 |
Previous Article | Next Article 
The Journal of Neuroscience, January 15, 2003, 23(2):716-724
Interaural Time Difference Discrimination Thresholds for
Single Neurons in the Inferior Colliculus of Guinea Pigs
Trevor M.
Shackleton1,
Bernt C.
Skottun2,
Robert
H.
Arnott1, and
Alan R.
Palmer1
1 Medical Research Council Institute of Hearing
Research, University Park, Nottingham, NG7 2RD, United Kingdom, and
2 Skottun Research, Piedmont, California 94611-5154
 |
ABSTRACT |
Sensitivity to changes in the interaural time difference
(ITD) of 50 msec tones was measured in single units in the inferior colliculus of urethane-anesthetized guinea pigs. ITD functions were
measured with 100 repeats and fine spacing (100 points per cycle). The
just noticeable difference (jnd) for ITD was determined using receiver
operating characteristic (ROC) analysis of the spike-count distribution
at each ITD. The jnd became progressively smaller as the signal
frequency increased from 50 to 800 Hz but became unmeasurable above 1 kHz. The lowest jnds (30 µsec) were comparable with human jnds,
indicating that there is sufficient information in the firings of
individual neurons to permit discrimination without obligatory pooling.
ROC analysis requires the choice of a reference ITD from which the jnd
may be found by stepping the target ITD through the ITD function. For
each neuron the reference was chosen to minimize the jnd. The lowest
jnd was usually for ipsilateral leading references, near the minimum of
the ITD function where the variance was also low, but where the slope
was nearing its steepest. This was despite the peak of the ITD function
occurring for contralateral leading stimuli. When the reference ITD was on midline, a jnd could be obtained by looking for firing rates either
greater or smaller than the firing rate at midline. The lower jnd was
usually obtained by looking for a decrease in firing rate. As duration
increased, jnds either decreased or increased, depending on unit type,
whereas when level increased, jnds generally increased.
Key words:
ITD; jnd; discrimination threshold; inferior
colliculus; guinea pig; binaural; interaural time difference
 |
Introduction |
For humans, the azimuthal
localization of sounds below 1500 Hz is mediated primarily by
sensitivity to the small difference in travel time to the two ears
[interaural time difference (ITD)]. The smallest change in the ITD of
pure tones detectable by humans [just noticeable difference (jnd)] is
10-20 µsec (Mills, 1958 ; Durlach and Colburn, 1978 ; Hafter et al.,
1979 ). This sensitivity is normally modeled using an array of
coincidence detectors, each of which fires maximally when spikes from
the two ears arrive at the same time, via axons with different
propagation delays, hence showing sensitivity to a particular ITD
(Jeffress, 1948 ). Neurons in the medial superior olive (MSO) behave
like coincidence detectors (Goldberg and Brown, 1969 ; Yin and Chan,
1990 ; Spitzer and Semple, 1995 ; Batra et al., 1997a ,b ). Because the
variability in synaptic delay is much larger than the psychophysically
determined jnd, it has been widely assumed that jnds as low as those of
humans could only be achieved if the responses from many neurons were combined (Hall, 1965 ; Yin and Chan, 1988 ; Carr, 1993 ; Gerstner et al.,
1996 ; Fitzpatrick et al., 1997 ; Yin et al., 1997 ).
There are examples, however, where the resolution measurable from
single neurons reflects the psychophysical thresholds. Individual neurons in the visual and somatosensory systems carry sufficient information to achieve performance comparable with psychophysical thresholds (Johansson and Vallbo, 1979 ; Bradley et al., 1985 ; Parker
and Hawken, 1985 ; Newsome et al., 1989 ; Hawken and Parker, 1990 ;
Vallbo, 1995 ). Individual auditory nerve fibers also carry sufficient
information to exceed human capability in tone detection and forward
masking (Relkin and Pelli, 1987 ; Relkin and Turner, 1988 ) and to equal
human capability in detecting tones in noise (Young and Barta, 1986 ).
Single goldfish auditory nerve fibers provide for level discrimination
that exceeds the animal's behavioral capability, although they do not
reach human performance (Fay and Coombs, 1992 ). In light of these
findings, which show that some individual neurons can match
psychophysical thresholds, it is important to reexamine the assumption
that behavioral ITD jnds require pooling across many cells.
The sensitivity to a change in stimulus is dependent on both the
variability in the response to a constant stimulus and the change in
response when the stimulus is changed (Green and Swets, 1974 ). It is
therefore vital that, in addition to the mean rate, the distribution of
neural spike counts to repeated stimulation is measured. Skottun
(1998) , using published mean rate responses (Stanford et al., 1992 ),
showed that single inferior colliculus (IC) and thalamic neurons can
achieve ITD jnds as small as those obtained in humans. However, he had
to make assumptions about the spike distributions. These were
subsequently measured in the IC of guinea pigs (Skottun et al., 2001 ),
which confirmed the earlier finding. In this paper, we study in greater
detail the ability of single IC neurons to signal differences in ITD.
We particularly focus on the effects of unit type, signal duration, signal level, and other factors relating to the comparison between neural and behavioral performance.
 |
Materials and Methods |
Recordings were made in the right IC of 15 pigmented guinea pigs
weighing 335-507 gm; in many of these experiments data were also
collected for other purposes. Animals were anesthetized with urethane
(1.3 gm/kg, i.p., in 20% solution in 0.9% saline) and Hypnorm
(Janssen, High Wycombe, UK) (0.2 ml, i.m., comprising fentanyl
citrate 0.315 mg/ml and fluanisone 10 mg/ml). To prevent bronchial
secretions, atropine sulfate (0.06 mg/kg, s.c.) was administered at the
start of the experiment. Anesthesia was supplemented with further doses
of Hypnorm (0.2 ml, i.m.), on indication of pedal withdrawal reflex. A
tracheotomy was performed, and core temperature was maintained at
38°C via a heating blanket and rectal probe. The animals were placed
inside a sound attenuating room in a stereotaxic frame in which hollow
plastic speculas replaced the ear bars to allow sound
presentation and direct visualization of the tympanic membrane. A
craniotomy was performed over the position of the IC. The dura was
reflected, and the surface of the brain was covered by a solution of
1.5% agar in 0.9% saline. Respiratory rate was monitored by means of
a fine polythene tube inserted into the tracheal cannula connected to a
low-pressure transducer; heart rate was monitored using a pair of
electrodes inserted into the skin to either side of the animal's
thorax. All experiments were performed in accordance with the United
Kingdom Animal (Scientific Procedures) Act of 1986.
Recordings were made with glass-insulated tungsten electrodes (Bullock
et al., 1988 ) advanced into the IC (optional charge) through the intact
cortex, in a vertical penetration, by a piezoelectric motor (Burleigh
Inchworm IW-700/710). Extracellular action potentials were amplified
(Axoprobe 1A, Axon Instruments, Foster City, CA), discriminated using a
level-crossing detector (SD1, Tucker-Davies Technologies), and their
time of occurrence was recorded with a resolution of 1 µsec.
Stimuli were delivered to each ear through sealed acoustic systems
comprising custom-modified Radioshack 40-1377 tweeters joined via a
conical section to a damped 2.5-mm-diameter, 34-mm-long tube (M. Ravicz, Eaton Peabody Laboratory, Boston, MA), which fit into the
hollow speculum. The output was calibrated a few millimeters from the
tympanic membrane using a Brüel and Kjær 4134 microphone fitted
with a calibrated 1 mm probe tube.
All stimuli were digitally synthesized (Tucker-Davies Technologies
System II) at between 100 and 200 kHz sampling rates and were output
through a waveform reconstruction filter set at 1/4 the sampling rate
(135 dB/octave elliptic: Kemo 1608/500/01 modules supported by custom
electronics). If not stated otherwise, stimuli were of 50 msec
duration, switched on and off simultaneously in the two ears with
cosine-squared gates with 2 msec rise/fall times (10-90%). The search
stimulus was a binaural pure tone presented every 250 msec, of variable
frequency and level. An ITD of 0.1 cycles was used for the search
stimulus because this is the modal characteristic delay in the IC
(McAlpine et al., 2001 ). When a unit was isolated the best frequency
(BF) and threshold at BF were obtained audiovisually. Units were then
characterized by a battery of tests that are detailed below.
Frequency response areas were obtained with single presentations of
diotic pure tones that were randomly chosen over a range of frequencies
from four octaves below BF to two octaves above BF with a spacing of
1/8 octave and levels from 100 to 0 dB attenuation in 5 dB steps.
Maximum sound level was ~100 dB sound pressure level between 50 Hz
and 1.5 kHz. The number of spikes elicited between 10 and 60 msec after
the stimulus onset was represented as colors on an attenuation versus
frequency grid. Responses were classified as type V, with a wide
V-shaped excitatory area; type I, with a restricted I-shaped region of
excitation that was flanked by no response at lower and higher
frequencies; or type O, with an O-shaped island of excitation at low
stimulus levels that was bounded by no response, or significantly
reduced response, at higher levels (Ramachandran et al., 1999 ).
Rate level functions were obtained using both noise and BF tones,
presented both monaurally and binaurally at a repetition rate of five
per second. Ten repeats of levels between 0 and 100 dB attenuation in 5 dB steps were presented in random order. Every level was presented
before any particular level was repeated. All spikes between 10 and 80 msec after the stimulus onset were included in the spike count.
Peristimulus response histograms (PSTHs) were obtained using 100 repeats of BF tones, presented both monaurally and binaurally at a
repetition rate of five per second at 20 dB above threshold. Tones were
presented in sine phase. Responses were classified into six types:
sustained units fired throughout the stimulus but lacked the onset peak
that characterized on-sustained types; onset units fired for <5 msec
at the stimulus onset, whereas broad-onset units fired for up to 30 msec after stimulus onset; pauser units had a precisely timed onset
peak followed by a lower level of sustained activity separated by a
cessation, or near cessation, of activity; multiple units had several
peaks of activity during the course of the stimulus (Le Beau et al.,
1996 ).
Binaural beat responses were obtained with the tone to the
contralateral ear (relative to recording site) being 1 Hz higher in
frequency than that to the ipsilateral ear (Yin and Kuwada, 1983a ).
This causes interaural phase to change during the stimulus, completing
a full cycle in 1 sec. The phase of the stimulus at the contralateral
ear leads that at the ipsilateral ear during the first half cycle. The
total duration of each beat stimulus was 3000 msec, producing three
cycles of interaural phase difference (IPD) for each of the 10 repetitions of the stimulus. Stimuli were presented every 6030 msec.
Mean best phase (BP) and vector strength, relative to the beat
frequency, were calculated from the middle two cycles of the beat
response (from 0.5 to 2.5 cycles), using the method of Goldberg and
Brown (1969) . A range of different carrier frequencies around BF were
sometimes used to assess the binaural type and degree of convergence
onto the unit (McAlpine et al., 1998 ).
ITD functions were obtained by delaying, or advancing, the fine
structure of the signal to the ipsilateral ear while keeping the signal
to the contralateral ear fixed. Positive ITDs correspond to the signal
at the contralateral ear leading (i.e., signal to ipsilateral ear
delayed). Signals were gated on and off simultaneously in the
two ears with rise/fall times of 2 msec. The signals were 50 msec tone
bursts at BF and 20 dB above rate threshold. Spikes were included in
the spike count if they occurred between 10 and 80 msec after the
stimulus onset. We first obtained ITD functions over ±1.5 cycles of BF
in 0.1 cycle steps using 50 repeats at a repetition rate of five per
second to determine the BP of the unit and the range over which to
perform a fine grained analysis (Fig.
1A, open
symbols). A fine-grained analysis was then performed from the
trough to the peak of the slope through zero ITD (Fig. 1A, filled symbols), which was also
usually the steeper slope (McAlpine et al., 1998 ). The step size was
normally 0.01 (or, occasionally, 0.02) cycles, and 100 repeats were
obtained. A single repeat consisted of the full range of ITD steps
presented in pseudorandom order. Mean BP and vector strength were
calculated from the coarse ITD functions using a modification of the
method of Goldberg and Brown (1969) in which the coarse ITD function
was treated like a period histogram and the strength of locking to the
IPD was measured.

View larger version (34K):
[in this window]
[in a new window]
|
Figure 1.
Illustration of ROC analysis.
A, Tone delay function using coarse steps ( ) and fine
steps ( ). B, Segment of fine-step tone delay function
(joined circles) with distribution of number of
times each spike count occurred superimposed. An example reference
( 0.02 cycles) and target ( 0.00 cycles) ITD are
circled and illustrated with arrows.
C, Distributions for example reference and target ITDs
replotted. D, "Neurometric" function showing
predicted percentage correct in a simulated 2IFC experiment (see
Materials and Methods, ROC analysis, for details). The circled
point shows the percentage correct for the example target ITD
of 0.0 cycles. E, ITD jnd as reference ITD is varied.
The circled point shows the example reference ITD of
0.02 cycles.
|
|
Receiver operating characteristic (ROC) analysis (Green and
Swets, 1974 ; Cohn et al., 1975 ; Bradley et al., 1987 ) was used to
determine the smallest change in ITD (jnd) that the cell could correctly indicate by a change in its firing rate. Although ROC analysis is well know in auditory psychophysics and has been used frequently in visual neurophysiology, it is less common in auditory neurophysiology; therefore we will explain the method in detail.
A distribution of the number of times each spike count occurred
during 100 repeats was constructed for every ITD (Fig.
1B,C). The distributions for
adjacent ITDs overlap considerably, so a given spike count does not
unambiguously indicate the ITD of the signal. To perform ROC analysis,
we first choose a reference ITD (Fig. 1B,
arrow, C, bottom panel) and
calculated the percentage of trials on which we could correctly
discriminate a target ITD from it on the basis of an increase in spike
count (the procedure for calculating percentage correct will be
described below). A single target is shown in Figure 1, B
(arrow) and C (top panel); however, all points in the ITD curve, on either side of the reference, are potential targets. For a given reference ITD (Fig.
1D, 0.02 cycles), a neurometric function can be
constructed using Equation 3, showing the percentage correct for all
possible targets. The circled point shows the percentage
correct for the target and reference illustrated in Figure 1,
B and C. For that reference ITD, the jnd for 75%
correct was determined from the function by interpolation. The process
was then repeated for all possible reference ITDs (Fig.
1E, showing the reference illustrated in Fig.
1B,C circled). From
these curves we determine the lowest jnd obtained (best jnd) and that
obtained with a zero ITD reference (midline jnd). In all figures in
this paper the magnitude of the jnd is plotted; that is, we ignore the
relative ITDs of the target and reference.
The argument above describes looking for a target that can be
discriminated from the reference based on an increase in the spike
count. There are also targets (with more negative ITDs than the
reference in Fig. 1B) that could be discriminated
from the reference on the basis of a decrease in spike count. We show
below that recalculating the ROC analysis on the basis of looking for a
decrease in spike count is not necessary; using 25% correct as the
threshold is entirely equivalent, as might be anticipated from looking
at Figure 1D.
We will now describe how we calculated the percentage correct values
shown in Figure 1D. The most common psychophysical
method used to measure discrimination is the two-interval forced choice (2IFC) method, in which the subject is presented with the target in one
interval and the reference in a second interval in random order and has
to identify the interval containing the target. Performance in such a
task (measured as the percentage of correct decisions) is equal to the
area under the ROC curve (Green and Swets, 1974 ). Rather than
explicitly plot ROC curves and calculate the area under them, we
directly calculated the percentage correct using a method derived from
consideration of the 2IFC task. It can easily be shown that this is
exactly the same as computing the area under the ROC curve. In a 2IFC
task, presentation of the target and reference stimuli elicits two
firing counts. The task is then to chose which interval the target
occurred in, on the basis of these firing counts. The optimum strategy
is to choose the interval with the higher firing count as the target
interval. On the basis of the distributions illustrated in Figure 1,
B and C, we can calculate the percentage of
trials on which this strategy will yield the correct decision. If the
firing count elicited by the reference stimulus is k, then
the correct decision will be reached if the spike count elicited by the
target stimulus is more than k. In other words, the
probability of being correct and the reference stimulus eliciting
k spikes is:
|
(1)
|
where P(lr = k) is the probability of k spikes being elicited
by the reference stimulus, and
P(lr k) is
the probability of k or more spikes being elicited by the
target stimulus. An equal number of spikes can be elicited, of course,
by both the reference and target stimuli; in this situation it is
assumed that an unbiased guess is made, resulting in the
P(lr = k)/2
term. Over the course of an experiment, many different spike counts will be elicited by the target stimulus, so the expected probability of
a correct response (or the probability of being correct over an
infinitely long experiment) for target t (on the basis of an increase in spikes) is given by summing over all possible spike counts:
|
(2)
|
Introducing the notation
f(k|t) for the spike count
distribution elicited by the target stimulus and
f(k|r) for the spike count
distribution elicited by the reference stimulus, and then substituting
Equation 1 into Equation 2 gives:
|
(3)
|
where nr and
nt are the number of repeats used to
generate the reference and target distributions (100 for both in this paper).
Study of Figure 1 will show that reliable performance would also be
obtained if the decision rule was to choose the target on the basis
that it would elicit fewer spikes than the reference. In this case the
correctly chosen targets will be on the opposite side of the reference
ITD. Equation 3 would then become:
|
(4)
|
However, because the terms in square brackets in Equations 3 and
4 are complements of each other, i.e.:
|
(5)
|
Equation 4 becomes:
|
(6)
|
which can be rewritten as:
|
(7)
|
because
In other words, the mathematics is symmetrical, and the 25% jnd
determined from Equation 3 (looking for an increase in firing rate) is
equivalent to the 75% jnd determined from Equation 4 (looking for a
decrease in firing rate). In the rest of the paper we will use the 25%
jnd from Equation 3 when discussing discrimination attributable to a
decrease in firing rate.
 |
Results |
The distribution of unit ITD jnds as a function of signal
frequency when using the reference ITD yielding the lowest jnd is shown
in Figure 2. For most units the signal
frequency was the same as the unit BF; however, for three units with
BFs between 1 and 2 kHz a lower frequency was used. The ITD jnd
decreases as signal frequency increases, with a possible increase above 850 Hz. It should be noted that we often did not proceed with a full
analysis for many units of 900 Hz and above, because the ITD function
was poorly modulated, and hence the ITD jnd would have been
unmeasurably large. Therefore, there is an implicit increase in ITD jnd
somewhere close to the maximum frequency shown. Both of these features
are consistent with the human psychophysical data. The lowest ITD jnd
found, at 600 Hz, was 33 µsec, comparable with the human
psychophysical jnd at 500 Hz and 50 msec duration of 23 µsec (Hafter
et al., 1979 ). Figure 2 has logarithmic axes for both ITD jnd and
signal frequency, so any power law should be a straight line. The line
shown is a least-squares best fit to a power law for frequencies up to
850 Hz, with a power of 0.98 (r2 = 0.50). This is a very
good fit to a 1/f law, which implies that IC neurons are
sensitive to a constant change in interaural phase difference. There is
a fuller discussion of this in Skottun et al. (2001) .

View larger version (17K):
[in this window]
[in a new window]
|
Figure 2.
ITD jnds using reference point chosen to yield
best jnd. A, Characterized according to PSTH
classification type (see Materials and Methods). Line is
a power-regression fit to data below 850 Hz. There is one point per
unit because PSTHs could be obtained from the data obtained in
collecting ITD curves even if no other data were available.
B, Characterized according to response area type (see
Materials and Methods). Response areas were not always collected
because of the premature loss of the unit, so there are fewer points
than in A.
|
|
The temporal response classification of each unit (Le Beau et al.,
1996 ) is shown using different symbols in Figure 2A.
There is an even spread of response types across frequency and ITD jnd, showing, perhaps surprisingly, that the ITD jnd is not influenced by
the temporal response type. Similarly, the classification according to
response area type (Ramachandran et al., 1999 ) is also not predictive
of ITD jnd (Fig. 2B).
To determine the optimum performance for each unit, we selected the
reference ITD to give the lowest ITD jnd, which we call the "best
jnd." However, most psychophysics is done using a midline reference
(zero ITD), so it is important to see how using a midline reference
affects the ITD jnds. ITD jnds calculated using a midline reference are
termed "midline jnds" and are shown by large symbols in Figure
3; these are linked by a line
to the corresponding best jnds shown by small dots. The
sloping portion of the ITD function is usually centered on midline, so
a midline jnd can often be obtained by looking for either an increase
or a decrease in firing rate. These jnds may be different, because both
the slope of the ITD curve and the variances may be different on either
side of the reference ITD. Jnds obtained by looking for either an
increase or a decrease in firing rate are equivalent to those obtained choosing thresholds of 75 or 25% correct, respectively, on neurometric curves like those in Figure 1D. Both of these midline
jnds were calculated, and the better one is plotted in Figure 3, with
jnds obtained by using an increase in firing rate (75% correct) shown by filled symbols and jnds obtained by using a decrease in
firing rate (25% correct) shown by open symbols. The
midline jnds are larger than the best jnds, which is expected by
definition, as shown in Figure 3B comparing the midline jnd
on the ordinate against the best jnd on the abscissa. The difference
between these jnds can be very large; however, some midline jnds can
still be as low as the best jnds, so conclusions about the relationship
between human psychophysical performance and neural jnds are unaffected by the choice of reference. It is also interesting that although the
midline jnds could occur with either increasing firing rate (toward the
peak) or decreasing firing rate (toward the trough) with no a priori
reason for choosing one over the other, most of the midline jnds that
are shown result from a decrease in firing rate.

View larger version (17K):
[in this window]
[in a new window]
|
Figure 3.
A, ITD jnds using midline reference
point (zero ITD). Solid, upward triangles
indicate an increase in firing rate (i.e., 75% correct).
Open, downward triangles indicate a
decrease in firing rate (i.e., 25% correct). Small,
filled circles are ITD jnds using the reference point
chosen to yield best jnd, joined to the corresponding midline jnds by
lines. B, Comparison of ITD jnds obtained
using reference point giving best jnd (abscissa) and
those obtained using midline reference point (zero ITD:
ordinate). The diagonal line marks
equality between jnds.
|
|
A comparison of the position of the reference ITD giving rise to the
best jnd for increasing firing rate is shown in Figure 4 for each unit. Figure
4A shows the fine ITD curves for all units plotted
over each other after normalizing. The position of the reference point
for the best jnd is shown on each curve by a filled circle.
Four units had ipsilateral peaks and slope the opposite way from the
other curves. Most of the reference points are close to the minimum in
the ITD function (just at the "knee-point" where the
slope is about to reach its maximum). This results in most of the
reference points having ITDs with ipsilateral leading. The positions of
the reference points as a function of frequency are shown in Figure
4B, with the reference points for curves with ipsilateral peaks shown as open circles. This emphasizes
that most of the reference points are at negative ITDs (ipsilateral leading), whereas the peaks of the ITD functions are on the
contralateral side (compare Fig. 7C).

View larger version (30K):
[in this window]
[in a new window]
|
Figure 4.
A, Fine ITD curves for all units
plotted over each other after normalizing by subtracting off the
minimum rate and dividing by the resulting maximum. The position of the
reference point for the best jnd is shown on each curve by a
filled circle. Four units had ipsilateral peaks and
slope the opposite way to the other curves. B, Positions
of the reference points. Points from units where the peak of the ITD
curve was contralateral are shown as filled circles, and
where the peak was ipsilateral they are shown as open
circles.
|
|
We investigated the effect of increasing stimulus duration in 16 units,
where stability was excellent. This increased the recording time from
just under 1 hr to several hours so it was not attempted often.
Duration was increased from 50 to 400 msec, and a ratio of on to off
duration of 1:3 was maintained; i.e., the longest stimuli were repeated
every 1600 msec. The results are shown in Figure
5, classified according to the unit
temporal response type (Le Beau et al., 1996 ). Sustained (two of two)
(Fig. 5A) and many on-sustained (six of nine) (Fig.
5B) units showed an improvement in ITD jnd with increasing
signal duration that was less than optimal (log/log slope of 0.5) but
comparable with humans (log/log slope of 0.2 shown as dotted
line in Fig. 5A). However, some of the on-sustained
(three of nine) (Fig. 5B) and all of the pauser (two of two)
(Fig. 5C) and broad-onset (three of three) (Fig.
5D) units showed poorer ITD jnds as signal duration increased. The decline in performance was caused both by an increase in
the variance of spike counts and by a decrease in the peak-to-trough modulation depth of the ITD function; however, we have no clear explanation for why this occurred.

View larger version (26K):
[in this window]
[in a new window]
|
Figure 5.
ITD jnds as a function of tone duration classified
according to PSTH type (see Materials and Methods). A,
Sustained units; B, on-sustained units;
C, pauser units; D, broad-onset units.
Dashed line in A has a slope of 0.2,
which corresponds to human psychophysics. Different symbols
indicate different units.
|
|
For 19 units we obtained ITD jnds using sound levels of 20 and 40 dB
above unit-rate threshold. A comparison of the ITD jnds obtained is
shown in Figure 6. In all except three
units, the 40 dB jnd is larger than the 20 dB jnd. In human
psychophysics (Hershkowitz and Durlach, 1969 ) the ITD jnd improves
significantly up to 20 dB above detection threshold, improves slightly
up to 40 dB above detection threshold, and is maintained above that, so
these results are slightly surprising. However, they are easily explainable in terms of the rate-level function of the units. Three
units had a lower ITD jnd at 40 dB than at 20 dB; these had a
monotonically increasing firing rate, which was still increasing between 20 and 40 dB. Of the eight units in which the ITD jnd at 40 dB
was >20% greater than the ITD jnd at 20 dB, but still measurable, six
had saturated at the best ITD, but the firing rate increased at the
worst ITD. In other words, the trough of the ITD function was filling
in, and the modulation of the ITD function consequently decreased. The
other two units were nonmonotonic, so the peak of the ITD function was
reduced, thus reducing the modulation of the ITD function. Of the five
units in which the ITD jnd became immeasurably large at 40 dB, four had
severely nonmonotonic rate-level functions so that the units did not
fire at all at the higher level. The other unit had saturated at the best ITD, but the firing rate increased greatly at the worst ITD, leading to a severely reduced modulation of the ITD function.

View larger version (13K):
[in this window]
[in a new window]
|
Figure 6.
Comparison of ITD jnds at different signals
levels, either 20 dB ( ) or 40 dB ( ) above unit pure-tone rate
threshold. For five units, the ITD jnd was too large to be determined
at 40 dB, so they are shown at the top of the plot
(there are two units at 615 Hz, shown displaced by ±5 Hz).
|
|
We determined mean best phase and vector strength from the coarse
ITD functions using the method of Goldberg and Brown (1969) by treating
the ITD function as a periodic function and converting the ITD to IPD.
We also measured the response to binaural beats (at 1 Hz) for many of
these neurons and also calculated the mean best phase and vector
strength for locking to the beat frequency. The agreement between best
phase determined from binaural beats and static tone bursts is shown in
Figure 7A and is excellent, with a Pearson correlation coefficient of 0.78. The agreement between
vector strengths is less good (Fig. 7B), with a correlation of 0.58. If only the units classified as sustained (15 of 35) or
on-sustained (12 of 35) according to the unit temporal response type
(Le Beau et al., 1996 ) were included in the analysis, then the vector
strength correlation increased to 0.75 and 0.60, respectively. Units
that responded throughout a stimulus, but only after a pause (i.e.,
pauser types: 5 of 35), gave a lower vector strength correlation of
0.27. Units that responded only at the stimulus onset or offset (onset,
broad-onset, and offset types) did not respond sufficiently well to the
binaural beat to yield a best phase estimate, so they were not included
in the analysis. Since the pioneering work of Yin and Kuwada (Kuwada
and Yin, 1983 ; Yin and Kuwada, 1983a ,b ; Kuwada et al., 1984 ), binaural
beats have been used routinely to measure ITD sensitivity. These data
provide additional confirmation of Yin and Kuwada's findings that this
is a valid technique at the level of the IC; however, it does reduce
the population of neurons from which binaural best phase can be
estimated and has well documented problems with adaptation (Spitzer and
Semple, 1993 ; McAlpine et al., 2000 ).

View larger version (32K):
[in this window]
[in a new window]
|
Figure 7.
A, Comparison of best phase
obtained from static tone delay functions (abscissa) and
1 Hz binaural beats (ordinate). B,
Comparison of vector strength obtained from static tone delay functions
(abscissa) and 1 Hz binaural beats
(ordinate). C, Best phase obtained from
tone delay curves as a function of signal frequency. The solid
line shows the linear regression fit to the data. The
dotted line shows a linear regression fitted to the data
obtained from noise delay curves by McAlpine et al. (2001) .
Symbols indicate PSTH classification; see Figure
2A for key.
|
|
Tone best phase tends to increase with frequency (Fig.
7C). The linear regression fitted to these data has a slope
of 0.109 cycles per kilohertz and an intercept of 0.08 cycles (Fig.
7C, solid line). Comparable data derived from
noise delay curves were reported by McAlpine et al. (2001) ; their fit
is shown in Figure 7C (dashed line).
Although it might be expected that those units that show the most
highly modulated ITD functions would give the lowest ITD jnds, this is
not the case. Even when the ITD functions are normalized by subtracting
out the baseline rate, there is still no relationship between vector
strength and ITD jnd. This is because the jnd is determined primarily
by the ratio of the slope of the ITD function to the variance of the
firing rate distribution, and the slope of the ITD function is
dependent on the stimulus frequency.
Throughout this paper we have shown ITD jnds derived from a ROC
analysis. This is computationally more intensive than the alternatives
but has the major theoretical advantage of making no assumptions about
the underlying spike-rate distributions. The most commonly used measure
of discrimination is d', which assumes that the spike-rate
distributions of the target and reference are both Gaussian and have
the same variance. Although neither of these assumptions is true,
d' analysis has the major advantage of computational
simplicity; only the means and variances of the spike rates need to be
computed. In Figure 8 we compare the ITD jnds obtained using both ROC and the standard separation, D,
which is a form of d' in the unequal variance case, obtained
by computing the ratio of the difference in mean firing rate divided by
the geometric mean of the SDs (Sakitt, 1973 ; Jiang et al., 1997a ). There is a great deal of similarity between the measures (Pearson correlation = 0.986), with the standard separation analysis
tending to overestimate the jnds slightly. This similarity is
emphasized by the regression line (Fig. 8B,
solid line) virtually overlying the line of equality (Fig.
8B, dashed line). This suggests that it
may be possible to use d' or the standard separation,
D, as a simple way to obtain a quite close approximate
estimate of ITD discrimination thresholds of single neurons. To what
extent this also applies to stimulus dimensions other then ITD and to
sense modalities other than hearing remains to be determined. For this data set, at least, the use of the standard separation, D,
would not have significantly biased the results. However, because ROC analysis makes fewer assumptions about the underlying spike-rate distributions, it remains the best method when they are unknown. To use
d' (or standard separation) without first testing the
spike-rate distributions could introduce biases, so to check that there
is no bias the spike-rate distributions for at least a few units would
need to be measured and checked for normality.

View larger version (15K):
[in this window]
[in a new window]
|
Figure 8.
Comparison of ITD jnds obtained from full ROC
analysis or by standard separation (D) analysis.
A, ITD jnds as a function of signal frequency.
B, Scattergram plot of standard separation
(D) jnds (ordinate) and ROC jnds
(abscissa). Dashed diagonal line marks
equality; solid diagonal line is linear regression fit
to the data.
|
|
 |
Discussion |
In a previous paper (Skottun et al., 2001 ), we showed the
basic result illustrated in Figure 2A, without the
classification according to PSTH type or response area. We argued that
the approach of the lowest jnds to those of human observers was
evidence for the sensitivity of single neurons being able to account
for human psychophysical jnds. In that paper we discuss the problem of
across-species comparison, so we will not pursue that further here. A
criticism that could be leveled against that paper is that we compared
human psychophysical jnds based on a midline reference with neural jnds based on a reference chosen to give the lowest possible jnd (best jnd).
In the current paper, we also compute ITD jnds with a midline reference
(Fig. 3A), so a comparison of best jnds (Fig.
2A) with midline jnds is possible (Fig.
3B). Although for many units midline jnds are higher than
the corresponding best jnd, there are many units for which the midline
jnds are just as low. The conclusion that single-cell jnds are
comparable with human performance still holds.
Fitzpatrick et al. (1997) have argued that the outputs of ~40
neurons are needed to give discrimination jnds of 16 µsec, on the
basis of an analysis of composite ITD curves (which are normally viewed
as predictive of noise delay curves). We claim that individual neurons
can yield tone discrimination jnds of 30 µsec; however, this does not
imply any disagreement about the underlying data but is merely a
different way of looking at the results. Fitzpatrick et al. (1997)
based their findings on a derivative of the Jeffress delay-line model
(Jeffress, 1948 ) in which they were trying to detect the change in the
location of the peak of activity along an ITD ordered line of cells.
Instead, we were looking for changes in the firing rate of isolated
individual neurons. Looking for shifts in a peak involves looking for a
change where the slope of the ITD functions are at their minimum and
the variability in the firing rate is at a maximum. This is the least
favorable situation for obtaining low jnds, so pooling is required to
obtain low jnds. We, on the other hand, were using a method that
selected the region of the ITD curve where there was maximal
discrimination information. This yielded jnds that were much lower and
suggests that single neurons carry enough information to allow
discrimination comparable with human psychophysics; however, this does
not imply that only a single neuron is used for discrimination. To do
so would require previous information about which neuron to use, because in a random field some neurons would show increasing firing rates and some decreasing firing rates in response to the same stimuli.
Our results are consistent with the Jeffress delay-line model in which
discrimination is performed at the edge of the region of peak activity,
a suggestion that has a long history and has been given recent impetus
by the findings of McAlpine et al. (2001) followed by Brand et al.
(2002) , showing that the peaks of ITD functions are often outside the
physiological range and the maximal slopes are around midline. Here,
the maximal change will be isolated to a few neurons at most, and the
identity of the relevant neurons will be signaled by them being at the
edge of the distribution. In other words, these results do not prove that single cells are used for ITD discrimination but just that they
carry enough information for them to allow this if they can be suitably
identified. It should also be noted that the use of an array of several
cells with different ITD tunings in concert to perform ITD
discrimination is not the same as pooling (which requires the addition
of the output of many cells with the same tuning to average out
uncorrelated noise). The core finding of this study is that any
pooling, or comparison of activity across a population, is performed
for reasons other than reducing noise to improve discrimination
performance. One possible reason for such a comparison across the
population is that there are many factors that can change the firing
rate of an individual neuron, such a stimulus level and frequency, as
well as stimulus ITD, so a change in firing rate of an individual
neuron is ambiguous about what it is signaling. However, a comparison
across several cells with similar frequency and level sensitivities
would reduce this ambiguity.
The best reference points for increasing firing rates tend to be
on the ipsilateral side (Fig. 4). This is despite the fact that peaks
of most of the ITD functions are on the contralateral side (Fig.
7C). McAlpine et al. (2001) followed by Brand et al. (2002)
have argued that there is selective pressure favoring placing the
maximum slopes of ITD functions across the midline, so the peaks are
pushed into contralateral space and are best-frequency dependent. We
also found the same relationship of peak position with best frequency
(Fig. 7C). That the best reference points are on the
ipsilateral side is consistent with the maximum slope being near
midline, because the reference points tended to be slightly toward the
minimum of the ITD function relative to the maximum slope (Fig. 4). It
is also probably of significance to theories of lateralization
discrimination that the better midline jnds were obtained with
decreasing spike rates. Cross-correlation-based models of the binaural
masking level difference (e.g., Colburn, 1977 ), supported by physiology
(Jiang et al., 1997a ,b ; Palmer et al., 1999 ), are also dependent on a
decrease in firing rate to indicate the presence of a signal in
interaurally in-phase noise.
Although the lowest single unit jnds are in line with human
psychophysics, the effects of duration and signal level are not so
clear cut. Psychophysical pure tone jnds either remain constant as
duration increases (Yost, 1977 ) or improve slowly with duration with a
log-log slope of 0.2 (Ricard and Hafter, 1973 ; Hafter et al., 1979 ),
which is less than the theoretical optimal improvement assuming
independent sampling as a function of duration (a log-log slope of
0.5) (Houtgast and Plomp, 1968 ). All of the sustained units and many of
the on-sustained units showed an improvement comparable with humans
(Fig. 5A,B), but all of the other
units showed poorer ITD jnds as duration increased. No onset units were tested with a duration sequence for obvious reasons. Thus, to match
human psychophysical results, a mechanism for selectively listening to
units with a sustained discharge is necessary. To some extent, the
units would be self selecting, because the sustained and on-sustained
units fire better throughout the stimulus than the other types, but
pausers also fire somewhat throughout the longer stimuli, and those
on-sustained units that get worse with increasing duration need to be
selected out.
The effect of signal level is somewhat more problematic. In human
psychophysics (e.g., Hershkowitz and Durlach, 1969 ), the ITD jnd
improves significantly up to 20 dB above detection threshold, improves
slightly up to 40 dB above detection threshold, and is maintained above
that. Most units, however, show a worsening of ITD jnd between 20 and
40 dB above unit threshold (Fig. 6). Although our results can be
explained in terms of the units' rate-level functions, they pose a
problem in accounting for the maintenance of the small human
psychophysical ITD jnd above 40 dB above detection threshold. Some of
the paradox can be explained away by remembering that there is a range
of unit rate-level thresholds, so it is possible that some neurons will
be within 20 dB of threshold even at the highest levels (75 dB above
detection threshold) tested by Hershkowitz and Durlach (1969) .
In summary, we have shown that there is sufficient information in
the firing rates of individual IC neurons to produce ITD jnds that are
comparable with those of humans psychophysically. Although there is
enough information, it is unlikely that individual neurons are
responsible for the whole animal behavioral response for various
reasons, not the least because of the problem of determining which
neuron to attend to and the ambiguity inherent in many factors other
than ITD affecting the firing rate of an individual neuron. What these
results do show is that the common assumption that there must be
pooling across cells to allow human psychophysical ITD jnds to be
achieved is not true and that any pooling or comparison of activity
across a population is performed for reasons other than reducing noise
to improve discrimination performance.
 |
FOOTNOTES |
Received Aug. 12, 2002; revised Oct. 15, 2002; accepted Nov. 1, 2002.
Correspondence should be addressed to Dr. Trevor M. Shackleton, Medical
Research Council Institute of Hearing Research, University Park,
Nottingham, NG7 2RD, UK. E-mail:
trevor{at}ihr.mrc.ac.uk.
 |
References |
-
Batra R,
Kuwada S,
Fitzpatrick DC
(1997a)
Sensitivity to interaural temporal disparities of low- and high-frequency neurons in the superior olivary complex. I. Heterogeneity of responses.
J Neurophysiol
73:1222-1236.
-
Batra R,
Kuwada S,
Fitzpatrick DC
(1997b)
Sensitivity to interaural temporal disparitites of low- and high-frequency neurons in the superior olivary complex. II. Coincidence detection.
J Neurophysiol
78:1237-1247[Abstract/Free Full Text].
-
Bradley A,
Skottun BC,
Ohzawa I,
Sclar G,
Freeman RD
(1985)
A neurophysiological evaluation of the differential response model for orientation and spatial-frequency discrimination.
J Opt Soc Am [A]
2:1607-1610[ISI][Medline].
-
Bradley A,
Skottun BC,
Ohzawa I,
Sclar G,
Freeman RD
(1987)
Visual orientation and spatial frequency discrimination: a comparison of single neurons and behavior.
J Neurophysiol
57:755-772[Abstract/Free Full Text].
-
Brand A,
Behrend O,
Marquardt T,
McAlpine D,
Grothe B
(2002)
Precise inhibition is essential for microsecond interaural time difference coding.
Nature
417:543-547[Medline].
-
Bullock DC,
Palmer AR,
Rees A
(1988)
Compact and easy-to-use tungsten-in-glass microelectrode manufacturing workstation.
Med Biol Eng Comput
26:669-672[ISI][Medline].
-
Carr CE
(1993)
Processing of temporal information in the brain.
Annu Rev Neurosci
16:223-243[ISI][Medline].
-
Cohn TE,
Green DG,
Tanner WP
(1975)
Receiver operating characteristic analysis. Application to the study of quantum fluctuation effects in optic nerve of rana pipiens.
J Gen Physiol
66:583-616[Abstract/Free Full Text].
-
Colburn HS
(1977)
Theory of binaural interaction based on auditory-nerve data. II. Detection of tones in noise.
J Acoust Soc Am
61:525-533[ISI][Medline].
-
Durlach NI,
Colburn HS
(1978)
Binaural phenomena.
In: Handbook of perception, Vol IV, hearing (Carterette EC,
Friedman MP,
eds), pp 365-466. New York: Academic.
-
Fay RR,
Coombs SL
(1992)
Psychometric functions for level discrimination and the effects of signal duration in the goldfish (carassius-auratus)
psychophysics and neurophysiology.
J Acoust Soc Am
92:189-201[Medline]. -
Fitzpatrick DC,
Batra R,
Stanford TR,
Kuwada S
(1997)
A neuronal population code for sound localization.
Nature
388:871-874[Medline].
-
Gerstner W,
Kempter R,
van Hemmen JL,
Wagner H
(1996)
A neuronal learning rule for sub-millisecond temporal coding.
Nature
383:76-78[Medline].
-
Goldberg JM,
Brown PB
(1969)
Response of binaural neurons of dog superior olivary complex to dichotic tonal stimuli: some physiological mechanisms of sound localization.
J Neurophysiol
32:613-636[Free Full Text].
-
Green DM,
Swets JA
(1974)
In: Signal detection theory and psychophysics. Huntington, NY: Krieger.
-
Hafter ER,
Dye RH,
Gilkey RH
(1979)
Lateralization of tonal signals which have neither onsets nor offsets.
J Acoust Soc Am
65:471-477[ISI][Medline].
-
Hall JL
(1965)
Binaural interaction in the acessory superior-olivary nucleus of the cat.
J Acoust Soc Am
37:814-823.
-
Hawken MJ,
Parker AJ
(1990)
Detection and discrimination mechanisms in the striate cortex of the old-world monkey.
In: Vision: Coding and efficiency (Blakemore C,
ed), pp 103-116. Cambridge, UK: Cambridge UP.
-
Hershkowitz RM,
Durlach NI
(1969)
Interaural time and amplitude jnds for a 500-Hz tone.
J Acoust Soc Am
46:1464-1467[Medline].
-
Houtgast T,
Plomp R
(1968)
Lateralization threshold of a signal in noise.
J Acoust Soc Am
44:807-812[Medline].
-
Jeffress LA
(1948)
A place theory of sound localization.
J Comp Psychol
44:35-39.
-
Jiang D,
McAlpine D,
Palmer AR
(1997a)
Detectability index measures of binaural masking level difference across populations of inferior colliculus neurons.
J Neurosci
17:9331-9339[Abstract/Free Full Text].
-
Jiang D,
McAlpine D,
Palmer AR
(1997b)
Responses of neurones in the guinea pig inferior colliculus to binaural masking level difference stimuli measured by rate-versus-level functions.
J Neurophysiol
77:3085-3106[Abstract/Free Full Text].
-
Johansson RS,
Vallbo ÅB
(1979)
Detection of tactile stimuli. Thresholds of afferent units related to psychophysical thresholds in the human hand.
J Physiol (Lond)
297:405-422[Abstract/Free Full Text].
-
Kuwada S,
Yin TCT
(1983)
Binaural interaction in low-frequency neurons in inferior colliculus of the cat. I. Effects of long interaural delays, intensity, and repetition rate on interaural delay function.
J Neurophysiol
50:981-999[Abstract/Free Full Text].
-
Kuwada S,
Yin TCT,
Syka J,
Buunen TJF,
Wickesberg RE
(1984)
Binaural interaction in low-frequency neurons in inferior colliculus of the cat. IV. Comparison of monaural and binaural response properties.
J Neurophysiol
51:1306-1325[Abstract/Free Full Text].
-
Le Beau FEN,
Rees A,
Malmierca MS
(1996)
Contribution of GABA- and glycine-mediated inhibition to the monaural temporal response properties of neurons in the inferior colliculus.
J Neurophysiol
75:902-919[Abstract/Free Full Text].
-
McAlpine D,
Jiang D,
Shackleton TM,
Palmer AR
(1998)
Convergent input from brainstem coincidence detectors onto delay-sensitive neurons in the inferior colliculus.
J Neurosci
18:6026-6039[Abstract/Free Full Text].
-
McAlpine D,
Jiang D,
Shackleton TM,
Palmer AR
(2000)
Responses of neurons in the inferior colliculus to dynamic interaural phase cues: evidence for a mechanism of binaural adaptation.
J Neurophysiol
83:1356-1365[Abstract/Free Full Text].
-
McAlpine D,
Jiang D,
Palmer AR
(2001)
A neural code for low-frequency sound localisation in mammals.
Nat Neurosci
4:396-401[ISI][Medline].
-
Mills AW
(1958)
On the minimum audible angle.
J Acoust Soc Am
30:237-246.
-
Newsome WT,
Britten KH,
Movshon JA
(1989)
Neuronal correlates of a perceptual decision.
Nature
341:52-54[Medline].
-
Palmer AR,
Jiang D,
McAlpine D
(1999)
Desynchronizing responses to correlated noise: a mechanism for binaural masking levels differences at the inferior colliculus.
J Neurophysiol
81:722-734[Abstract/Free Full Text].
-
Parker AJ,
Hawken MJ
(1985)
Capabilities of monkey cortical cells in spatial-resolution tasks.
J Opt Soc Am [A]
2:1101-1114[ISI][Medline].
-
Ramachandran R,
Davis KA,
May BJ
(1999)
Single-unit responses in the inferior colliculus of decerebrate cats I. Classification based on frequency response maps.
J Neurophysiol
82:152-163[Abstract/Free Full Text].
-
Relkin EM,
Pelli DG
(1987)
Probe tone thresholds in the auditory nerve measured by two-interval forced-choice procedures.
J Acoust Soc Am
82:1679-1691[ISI][Medline].
-
Relkin EM,
Turner CW
(1988)
A reexamination of forward masking in the auditory nerve.
J Acoust Soc Am
84:584-591[ISI][Medline].
-
Ricard GC,
Hafter ER
(1973)
Detection of interaural time differences in short duration, low frequency tones.
J Acoust Soc Am
53:335.
-
Sakitt B
(1973)
Indices of discriminability.
Nature
241:133-134[Medline].
-
Skottun BC
(1998)
Sound localization and neurons.
Nature
393:531[Medline].
-
Skottun BC,
Shackleton TM,
Arnott RH,
Palmer AR
(2001)
The ability of inferior colliculus neurons to signal differences in interaural delay.
Proc Natl Acad Sci USA
98:14050-14054[Abstract/Free Full Text].
-
Spitzer MW,
Semple MN
(1993)
Responses of inferior colliculus neurones to time-varying interaural phase disparity: effects of shifting the locus of virtual motion.
J Neurophysiol
69:1245-1263[Abstract/Free Full Text].
-
Spitzer MW,
Semple MN
(1995)
Neurons sensitive to interaural phase disparity in gerbil superior olive: diverse monaural and temporal response properties.
J Neurophysiol
73:1668-1690[Abstract/Free Full Text].
-
Stanford TR,
Kuwada S,
Batra R
(1992)
A comparison of the interaural time sensitivity of neurons in the inferior colliculus and thalamus of the unanesthetized rabbit.
J Neurosci
12:3200-3216[Abstract].
-
Vallbo ÅB
(1995)
Single-afferent neurons and somatic sensation in humans.
In: The cognitive neurosciences (Gazzaniga MS,
ed), pp 237-252. Cambridge, MA: MIT.
-
Yin TCT,
Chan JCK
(1988)
Neural mechanisms underlying interaural time sensitivity to tones and noise.
In: Auditory function: neurobiological bases of hearing (Edelman GM,
Gall WE,
Cowan WM,
eds), pp 385-430. New York: Wiley.
-
Yin TCT,
Chan JCK
(1990)
Interaural time sensitivity in medial superior olive of cat.
J Neurophysiol
64:465-488[Abstract/Free Full Text].
-
Yin TCT,
Kuwada S
(1983a)
Binaural interaction in low-frequency neurons in inferior colliculus of the cat. II. Effects of changing rate and direction of interaural phase.
J Neurophysiol
50:1000-1019[Abstract/Free Full Text].
-
Yin TCT,
Kuwada S
(1983b)
Binaural interaction in low-frequency neurons in inferior colliculus of the cat. III. Effects of changing frequency.
J Neurophysiol
50:1020-1042[Abstract/Free Full Text].
-
Yin TCT,
Joris PX,
Smith PH,
Chan JCK
(1997)
Neuronal processing for coding interaural time disparities.
In: Binaural and spatial hearing in real and virtual environments (Gilkey RH,
Anderson TR,
eds), pp 427-445. Mahwah, NJ: Erlbaum.
-
Yost WA
(1977)
Lateralization of pulsed sinusoids based on interaural onset, ongoing, and offset temporal differences.
J Acoust Soc Am
61:190-194[Medline].
-
Young ED,
Barta PE
(1986)
Rate responses of auditory nerve fibers to tones in noise near masked threshold.
J Acoust Soc Am
79:426-442[ISI][Medline].
Copyright © 2003 Society for Neuroscience 0270-6474/03/232716-09$05.00/0
This article has been cited by other articles:

|
 |

|
 |
 
D. J. Tollin, K. Koka, and J. J. Tsai
Interaural Level Difference Discrimination Thresholds for Single Neurons in the Lateral Superior Olive
J. Neurosci.,
May 7, 2008;
28(19):
4848 - 4860.
[Abstract]
[Full Text]
[PDF]
|
 |
|

|
 |

|
 |
 
Z. M. Smith and B. Delgutte
Sensitivity of Inferior Colliculus Neurons to Interaural Time Differences in the Envelope Versus the Fine Structure With Bilateral Cochlear Implants
J Neurophysiol,
May 1, 2008;
99(5):
2390 - 2407.
[Abstract]
[Full Text]
[PDF]
|
 |
|

|
 |

|
 |
 
Z. M. Smith and B. Delgutte
Sensitivity to Interaural Time Differences in the Inferior Colliculus with Bilateral Cochlear Implants
J. Neurosci.,
June 20, 2007;
27(25):
6740 - 6750.
[Abstract]
[Full Text]
| |