. Canceling of masking-signal
artifact was observed in the course of averaging because the ILO
system alternates the phase of every accepted stimulus and response.
Before the execution of forward masking experiments, the TEOAE was
also masked by continuous broad-band noise delivered contralaterally.
In all forward masking experiments test clicks were delivered in
sequence (inter-click interval 30 milliseconds) with the repetition
rate of 3 Hz (Fig. 6). Such a low stimulation rate
was used in order to guarantee a 200 milliseconds pause between
the test series. This time was probably essential for the excitation
decay in the olivocochlear reflex arc (Giraud
et al., 1997; Warren & Liberman, 1989). Emission
to each test click was stored separately. At least 1000 TEOAE responses
were recorded without windowing. After averaging TEOAE responses
in each software buffer (to different test clicks) were time-windowed
(4-15 milliseconds) and their RMS amplitudes were calculated using
ILO88 software. To trace baseline variations in response amplitude
(see for example: (Berlin et al.,
1993), TEOAE records were obtained alternatively:
with and without contralateral or ipsilateral masking stimulation.
Each TEOAE record in the presence of noise preceded the record without
a masker. The mean differences (and their standard errors) of TEOAE
amplitudes from these pairs (5 pairs per each point) were calculated.
The time delay (D t) between the
the onset of masker and the second test click in sequence was adjusted
to be 1 to 30 milliseconds (Fig. 1). In noise-to-click
forward masking experiments it was fixed at two predetermined values:
0 milliseconds (test A) or 15 milliseconds (test B). A tone-tailed
test (t-test) was applied to determine the statistical
significance of the TEOAE amplitude changes under masking conditions.
Fig. 6. Time patterns used in forward masking
studies. For the picture clarity only the case of noise-to-click
masking was illustrated. Test clicks were separated by the 30
ms interval. Test sequences were delivered with the rate of 3
Hz. Time delay (D t) between the
masker onset and the second click in the test sequence varied
from 1 to 30 milliseconds in click-to-click masking experiments
and was equal to 0 (test A) or 15 milliseconds (test B) in noise-to-click
masking experiments.
8. Contralateral
Masking With Continuous Broad-Band Noise
Contralateral noise remarkably reduced the TEOAE
amplitude. In one subject OAE evoked by the clicks of moderate intensity
of 65.5 dB SPL (relating to subjective threshold it was 30 dB SL)
were diminished by as much as 2.3 dB with the use of 60 dB SL contralateral
noise. The effect was observed at the masker intensities up to 30
dB SL .
9. Ipsilateral
Click-to-Click Forward Masking
TEOAEs were dramatically suppressed during the
first ms after masking click delivery (Fig. 7).
This suppression consisted in the overall decrease of emission-time
components with maybe a more prominent reduction of long-latency
emission. the amplitude of emission recovered to 90% of the control
value in 5 milliseconds. Changes of emission amplitude at longer
interstimulus intervals were not significant.

Fig.7. Changes of TEOAE amplitude
with interstimulus time interval (D
t) under click-to-click forward masking conditions. Filled circle
indicates the control TEOAE amplitude (TEOAE amplitude to the first
click in test sequence). Dashed line indicates noise level.
Test click intensity = 20 dB SL; masking click intensity = 46 dB
SL.
10. Contralateral
Versus Ipsilateral Noise-To-Click Forward Masking
Contralateral broad-band noise burst stimulation
with the intensity of 50 dB SL (65 dB nHL) evoked statistically
significant reduction of TEOAE amplitude 15 milliseconds after masker
onset (Fig.8). This effect became more prominent
with the increase of noise duration up to 30 milliseconds. The same
noise stimulation presented ipsilaterally, evoked similar effect
at the intervals between masker and the test of more than 30 milliseconds
(Fig. 8). These effects could not be related to
the efferent feedback activation by the test sequence because there
were no statistically significant changes in the amplitude of OAE
evoked by different clicks in test sequence without masking (Fig.
8). The time course of ipsilateral and contralateral suppressions
was practically identical. Nevertheless, the prominent ipsilateral
suppression at the masker-stimulus onset delay of 15 milliseconds
was also found. It corresponded to the 5 milliseconds difference
between masker end and the stimulus delivery, and obviously related
to the dramatic TEOAE suppression revealed in click-to-click forward
masking experiment (Fig. 7).
Fig 8. Temporal dynamics of contralateral
(A) and ipsilateral (B) suppression
of TEOAE. Each point represents the mean difference of TEOAE amplitudes
(5 pairs) recorded in masker-on and masker-off conditions. Open
squares on B show the mean TEOAE amplitudes without
masker. The latter amplitudes were related to the mean amplitude
of TEOAE evoked by the first click in test sequence. Error bars
indicate standard errors.
11. Middle-Ear
Reflexes
In noise-to-click forward-masking experiments noise
intensities as high as 50 dB SL were used. With the noise presented
continuously, this value was found to be only slightly below the
threshold of stapedial muscle reflex in this subject. Nevertheless,
the middle-ear reflex threshold using short-noise bursts of the
maximum for our experiments duration (30 milliseconds), was determined
to be as much as 80 dB SL, which is 30 dB higher than the intensity
used in masking experiments . To eliminate the possibility of the
middle-ear reflexes which cannot be recorded with conventional impedance
measurements, the sound pressure in the outer-ear canal during alternative
presentation of contralateral noise was evaluated. There was no
pressure excursion at the 40 to 110 milliseconds poststimulus time
when the stapedial reflex could be observed (Fisch
& Schulthess, 1963; Metz, 1951). The observation
could not rule out the theoretical possibility of slowly developing
reflex tension in the middle-ear muscles. In order to exclude this
possibility, the TEOAE amplitudes were compared without masker and
just before masker onset (it is a response to the first click in
test sequence). No statistically significant differences were found
(Tavartkiladze et al., 1997).
12. Efferent-Mediated
Effects in Ipsilateral-TEOAE Suppression
The magnitudes of the TEOAE suppression caused
by contralateral continuous noise (e.g., 0.6 dB with the contralateral
noise at 30 dB SL in one subject were only slightly less than previously
reported mean values for normal-hearing subjects (0.7 dB with the
masker intensity of 20 dB SL) (Collet
et al., 1990). Hence, the excitability of the olivocochlear
reflex arc (at least from contralateral side) was unlikely to differ
significantly from the typical one. The dramatic decrease of the
TEOAE under click-to-click forward-masking conditions at the interstimulus
intervals smaller than 5 ms (Fig. 7) could be attributed
exclusively to the intracochlear processes due to the longer minimal
latency of the medial olivo-cochlear neuron responses to the external
sound. This latency was found to be at least 6-8 ms in cat (Liberman
& Brown, 1986) and 7 milliseconds in guinea
pig (Brown, 1989),
and there is no reason to expect the significant reduction of this
time in human beings. Moreover, practically complete TEOAE inhibition
observed withing the first 5 ms poststimulus (Fig. 7)
correlated well with the degree of the TEOAE suppression that was
reported previously for the ipsilateral simultaneous TEOAE masking
(Tavartkiladze et al., 1994).
Hence, the TEOAE suppression observed 5 ms after the end of ipsilateral
masking noise burst (Fig. 8) may have been mainly
of cochlear origin.
It is known that short acoustic clicks with relatively
low repetition rate are quite ineffective in eliciting efferent
response (Liberman & Brown, 1986).
Longer stimuli (i.e., tone bursts of 50 milliseconds) are capable
of exciting the MOCS neurons (Brown,
1989). Accordingly, noise bursts presented contralaterally
or ipsilaterally elicited a statistically significant TEOAE reduction
30 milliseconds and more after the end of noise stimulation (Fig.
8). The latency of this effect from the contralateral side
was found to be less than 15 milliseconds (Fig. 8).
This value differs somewhat from the previously reported estimate
of the contralateral TEOAE-suppression latency (less than 40-140
milliseconds) (Lind, 1994)
and from the latency of the efferent-mediated ipsilateral suppression
of the compound-action potential in guinea pigs [30-40 milliseconds
(Bonfils & Puel, 1987].
So far no systematic studies of this question have been performed.
Moreover, at the 15 milliseconds interval between contralateral
noise and test click the possibility that additional TEOAE suppression
related to the intracochlear processes on the ipsilateral side cannot
be exclude. The degree of acoustic isolation between the two ears
was not greater than 40 dB, and attenuated noise could stimulate
ipsilateral cochlea owing to crosstalk. Nevertheless, the effect
at longer noise-to-click intervals appears to result from MOCS activation
because (1) its duration was not explained by intracochlear suppression
(Fig. 7 and 8) and (2) the suppression magnitude
was similar from ipsilateral and contralateral sides. The long duration
of the efferent-mediated inhibition of TEOAE (more than 80 milliseconds;
see Fig. 8) did not contradict previously reported
TEOAE forward masking data (Gobsch
et al., 1992; Lind, 1994) and other studies of ipsilateral
effects (Berlin et al., 1995).
The most striking result of our experiments was
the close resemblance of the magnitudes and time courses of the
efferent-mediated effects elicited from contralateral and ipsilateral
sides (Fig. 8). Berlin,
et al. (1995) compared
forward masking of TEOAE by ipsilateral, contralateral and binaural
noise. In full accordance with the data presented in this chapter,
they found TEOAE suppression of approximately the same magnitude
(about 0.5 dB) for both ipsilateral and contralateral noise stimulation.
Binaural noise stimulation caused more prominent reduction of TEOAE
amplitude (about 1-1.5 dB). Differences between ipsilateral and
contralateral effects were not significant 20 to 100 milliseconds
after noise stimulation (Berlin et
al, 1995). These results appear to contradict the
results of Liberman and Brown (1986)
who reported that 59% of MOCS neurons are most sensitive to the
ipsilateral stimuli, 29%, to the contralateral ones, and 11%, from
both. Consequently one could expect some difference in the magnitude
of the efferent-mediated TEOAE suppression evoked by contralateral
and ipsilateral stimulation. This discrepancy may be related to
the fact that the MOCS neuron excitability pattern depends on the
level of general anesthesia. Indeed, it was speculated that percent
of binaurally responding MOCS neurons can be higher in less anesthetized
animals (Liberman & Brown, 1986).
Moreover, in unanesthetized decerebrated cats, 60% of efferent units
were reported to respond to both contralateral acoustic stimulation
and ipsilateral electrical stimulation (Fex,
1962, 1965). Thus, in awake human beings, a significant
portion of MOCS neurons can be expected to be bilaterally activated.
This could explain the similar magnitudes of the efferent-mediated
TEOAE suppressions evoked by contralateral and ipsilateral stimuli.
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