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The Journal of Neuroscience, February 15, 1999, 19(4):1508-1516
Neural Coding of Sound Frequency by Cricket Auditory
Receptors
Kazuo
Imaizumi and
Gerald S.
Pollack
Department of Biology, McGill University, Montréal, Quebec
H3A 1B1, Canada
 |
ABSTRACT |
Crickets provide a useful model to study neural processing of sound
frequency. Sound frequency is one parameter that crickets use to
discriminate between conspecific signals and sounds made by predators,
yet little is known about how frequency is represented at the level of
auditory receptors. In this paper, we study the physiological
properties of auditory receptor fibers (ARFs) by making single-unit
recordings in the cricket Teleogryllus oceanicus. Characteristic frequencies (CFs) of ARFs are distributed
discontinuously throughout the range of frequencies that we
investigated (2-40 kHz) and appear to be clustered around three
frequency ranges (
5.5, 10-12, and
18 kHz). A striking
characteristic of cricket ARFs is the occurrence of additional
sensitivity peaks at frequencies other than CFs. These additional
sensitivity peaks allow crickets to detect sound over a wide frequency
range, although the CFs of ARFs cover only the frequency bands
mentioned above. To the best of our knowledge, this is the first
example of the extension of an animal's hearing range through multiple
sensitivity peaks of auditory receptors.
Key words:
insect hearing; Teleogryllus oceanicus; frequency sensitivity; sound communication; ultrasound; acoustic
startle response; phonotaxis
 |
INTRODUCTION |
Sound frequency is an important
carrier of information for many animals. The neural analysis of sound
frequency begins with auditory receptor neurons. Understanding how the
population of receptor neurons in an animal's ear represents sound
frequency is required for a more general knowledge of the neural
analysis of acoustic signals. One model system for studying the
neurobiology of acoustic behaviors in general, and the analysis of
sound frequency in particular, is the auditory system of crickets. In
this paper, we describe the frequency sensitivity and selectivity of
auditory receptors in the Australian field cricket Teleogryllus
oceanicus.
Crickets hear sounds ranging in frequency from 2 to at least 100 kHz
(Hoy et al., 1982
), with ~70 auditory receptors in each ear (Young
and Ball, 1974
). Two narrower frequency regions within this wide range
are of particular behavioral relevance. Sound energy in intraspecific
signals is concentrated in relatively narrow spectral bands. In
T. oceanicus, for example, intraspecific songs have dominant
frequencies near 4.5 kHz (Nolen and Hoy, 1986
; Libersat et al., 1994
;
Balakrishnan and Pollack, 1996
). The other class of behaviorally
relevant sounds, the echolocation cries of aerially hunting bats, has
energy in ultrasonic frequencies (Suga, 1990
). Behavioral studies have
shown that crickets have enhanced sensitivity to sounds in these two
frequency ranges (Popov and Shuvalov, 1977
; Moiseff et al., 1978
;
Pollack et al., 1984
; Nolen and Hoy, 1986
). Furthermore, crickets
categorize the entire audible range into low frequencies and
ultrasound, with a sharp boundary at 15 kHz (Wyttenbach et al.,
1996
).
In the past, only a few studies have addressed the physiology of
cricket auditory receptors (Zaretsky and Eibl 1978
; Esch et al., 1980
;
Hutchings and Lewis, 1981
; Oldfield et al., 1986
). Most of these failed
to investigate sensitivity to ultrasound, either because of technical
reasons or because they were performed before the behavioral
significance of ultrasound was appreciated. Moreover, these studies
described responses at threshold sound intensities and thus neglected
the suprathreshold intensities at which most acoustic behaviors occur
(Capranica, 1992
).
In this paper, we address the general physiological properties of
cricket auditory receptors. Our main goal is to explore sensitivity to
different frequencies at suprathreshold intensities and frequency
selectivity at threshold, as well as suprathreshold intensities.
Part of the work has been published previously in preliminary form
(Imaizumi and Pollack, 1996
, 1997
).
 |
MATERIALS AND METHODS |
Animals. Australian field crickets, T. oceanicus, were cultured on a 12 hr dark/light cycle at 25-28°C
in our laboratory colony. They were kept in a crowded population and
fed water and cat chow (Ralston Purina, St. Louis, MO) ad
libitum. Only adult virgin females, 14-23 d after the final molt,
were used.
Recording procedures. Animals were waxed on a platform
ventral side up after removal of the wings, midlegs, and hindlegs. The
femur of each front leg was fixed, with warm wax, perpendicular to the
cricket's longitudinal axis. The tibia was held flexed against the
femur. The prothoracic ganglion, which is where auditory receptors
terminate (Eibl and Huber, 1979
), was exposed by ventral dissection and
kept moist with modified TES ringer (Strausfeld et al., 1983
;
Pollack, 1994
). The ganglion was stabilized by a silver platform, and a
chlorided silver ground wire was placed into the abdomen. Experiments
were performed in a sound-attenuating chamber at 20-23°C.
We used two different recording techniques: whole tympanal nerve (WTN)
and single-unit recordings. The WTN recordings monitored compound
action potentials of a population of auditory receptor fibers (ARFs).
Two Teflon-insulated silver wires (outer diameter, 114 µm), the tips
of which were bare, were inserted into the femur close to the nerve
that carries the axons of ARFs. To eliminate efferent activity from the
recordings, the leg nerve was cut between the coxa and prothoracic
ganglion. Nevertheless, spontaneous activity was not eliminated (see
Fig. 4). Single-unit recordings were made with glass micropipettes,
filled with either 3 M KCl (resistance, 10-40 M
) or
2-4% Lucifer yellow CH (Aldrich, Milwaukee, WI) in distilled water
(resistance, 100-300 M
) in the leg nerve near its entry into the
prothoracic ganglion. The anatomy of axon terminals of ARFs as revealed
by injection of Lucifer yellow is described elsewhere (Imaizumi and
Pollack, 1996
, 1998
).
Acoustic stimulation. Sound stimuli were generated by a
National Instruments (Austin, TX) AT-MIO-64F5 input-output board
(resolution, 12 bits; digital-to-analog update rate, 250 kHz) driven by
software written using LabWindows/CVI (National Instruments).
After power amplification (Amcron) and computer-controlled attenuation
(Mike Walsh Electronics), stimuli were delivered either through 4-inch magnetic speakers (InterTAN, Fort Worth, TX) for lower frequencies (
10 kHz) or through piezoelectric speakers (Matsushita Electric Industrial) for higher frequencies (>10 kHz), ipsilateral to
the recording side. The fundamental frequency was more intense than all
harmonics by at least 45-50 dB. Increments between sound frequencies were 0.5 kHz for stimuli in the range of 2-6 kHz, 1 kHz in the range
of 6-10 kHz, 2 kHz in the range of 10-20 kHz, and 5 kHz in the range
of 20-40 kHz. Sound intensity (re. 20 µPa) was calibrated with a
1/4-inch Brüel & Kjaer 4135 condenser microphone and 2610 measuring amplifier. Sound stimuli were 30 msec in duration (including 5 msec rise and fall times) and were presented at two pulses per second. The search stimulus used was either 4.5 kHz (or 5 kHz) at 80 dB
sound pressure level (SPL) or bandpass filtered white noise
(3-50 kHz) at 90 dB SPL.
Data analysis. Responses were stored on magnetic tape and
were digitized (sampling rate, 10 kHz/channel) and analyzed using the
computer program SWEEPS (Pollack, 1997
). The WTN recordings were
bandpass filtered (100-1000 Hz), full-wave rectified, and integrated
over a 40 msec time window beginning at stimulus onset. For single-unit
recordings, the number of spikes was counted in a 50 msec time window
beginning at stimulus onset, except for one ARF with unusually long
latency in which the window began 10 msec after stimulus onset.
We describe ARFs according to a number of parameters. Characteristic
frequency (CF) is normally defined as the frequency at which threshold
is the lowest. However, because cricket auditory receptors have
extremely small axons, we were not always able to maintain recordings
long enough to measure threshold. In these cases, we took as CF the
best frequency (BF) that, at the lowest suprathreshold intensity
tested, elicited the largest number of spikes. BF is usually defined as
the frequency that elicits the largest number of spikes at a given
sound intensity. We used this definition in most cases, but we departed
from it for some ultrasound ARFs. As shown in Figure 3E,
some ultrasound ARFs are sensitive to 10 and/or 16 kHz, as well as to
ultrasound. At high sound intensity, they may produce a larger number
of spikes to 10 or 16 kHz than to ultrasound, although a peak in spike
count near the CF is still evident. Strictly speaking, the BF at these
intensities would be 10 or 16 kHz. However, to ensure that single ARFs
maintained a single identity through the analysis, we took as BF the
frequency of the response peak closest to CF. Spontaneous rate was
determined from recordings 2-20 sec (primarily 6-15 sec) in duration
without sound stimulation. Threshold intensity was estimated from
nonlinear curves fit to intensity-response data (Yates, 1990
) as the
sound intensity at CF at which an ARF produced one spike above the
spontaneous rate. Curves were fit using Sigma Plot (SPSS,
Chicago, IL). In most cases, a five-parameter sigmoid model was used.
For ARFs with high threshold, either a four-parameter sigmoid or
logistic model was applied.
 |
RESULTS |
We made single-unit recordings from more than 120 ARFs. ARFs
respond to sound in a tonic manner (Fig.
1). Because the axons of cricket ARFs are
too small to make prolonged stable single-unit recordings, the mean
recording duration was ~3 min (range of 1-11 min).

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Figure 1.
Single-unit recordings from two different ARFs.
ARFs respond in a tonic manner. Stimulus frequency and intensity are
given at the left of the traces. Stimulus monitors are
shown below the traces. Calibration applies to
all traces.
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|
Distribution of CF
We determined the CFs of 86 ARFs. They appear to fall into three
populations based on their CF: low-frequency (
5.5 kHz), mid-frequency
(10-12 kHz), and ultrasound (
18 kHz) ARFs (Fig. 2A). Three-quarters
(74.5%) of ARFs had CFs from
3 to 5.5 kHz. Among these, a majority
showed CFs from 4 to 5.5 kHz. The remaining CFs were 10-12 kHz (8%)
or in the ultrasound range,
18 kHz (17.5%) (Fig.
2A). We did not encounter any ARFs with CFs in the
range of 6-9 kHz. Seven ARFs appeared to have CFs outside of the range we investigated (3-40 kHz in the early experiments, 2-40 kHz in the
later ones).

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Figure 2.
A, The distribution of CFs of 86 ARFs. CFs of 3 kHz and lower and 40 kHz and higher are expressed as
3 and 40, respectively. ARFs
appear to fall into three populations based on CF ( 5.5, 10-12, and
18 kHz). B, The relationship between the shift
of best frequency and stimulus intensity. Ten representative ARFs are
illustrated by different symbols.
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|
We determined CF from BF at the lowest suprathreshold intensity tested
(see Materials and Methods). If the BF changes with stimulus intensity,
our determination may not be appropriate. In vertebrate auditory nerve
fibers (ANFs), for instance, BF is shifted to lower frequencies with
increasing stimulus intensities (Møller, 1977
; Capranica, 1992
;
Sams-Dodd and Capranica, 1994
). Figure 2B illustrates
that BF was fairly stable in those ARFs that we tested over a wide
range of intensities. The changes that did occur were all to
neighboring frequencies that we examined (see Materials and Methods for
ultrasound ARFs) (Fig. 2B). Therefore, our
determination of CF from BF at the lowest suprathreshold intensity tested is appropriate.
Iso-intensity responses of ARFs
Most low-frequency ARFs are similar to one another in
their patterns of frequency sensitivity. They are fairly selective at low intensities, and at higher intensities, they exhibit additional sensitivity peaks to higher sound frequencies, generally in the range
of 8-12 kHz (Fig. 3A). A
small number of low-frequency ARFs had another sensitivity peak even at
low intensities (Fig. 3B). We found two types of
mid-frequency ARFs based on their frequency filtering properties. One
of these, which we refer to as mid-frequency low-pass ARFs, responds
well to CF and lower (Fig. 3C). The other type,
mid-frequency high-pass ARFs, responds to CF (10 or 12 kHz) and higher
(Fig. 3D). We also found two types of ultrasound ARFs. One
type is almost as sensitive to 10 or 16 kHz as to ultrasound (Fig.
3E). The other type is sensitive only to ultrasound at low intensities (Fig. 3F).

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Figure 3.
Iso-intensity curves of six representative ARFs.
The mean number of spikes from three responses is illustrated as a
function of frequency. ARF identifications and their CFs are shown on
the top left or right. Stimulus intensity
is given beside each iso-intensity curve.
A and B are low-frequency ARFs.
C and D are mid-frequency low- and
high-pass ARFs, respectively. E and F are
ultrasound ARFs. See Results for further explanation.
|
|
Our sample of ARFs is representative of the entire population of
auditory receptors
It is extremely unlikely, given the sample size of our single-unit
recordings (n = 86), that we have recorded from each of the ~70 receptors in the cricket's ear. To determine whether our sample is representative of the entire receptor population, we compared
WTN recordings with single-unit recordings. Examples of WTN recordings
are shown in Figure 4. These recordings
reflect the summed activity of all ARFs that respond to the stimulus. The conspicuous differences in amplitude of compound action potentials elicited by low frequency and ultrasound are attributable to the differences of the number of receptors responding to these frequencies (Pollack and Faulkes, 1998
). Figure
5A summarizes WTN response amplitude from 10 different ears in response to 80 dB stimuli. Figure
5B shows the total number of spikes produced by 80 ARFs, recorded as single units, to the same stimuli (we excluded six ARFs for
which we did not have responses at 80 dB over the entire frequency
range). The iso-intensity curve for the summed single-unit responses is
quite similar to the WTN recording, with the exception that the small
peak visible at 30 kHz in the summed single-unit responses is not
evident in the WTN recordings (Fig.
5A,B). The overall similarity of
the two curves, however, suggests that our sample of ARFs is reasonably
representative of the entire population of auditory receptors.
Nevertheless, we cannot exclude the possibility that we have missed
some receptor types.

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Figure 4.
Extracellular recordings from the WTN in one
animal. Stimulus frequency and intensity are given at the
left of the traces. Stimulus traces are shown at
bottom. Scale bar applies to all traces.
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Figure 5.
Comparison between WTN and single-unit recordings.
A, WTN recordings were filtered, full-wave rectified,
integrated, and normalized to the maximum response. Responses from 10 different ears were averaged and normalized again. In each WTN
recording, 3-10 repetitions were presented at each frequency. Error
bars indicate SDs. B, Summed spike counts of 80 ARFs
stimulated over the range of 3-40 kHz at 80 dB. See Results for
further explanation.
|
|
Additional sensitivity peaks
The iso-intensity curves of Figure 3 show that single ARFs may
exhibit sensitivity peaks at several frequencies in addition to their
CF. To examine this phenomenon more systematically, we adopted a
quantitative criterion for the identification of additional peaks.
Sensitivity peaks were identified at those frequencies that elicited
spike counts above the threshold level (see Materials and Methods) and
were flanked by troughs in which the response dropped to 75% of that
at the peak. Sensitivity peaks occasionally spanned two to three
frequencies. In these cases, if mean spike count was greatest at one of
these frequencies, this was taken as the position of the sensitivity
peak. If spike counts were equal, the position of the peak was
taken either as the frequency at which the SD of the response of
the ARF was the lowest or as the mean of the frequencies, if the
SDs were the same. Figure 6 illustrates
additional sensitivity peaks of two ARFs. There are two sensitivity
peaks in Figure 6A (a and b)
and three in Figure 6B (c-e). Sensitivity
peaks a and c occurred at BF (see Materials and
Methods), and b, d, and e were
additional sensitivity peaks. In general, the frequencies of additional
sensitivity peaks remain stable with increasing intensity. In Figure
3D, for example, an additional sensitivity peak is apparent
at 16 kHz for all intensities illustrated. Rarely (~7% of additional
sensitivity peaks), the additional sensitivity peaks shifted to
neighboring stimulus frequencies as intensity increased. In these
cases, we designated additional sensitivity peaks according to their
frequencies at the lowest sound intensities at which they appeared. The
number of additional sensitivity peaks in single ARFs varied from one
to five.

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Figure 6.
Criteria for sensitivity peaks. Iso-intensity
responses were normalized to the number of spikes at BF (see Materials
and Methods) after spontaneous rate was subtracted. Sensitivity peaks
occurred at frequencies that elicited responses above threshold levels
(see Materials and Methods) and were flanked by troughs in which the
responses dropped to 75% of the peak. Peaks in A
(a) and B
(c) occurred at BF. Additional sensitivity peaks
occurred at A (b) and
B (d, e). Spontaneous
rates, threshold, and 75% bandwidth (75% BW)
are illustrated by different dashed lines. ARF
identifications, CFs, and sound intensity above threshold
(+TH) are given at the top left or
right. Both A and B are
iso-intensity curves at 80 dB. A, Low-frequency ARF with
unusually low threshold and long latency. This ARF maintained its
frequency selectivity, even at nearly 60 dB above threshold.
B, Ultrasound ARF. This ARF was almost equally sensitive
to 16 and 30 kHz at threshold. Additional sensitivity peaks occurred at
5 and 18 kHz.
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|
In a sample of 70 ARFs (most of them tested at more than one
intensity), 132 additional sensitivity peaks occurred. In Figure 7, the positions of additional
sensitivity peaks are plotted as a function of CF. The diameter of each
point corresponds to the sample size. The points above and
below the diagonal dashed line represent
additional sensitivity peaks at frequencies above and below CF,
respectively. Although we did not find any ARFs with CFs of 6-9 kHz,
nor with CFs between 12-18 kHz, additional sensitivity peaks in these
ranges are not uncommon. Interestingly, most ARFs, including
mid-frequency high-pass and ultrasound ARFs, show sensitivity peaks to
4-5.5 kHz at high intensities (e.g., Figs. 1,
3D,E). This suggests that most ARFs
may respond to intraspecific signals at high intensity.

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Figure 7.
Frequencies of 132 additional sensitivity peaks
are plotted as a function of CF. The diameter of each point is
proportional to the number of additional sensitivity peaks occurring at
those coordinates (the smallest points correspond to
n = 1). The diagonal dashed line
separates additional sensitivity peaks occurring at frequencies above
and below CF.
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|
The occurrence of multiple sensitivity peaks in single ARFs should
serve to extend the cricket's audible range beyond that covered by the
CFs of their ARFs. In Figure 8, we plot
the 75% bandwidths of ARFs (Fig. 6) at 70 and 80 dB. Each
row in Figure 8 represents a single ARF. We could not
determine bandwidths for ARFs with CFs near the ends of the range of
frequencies tested, because their response curves were truncated on one
side. Thus, we include only ARFs with CFs of 4-35 kHz in Figure 8. At
70 dB, the population of bandwidths leaves a gap in the frequency range from 6 to 10 kHz, but at 80 dB, the entire frequency range is filled in
by the bandwidths of ARFs (Fig. 8). These data show that crickets can
hear a wide range of sound frequencies, even though they lack ARFs
tuned to some portions of the range.

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Figure 8.
Representation of a wide range of audible
frequencies by ARFs. Each row represents 75%
bandwidth(s) of sensitivity peak(s) from a single ARF. The plots
for 80 and 70 dB show the bandwidths of 50 and 40 ARFs, respectively.
Only ARFs with CFs of 4-35 kHz and that continued to exhibit a clear
sensitivity peak at BF (as defined in Materials and Methods) at these
relatively high intensities were included.
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Additional sensitivity peaks are not distributed randomly across the
range of audible frequencies. Two factors may contribute to their
distribution. Figure 9A shows
that additional sensitivity peaks are clustered at ~4-6 and 8-12
kHz. There are hints of additional clusters near 15 kHz and from 25-35
kHz, as well. Thus, additional sensitivity peaks occur near the
dominant frequency of intraspecific signals and its higher
harmonics.

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Figure 9.
Distributions of additional sensitivity peaks.
A, Additional sensitivity peaks are plotted according to
the frequencies at which they occur. The origins of ARF populations
contributing the additional sensitivity peaks are illustrated with
different fill patterns. Peaks are clustered at the
frequency of intraspecific signals (4-6 kHz) and its higher harmonics.
B, Additional sensitivity peaks are plotted as multiples
of the CF of the ARF in which they occur. For this analysis, ARFs with
CFs 3 or 40 kHz were excluded. Peaks are clustered at harmonics of
the CF ( , , 1/2, and 2 times the CF). See
Results for further explanation.
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|
In Figure 9B, the positions of additional sensitivity peaks
are plotted as multiples of the CFs of the ARFs in which they occur. We
excluded ARFs with CFs
3 or
40 kHz. Here, it is evident that the
additional sensitivity peaks tend to occur at subharmonics and higher
harmonics of the CF. This suggests that the positions of the peaks may
be set by factors (e.g., mechanical resonance) similar to those that
determine the value of the CF.
The cluster of additional sensitivity peaks at 4-6 kHz is derived from
all ARF populations (Fig. 9A). Approximately half of the
low-frequency ARFs contributing to this cluster had CFs of 3 kHz or
lower (e.g., Fig. 7). Additional sensitivity peaks near 10 kHz occurred
primarily in low-frequency ARFs with CFs of 4.5-5.5 kHz and to a
lesser extent in ultrasound ARFs. Additional sensitivity peaks near
16 kHz occurred in all populations. Additional sensitivity peaks at
20-35 kHz were primarily derived from low-frequency ARFs (Figs. 7,
9A). However, most of these peaks were not consistent and
disappeared at higher intensities (e.g., Fig. 3A).
In Figure 9B, the most conspicuous clusters of additional
sensitivity peaks occurred at
,
, 1/2, and 2 times the CF. The clusters at the subharmonics derive primarily from 10 kHz and ultrasound ARFs, and those at higher harmonics are primarily
from low-frequency ARFs.
Frequency selectivity at CF
We quantified frequency selectivity by computing the quality
factor at 75% (Q75%), defined as BF divided by the
bandwidth at 75% of the normalized response at a given intensity (Fig.
6). The larger the Q75% value, the greater the
frequency selectivity. To compare frequency selectivity among the ARF
populations, we chose two narrow intensity ranges, from 0 to <5 dB
above threshold (Fig.
10A) and from 10 to
<15 dB above threshold (Fig. 10B).
Q75% varies widely among ARFs. At near-threshold
intensity, there appears to be a tendency for low-frequency ARFs to be
more sharply tuned than ultrasound ARFs, although the difference is not
significant (Fig. 10A). At higher intensity, the
Q75% values of the three ARF populations are
similar (Fig. 10B).

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Figure 10.
Frequency selectivity of ARFs. Frequency
selectivity (Q75% value) was calculated as BF
divided by 75% bandwidth. Sample sizes and stimulus intensity above
threshold (+TH) are given at the top
right. A, Q75% values
from threshold to <5 dB above threshold are plotted as a function of
BF. Although there appears to be a trend toward sharper tuning for
low-frequency ARFs, the difference between Q75%
values of low-frequency and ultrasound ARF populations is not
significant (t test, df = 13;
t = 1.75; p = 0.104).
B, Q75% values from 10 to <15
dB above threshold are shown. Q75% values are
similar for the three ARF populations (ANOVA,
dfeffect = 2; dferror = 14; F = 1.18; p = 0.335).
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|
ARFs become less sharply tuned as intensity increases. The relationship
between Q75% and stimulus intensity is shown in
Figure 11A for a few
representative ARFs. Q75% decreases with increasing
stimulus intensity. Regression lines for a larger number of ARFs are
shown in Figure 11B.

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Figure 11.
Frequency selectivity decreases with increasing
intensity. A, The Q75% values of
four representative ARFs are plotted as a function of increasing
intensity above threshold at CF with different symbols and shades of
gray. B, The changes of
Q75% values with increasing intensity for a
larger number of ARFs (n = 19) are plotted as
slopes of regression lines of log Q75% versus
intensity. Regression lines were calculated from three to five values
for each ARF.
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 |
DISCUSSION |
Our results demonstrate that the wide frequency range of cricket
hearing is mediated by a discontinuous population of receptor neurons,
the CFs of which are clustered around a few frequency regions within
the audible range. The overall hearing range extends beyond that
covered by the CFs of ARFs, because ARFs exhibit distinct sensitivity
peaks at frequencies other than the CF. This situation differs from
that found in the ears of higher vertebrates and bushcrickets, which
also have extended hearing ranges. In these animals, the broad range of
hearing is matched by a similarly broad range of CFs of receptor
neurons (cats: Kiang, 1965
; bushcrickets: Römer, 1983
; Stumpner,
1996
). Our results are, to our knowledge, the first to demonstrate that
a broad range of hearing is generated by multiple sensitivity peaks of
receptor neurons.
Distributions of CFs
Frequency sensitivity of cricket ARFs has been reported in three
papers (Zaretsky and Eibl, 1978
; Esch et al., 1980
; Hutchings and
Lewis, 1981
). In all three cases, as in the present study, the largest
population of ARFs had CFs near the dominant frequency of the calling
song. Two of the studies (Zaretsky and Eibl, 1978
; Esch et al., 1980
)
were limited to frequencies
20 kHz, and thus ultrasound ARFs were
unlikely to have been detected. In contrast, Hutchings and Lewis (1981)
used frequencies up to 42 kHz and, like us, studied T. oceanicus. However, they did not describe CFs in sufficient detail
for a direct comparison with our results.
Discontinuous distributions of CFs are often found in lower vertebrate
ANFs (frogs: Feng et al., 1975
; Narins and Capranica, 1976
; lizards:
Weiss et al., 1976
), and, as for crickets (see below), reflect the
frequencies of behaviorally relevant sounds (Simmons and Buxbaum,
1996
).
Frequency selectivity of ARFs
Frequency selectivity, measured as the Q75%
bandwidth of the sensitivity peak corresponding to the BF, was not
significantly different among the different populations of ARFs.
However, there appears to be a trend toward greater selectivity, near
threshold, of low-frequency ARFs (Fig. 10A).
In vertebrate ANFs, frequency selectivity tends to increase with CF
(Kiang, 1965
; Liberman, 1978
; Sachs et al., 1980
; Eatock et al., 1981
;
Salvi et al., 1992
; Sams-Dodd and Capranica, 1994
; Köppl 1997
).
In cricket ARFs, a similar tendency is absent.
Multiple sensitivity peaks
A striking characteristic of cricket ARFs is the occurrence of
multiple sensitivity peaks. This property was reported previously for
crickets by Esch et al. (1980)
and Hutchings and Lewis (1981)
, who
found ~10% of the ARFs they recorded showed two distinct frequency optima. Hutchings and Lewis (1981)
also illustrated many ARFs that
appeared to have several distinct frequency optima (e.g., their Figs.
5, 6). In our experiments, which included suprathreshold intensities,
multiple sensitivity peaks occurred in most ARFs. Multiple sensitivity
peaks are not unique to cricket ARFs. They have also been observed in
locusts (Michelsen, 1971a
; Inglis and Oldfield, 1988
). The multiple
sensitivity peaks of locust ARFs could be explained by the relationship
between the spatially distributed resonances of the tympanal membrane
and the locations of receptors (Michelsen, 1971a
,b
).
It seems likely that, in crickets too, multiple sensitivity peaks may
have their origin in the still unknown biophysical mechanisms underlying the frequency selectivity of ARFs. The main sound-collecting structure, the posterior tympanal membrane, is broadly tuned to the
dominant frequency component of the species calling song (Paton et al.,
1977
; Larsen, 1987
; but see Johnstone et al., 1970
). However, its
tuning is not sharp enough to account for the selectivity of ARFs with
CFs near this frequency. Furthermore, the decreasing sharpness of
tuning with increasing intensity (Fig. 11) is not accounted for by the
linear response of the tympanal membranes to increasing intensity
(Paton et al., 1977
). It seems clear that there are one or more
additional stages of filtering (Kalmring et al., 1978
), which might
reside in the mechanics of the inner ear (Kalmring and Jatho, 1994
)
and/or within the receptor neurons themselves (Oldfield, 1985
). A large
proportion of additional sensitivity peaks occurs at frequencies of
4-6 kHz (Fig. 9A), i.e., near the dominant frequency of
communication signals in this species. This may be attributable in part
to the inability of additional stages of filtering to overcome the
relatively large vibration of the tympanum in this frequency range
(Johnstone et al., 1970
; Paton et al., 1977
). The tendency toward a
harmonic relationship between frequencies of additional sensitivity
peaks and the CF, evident in Figure 9B, also points to
additional stages of filtering as the most likely site for generation
of these peaks.
Behavioral roles of the different ARF populations
Two of the three ARF populations, the low-frequency and
ultrasound ARFs, seem clearly related to behavior. T. oceanicus communicates using acoustic signals with dominant
frequencies near 4.5 kHz, i.e., in the same range as the CFs of the
majority of low-frequency ARFs (Fig. 2A). Ultrasound
stimuli elicit startle or avoidance responses, which may offer
protection against predation from echolocating bats (Moiseff et al.,
1978
; for review, see Hoy, 1994
). The behavioral roles of mid-frequency
ARFs are less apparent. One possibility is that, like low-frequency
ARFs, they mediate responses to communication signals. The songs of
T. oceanicus do contain energy at higher harmonics of the
dominant frequency. Behavioral experiments have shown that these may
contribute to both the recognition and localization of the signals
(Latimer and Lewis, 1986
). A second possibility is that mid-frequency
ARFs, in particular those with high-pass characteristics, play a role
in startle or avoidance responses.
Of particular interest is our finding that ARFs with CFs in the
ultrasound range often have additional sensitivity peaks in the range
of 4.5-5.5 kHz (Fig. 7). Startle or avoidance responses, similar to
those evoked by ultrasound, are also occasionally elicited by
low-frequency stimuli of sufficient intensity (Popov and Shuvalov, 1977
; Nolen and Hoy, 1986
). Our results raise the possibility that
avoidance responses to low-frequency sounds occur because these stimuli
activate ultrasound ARFs via their additional sensitivity peaks.
Behavioral experiments show that, although crickets detect sounds over
a broad range of frequencies, they categorize their auditory world into
only two frequency bands: a low-frequency band extending up to ~15
kHz and a high-frequency band extending from 15 kHz into the ultrasound
range (Wyttenbach et al., 1996
). The existence of multiple sensitivity
peaks implies that none of the three ARF populations will be activated
exclusively by stimuli in their "own" frequency band. Particularly
at higher intensities, identification of a sound as belonging to the
"low-frequency" or "high-frequency" categories may be ambiguous
at the level of single receptor neurons. The sharp categorization of
sound frequencies likely comes about as a result of interactions among interneurons.
 |
FOOTNOTES |
Received Sept. 15, 1998; revised Nov. 30, 1998; accepted Dec. 3, 1998.
This work was supported by grants from the Natural Sciences and
Engineering Research Council of Canada and the Whitehall Foundation to
G.S.P. and in part by a Government of Canada award to K.I.
Correspondence should be addressed to Gerald S. Pollack, Department of
Biology, McGill University, 1205 Avenue Dr. Penfield, Montréal, Quebec H3A 1B1, Canada.
 |
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