The Journal of Neuroscience, July 2, 2003, 23(13):5617-5626
Previous Article | Next Article 
Central Cellular Mechanisms Underlying Temperature-Dependent Changes in the Goldfish Startle-Escape Behavior
Thomas Preuss and
Donald S. Faber
Albert Einstein College of Medicine, Department of Neuroscience, New
York, New York 10461
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Abstract
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Activation of auditory afferents on the lateral dendrite of the Mauthner
(M)-cell triggers an escape response (C-start) in goldfish. To study distinct
behavioral changes and their physiological correlates on a cellular level we
examined the effect of acute changes of temperature on M-cell membrane
properties and intracellular responses to sound clicks and on C-start
kinematics and behavior, focusing on threshold and initial escape direction,
two properties determined on the M-cell level. Cooling slowed C-start motor
performance, increasing response latency and decreasing peak velocity and peak
acceleration, but increased the probability of triggering the escape. In
addition, the likelihood of escapes in an inappropriate direction (e.g.,
responses toward the stimulus instead of away from it) increased at low
temperatures. On a cellular level, cooling caused a distinct increase in input
resistance of the M-cell and in the dendritic space constant for the
auditory-evoked synaptic potentials. Moreover, cooling decreased the magnitude
and delayed the onset of feedforward inhibition of the M-cell. These
temperature-induced changes in the network and in the intrinsic M-cell
properties combine to support behavioral hyperexcitability, but apparently
also alter the directional decision-making process during an escape. More
generally, our results illustrate that the balance between excitatory and
inhibitory influences can determine the expression of a behavior and its
modification and at the same time underline the significance of temperature
for nervous system function and behavior.
Key words: dendritic cable properties; auditory-evoked response; excitatory/inhibitory balance; kinematics; neural temperature effects; escape behavior; neuroethology; Mauthner cell
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Introduction
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One fundamental issue in neuroscience is to understand the neural basis of
naturally occurring behaviors; this can be approached by perturbing a system
that is accessible for both cellular and behavioral investigations. Then, it
may be possible to draw general conclusions from the changes observed at these
levels. Poikilotherms, that is, cold-blooded animals, are well suited for such
studies because they have the task of maintaining coordinated sensorimotor
function in the face of continual changes in temperature, which are known to
influence both nervous system function and behavior. More specifically, it is
established that a wide range of aquatic species are subjected to acute
temperature changes that can be as great as 15°C over only a few minutes
(Montgomery and MacDonald,
1990
). The present study was designed to quantify the effects of
acute temperature changes on the teleost startle response to extract central
cellular and synaptic mechanisms critical to the proper execution of this
behavior.
The teleost C-start is a prominent startle response to sudden visual or
mechanosensory stimuli (Eaton and Hackett,
1984
), considered to be important for predator avoidance
(Eaton et al., 1977
; Webb
1978a
,
1986
; for review, see
Domenici and Blake, 1997
).
C-starts are controlled by a brainstem escape network that includes two large
reticulospinal Mauthner neurons (M-cells) and their associated networks
(Faber et al., 1989
), which
have been the subject of numerous neurophysiological
(Furshpan and Furukawa, 1962
;
Furukawa and Furshpan, 1963
;
Faber and Korn, 1978
;
Korn et al., 1990
;
Faber et al., 1991
;
Zottoli and Faber, 2000
) and
neuroethological (Eaton and Hackett,
1984
; Eaton, 1991
;
Eaton et al., 1981
,
1991
,
2001
) studies. Essentially, an
action potential in one M-cell activates contralateral motor execution
networks that cause an initial fast body bend (C-start) away from an aversive
stimulus (Zottoli, 1977
;
Eaton et al., 1981
). Thus,
activity in the left or right M-cell determines the initial escape direction
and execution, whereas the subsequent parts of the escape are apparently
controlled by other descending brainstem neurons
(Fetcho, 1991
;
Foreman and Eaton, 1993
).
Escape success depends largely on the motor performance during C-starts, on
behavioral responsiveness (i.e., on response threshold) (Webb
1981
,
1986
;
Blaxter and Fuiman, 1990
;
Webb and Zhang, 1994
), and on
the control of its directionality (Eaton
et al., 2001
), features that may be sensitive to changes in
ambient temperature (Webb,
1978b
; Webb and Zhang,
1994
; for review, see Temple
and Johnston, 1997
). Although changes in the kinetic properties of
the neuromuscular system may account for the thermal dependence of swimming
performance (Bennett, 1985
,
1990
;
Johnson et al., 1998
), the
effect of temperature on behavioral responsiveness is likely to be
attributable to cellular and synaptic factors that determine M-cell
excitability, including the temperature sensitivity of the sensory pathway
(Fay and Ream, 1992
). Indeed,
our findings indicate that an increased behavioral responsiveness and a
decreased directional selectivity during acute cold exposure can be correlated
to changes in the two mechanisms that control M-cell activation, namely its
dendritic cable properties and the balance between synaptic excitation and
inhibition.
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Materials and Methods
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Goldfish (Carassius auratus), 1013 cm in body length, were
obtained commercially between May and October 2001 (Hunting Creek Fisheries,
Thurmont, MD) and maintained in groups of 1015 animals in a 120 l
recirculating system of de-ionized water conditioned with NovAqua (0.13 ml/l;
Novalek, Hayward, CA), Instant Ocean (16 mg/l; Aquarium Systems, Mentor, OH),
Copper Safe (0.32 ml/l; St. John Laboratories, Harbor City, CA) at 18°C on
a 12 hr light/dark photoperiod. Water quality was monitored regularly and was
the same for holding and experimental tanks (pH 7 ± 0.2; dissolved
oxygen saturated, 8 ppm). Fish were allowed to acclimate for at least 3 weeks
before use.
Behavioral experiments. A total of 39 animals were used to study
the effect of acute temperature exposure on the escape behavior. Individual
groups of three fish were transferred from the holding tank to an experimental
tank that contained either water at the acclimation temperature (18°C) or
cold (8°C) water and were allowed to adapt for 30 min before testing.
Thus, three fish were tested together for each trial. We chose to use three
fish in the arena rather than an isolated one, as had been done in previous
studies (Oda et al., 1998
;
Zottoli et al., 1999
), because
it allowed us to collect extensive data on behavioral responsiveness,
including its dependence on stimulus intensity. This modification was possible
because the experimental tank is significantly larger than that used in
previous studies of this behavior. The larger tank allows most escapes to
occur in an open field that is at least two to three body lengths square,
thereby reducing the effects of any nearby obstructions
(Eaton and Emberley, 1991
).
Because isolated fish quickly learn to avoid the center of the arena, using
three fish is favored. As described below, the results are consistent with the
notion that the three fish respond independently. After the conclusion of
1520 escape trials at a given temperature, the water temperature was
raised to 18°C or lowered to 8°C, as appropriate, with the fish
remaining in the tank, and then another 1520 escape trials followed.
The starting temperature alternated from one group to the next. The more rapid
temperature change experienced by the fish exposed first to cooling, compared
with those cooled after being first studied in the warm, had no obvious effect
on their response frequencies.
The experimental setup consisted of a circular acrylic tank (76 cm
diameter, 28 cm water depth) connected to a water reservoir attached to a
chiller (Delta Star; Aqua Logic, San Diego, CA), which changed the water
temperature in the experimental tank from 18 to 8°C in
50 min.
Temperature was returned to 18°C at a similar rate by two 200 W water
heaters. The water temperature in the tank was continuously monitored and
regulated to ±1°C by a digital temperature controller (Nema Type
4x; Aqua Logic). To eliminate external mechanosensory and visual cues, the
tank was on an antivibration table (TMC 63-530; Technical Manufacturing Corp.,
Peabody, MA) and had surrounding opaque covers. Illumination was provided
through a 3 mm thick translucent tank cover by a single 100 W floodlight
centered above the tank and from below with three 40 W lights with translucent
covers. The inner side walls of the tank were lined with 6 cm thick and 26 cm
high polyurethane foam, which served to support an underwater loudspeaker
(UW-30; University Sound, Buchanan, MI) for sound stimulation. Short-latency
C-start escapes were elicited with sound clicks consisting of a single sine
wave of 200 Hz produced by a digital waveform generator (Model 39; Wavetek
Ltd, Norfolk, UK) in combination with an audio power amplifier (Servo 120;
Samson, Syosset, NY). The stimulus amplitude and the time intervals between
trials were varied randomly, from 130 to 170 dB sound reference level 1 µPa
(which translates to
60110 dB in air) and 220 min,
respectively. Ventral views of the animals were recorded at 1000 frames/sec
and at a spatial resolution of 512 by 384 pixels through a mirror at 45°
below the tank, using two high-speed video cameras (Kodak Extapro 1000 HRC;
Eastman Kodak, San Diego, CA), and stored on an internal magneto-optical
drive. The field of view of one camera, equipped with a 8.5 mm wide-angle
lens, covered the entire tank area, to record the escape behavior of all three
animals simultaneously for determining escape probabilities and trajectories.
The second camera was equipped with a 50 mm lens and recorded a magnified view
of a 32 x 25 cm area in the middle of the tank (see
Fig. 5). Typically, the
experimenter waited until at least one fish was in this zone before activating
the stimulus. This procedure allowed recording C-starts, with high resolution,
of fish that had an unobstructed escape path (i.e., at least a body-length
distance from the border of the aquarium). In general, the behavior was also
not impeded by neighboring fish, because the separation between fish in these
experiments was greater than one body length in 83% of the cases. A 1 msec
light-emitting diodestimulus marker added to the optical path outside
the tank and not seen by the fish indicated the stimulus onset and served as a
reference point for latency measurements. In addition, the waveform and
amplitude of the auditory stimulus was recorded (sampling rate, 30 µsec)
with two hydrophones (SQ05; Sensor Technology, Collingwood, Ontario, Canada),
one positioned close to the underwater speaker and the other on the opposite
border. A series of hydrophone recordings from various midwater positions in
the tank revealed an approximate radial intensity gradient of the sound field
with a maximum at the position of the underwater loudspeaker.

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Figure 5. Effects of temperature on response direction. Left, Top view of the tank,
illustrating the location and relative size of the high-magnification region.
The inappropriate response direction for fish within the zone defined by the
dashed circle is defined as toward the stimulus, and the corresponding
response frequencies in 8 and 18°C are plotted at the upper right. In
contrast, when the fish is at least partially in the outer zone, the
inappropriate response is now defined as one during which it turns into the
wall. The response frequencies for this case are plotted at the lower
right.
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C-start kinematics and latency were analyzed at 1000 frames/sec. For each
escape sequence, 180 frames (starting 10 frames before the stimulus) were
digitized and the x- and y-positions of the head and the
center of mass (COM) were measured using video-image tracking software
(WINanalyze; Micromak, Erlangen, Germany). To facilitate detection, two
markers were glued to the ventral midline in some fish, one close to the tip
of the head and the other at the approximate position of the animals' center
of mass (Fig. 1), which is
roughly defined as the midline point approximately one-third of the body
length from the rostral end of the animal. The body-length-specific
instantaneous velocity (body lengths/sec) and acceleration of the COM, and the
total distance traveled by the COM at various time intervals (i.e., 100 and
150 msec after stimulus onset, and 100 msec after onset of the behavioral
response) were calculated from smoothed (10 factor binomial; Igor Pro;
WaveMetrics, Lake Oswego, OR) x-, y-position data. In
addition, the angle between the orientation of the fish and the speaker
(Fig. 1) and the angular
velocity and acceleration were calculated for successive frames. Response
latency was defined as the first detectable movement of the head after the
stimulus and was measured manually in successive video images of marked and
unmarked fish. When more than one fish responded in a given trial (<20% of
the analyzed escapes), only the measurement from the fish that responded first
was used for kinematic analysis. The relative frequency of C-starts was
calculated from individual experimental trials with three animals each, and
when more than one fish responded, only those C-starts that began within 2
msec after the onset of the first response in the warm (18°C) or 4 msec in
the cold (8°C) were scored, eliminating responses that might have been
triggered by movements of the first fish to react. These time windows, which
are quite restrictive, were based on our physiological measurements of sensory
and M-cell processing times at the two temperatures (see
Table 1). For all kinematic
measurements, restricted to marked fish, the mean ± SE was calculated,
with N equal to the number of animals and n to the number of
escapes analyzed. In contrast, measurements of latencies (n = number
of escapes) and response frequencies (n = total number of trials)
included unmarked fish and had larger sample sizes

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Figure 10. Temperature dependence of feedforward inhibition in the escape network.
A, M-cell potentials were evoked by pairing a sound-evoked PSP with
the antidromic action potential. Superimposed records of the antidromic action
potential when evoked alone (control) and when paired with a preceding sound
evoked PSP (dashed line). To better illustrate the magnitude of the action
potential shunt, the PSP alone (data not shown) was digitally subtracted from
the composite response (shunted). Note that because there is only a small
inhibitory driving force, the PSP itself is predominantly excitatory (see
Results). B, The magnitude of this shunt was used to calculate the
inhibitory conductance, GIPSP. Top, Sound-evoked PSPs;
middle, the calculated corresponding inhibitory conductances
(GIPSP) obtained by varying interstimulus interval and
expressed as fractions of input conductance (Gm). Solid
traces are at 18°C and dotted traces, 8°C. The first vertical dashed
line of each pair indicates the time of PSP onset and the second corresponds
to the peak of GIPSP. Note the decrease in amplitude of
the inhibition and the increase in its time to peak at 8°C. All traces in
A and B are the averages of five sweeps.
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Electrophysiological recordings. A total of 19 goldfish were used
to study in vivo effects of acute temperature exposure on the
electrical and synaptic properties of the M-cell. The temperature in these
experiments was initially 8°C (measured in the brain), and it was
subsequently raised to 18°C within a 30 min period. The temperature was
measured with a 33-gauge hypodermic thermocouple probe (HYP-0; Omega,
Stamford, CT) inserted into the medulla oblongata. Brain temperature was
changed by varying the temperature of the water used to aerate the gills and
was kept within a range of ±1°C by using a cooling/heating system
similar to that described for the behavioral experiments. The saline used to
superfuse the brain was kept at the same temperature as the respiration water
by using a constant-temperature funnel (Aldrich, Milwaukee, WI) connected to
the cooling system. The fish were anesthetized initially using ice-cold water
and throughout the experiment by flowing aerated, conditioned tap water
containing anesthetic (70 mg/l 3-aminobenzoic acid ethyl ester; Sigma, St.
Louis, MO) through the gills; they were immobilized with
D-tubocurarine (1 mg/g of body weight) injected intramuscularly.
The surgical and recording procedures were similar to those described
previously (Faber and Korn,
1978
).
Intracellular responses to sound and antidromic stimulation were recorded
from various positions (50400 µm from the axon cap; i.e., the
initial segment and axon hillock region of the M-axon) along the M-cell
lateral dendrite and from the soma, with electrodes (710 M
)
filled with 5 M K-acetate. Recordings were made either with a
single electrode in up to seven successive penetrations or with two electrodes
simultaneously. All recordings were in current-clamp, and cross talk between
the electrodes was minimized electronically with an Axoprobe-1A amplifier
(Axon Instruments, Foster City, CA). Data were recorded online with a
Macintosh G4, using acquisition software developed in the laboratory (sampling
rate, 1030 µsec) and analyzed with the same software and with Igor
Pro. Sound-evoked PSPs were elicited by single sine waves of 200700 Hz
and 6684 dB in air produced by the waveform generator in combination
with two speakers, one on each side of the fish and slightly above it. The
loudspeakers, with integrated amplifiers, were each 60 cm from the animals'
heads. The sound stimulus was recorded with a microphone positioned above the
fish, stored online together with the electrical recordings, and calibrated
with a sound-level meter (72-860; Tenma, Springboro, OH). For antidromic
stimulation of the M-cell a bipolar electrode (SS 2C TW; Plastics One,
Roanoke, VA) was placed on the exposed spinal cord near the posterior end of
the dorsal fin.
Statistical analysis. Data were analyzed using a statistical
software package (SAS 8.1; SAS Institute, Cary, NC). Hypotheses about fish
kinematics were assessed with a mixed-models repeated-measures ANOVA. In
general, the same approach was used to test hypotheses related to data on
M-cell physiology, unless the study design required a t test, as
noted in Results. Hypotheses concerning the distribution of escape behavior,
in which fish triplets were the unit of analysis, were assessed by applying a
goodness-of-fit test to the binomial distribution
(Morel and Neerchel,
1998
).
 |
Results
|
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Effects of cooling on escape behavior
Sound-evoked, short-latency escapes in goldfish are characterized by an
initial C-shaped bend of the animal head and tail around the COM
(Fig. 1A), followed by
a return flip of the tail associated with forward propulsion (stages 1 and 2
in Foreman and Eaton, 1993
).
The C-bend formation was typically correlated with a distinct increase in head
velocity and head acceleration. In the example of
Figure 1B, the two
parameters had peaks at 31 and 21 msec (18°C) after stimulus onset,
respectively. On average (N = 6 fish; n = 18 trials), peak
latencies were 27.5 ± 1.1 msec for head velocity and 16.3 ± 0.5
msec for head acceleration. The kinematic profile of the COM was bimodal, with
initial velocity and acceleration peaks at 26 and 19 msec, respectively,
indicating a small displacement of the COM during C-bend formation, with the
second velocity and acceleration peaks at 46 and 33 msec being indicative of
the forward propulsion of the body during the return flip
(Fig. 1B, solid
lines). Escape-angle (i.e., the total angular rotation performed by an animal
during the C-bend and the return flip), was highly variable and depended on
the fish's initial orientation with respect to the underwater loudspeaker.
However, no obvious correlation was found between the escape-angle magnitude
and the velocity and acceleration peak amplitudes (data not shown).
Exposing goldfish acclimated to 18°C to an acute temperature drop of
10°C profoundly slows all aspects of the C-start response.
Figure 2 compares the kinematic
profiles of two C-starts that are from the same animal and have similar escape
angles at different temperatures (Fig.
2D). It shows that cooling delayed the start of COM
movement (i.e., the onset of the velocity and acceleration changes) by
20
msec and prolonged the peak time of COM velocity and escape-angle velocity
(Fig. 2AC).
Overall (N = 6; n = 21), the change in temperature resulted
in a delay in onset of the velocity curve of 13.8 ± 1.9 msec
(F = 53.18; df = 1, 19; p < 0.001) and a delay in the
onset of the acceleration curve of 13.6 ± 1.9 msec (F = 52.02;
df = 1, 19; p < 0.0001). Cooling also decreased C-start motor
performance (Fig. 3), as
indicated by a significant reduction of the COM peak velocity (F =
4.67; df = 1, 33; p < 0.04), COM peak acceleration (F =
8.81; df = 1, 33; p < 0.006), peak angular velocity (F =
5.17; df = 1, 29; p < 0.04), and peak angular acceleration
(F = 5.48; df = 1, 23; p < 0.03). However, this decrease
in peak performance is primarily attributable to a slowing of the return flip;
i.e., the second velocity and acceleration peaks are reduced in cold compared
with warm (Fig. 2A,C).
In contrast, the first peaks of the velocity and acceleration are similar in
magnitude at both temperatures, which suggests that, besides delaying its
onset, cooling has little effect on the initial C-bend formation.

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Figure 2. Effects of cooling on kinematics of C-start escape. Plots of COM velocity
(A), angular velocity (B), COM acceleration (C),
and animal orientation (D) versus time for C-starts evoked at
18°C (solid lines) and 8°C (dotted lines), respectively. Note that
cooling slows motor performance.
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Figure 3. Quantitative effects of cooling on kinematics of C-start escape. Bar plots
of body-length-specific peak velocity (A), body-length-specific peak
acceleration (B), peak angular velocity (C), and peak
angular acceleration (D) for C-starts evoked at 18 and 8°C.
Cooling significantly decreases motor performance for all measures. Error bars
indicate SEM. Bl, Body length.
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Consistent with the prolonged peak in angular velocity in the cold
(Fig. 2B), mean
escape-trajectory angles increased significantly from 74 ± 5.9° at
18°Cto97 ± 6° at 8°C(F = 4.29; df = 1, 68;
p < 0.04). Thus, cooling produced an overall shift toward larger
escape angles without altering the variability of this parameter
(Fig. 4A).

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Figure 4. Escape trajectory and motor performance during acute temperature exposure.
A, Cumulative distributions of escape angles at 18 (N = 9;
n = 34) and 8°C (N = 9; n = 36), obtained from
fish with markers. Note that cooling shifts the distribution to the right
(i.e., toward larger escape angles). B, Cumulative distributions of
response latencies at 18 (N = 27; n = 53) and 8°C
(N = 33; n = 48), obtained from unmarked fish in the central
region of the arena. Cooling significantly increases the latency of C-start
escapes and broadens the latency distribution. C, Bar plots of
distance traveled in body lengths within defined time intervals. Bl, Body
length.
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C-bend formation latency, measured as the first detectable movement of the
head after stimulus onset, is a behavioral measure directly correlated to the
activity in the brainstem escape network that includes the two M-cells
(Eaton et al., 1981
) and thus
yields important information with respect to the temperature dependence of the
system. This measure increased significantly on average, from 11.5 ±
0.3 msec at 18°C to 27.3 ± 0.8 msec at 8°C (F =
202.66; df = 1, 74; p < 0.0001). In addition, in the cold the
distribution of response latencies was much wider than in the warmer
temperature, as illustrated by the cumulative distributions in
Figure 4B, although
the coefficient of variation was relatively constant.
One important measure of C-start motor performance that integrates all of
the kinematic parameters described above is the distance traveled by the COM
in a specified time interval. Cooling to 8°C significantly (F =
12.66; df = 1, 33; p < 0.002) decreased the distance traveled
within 100 msec after stimulus onset compared with warm
(Fig. 4C, left).
However, after an additional 50 msec the differential was not significant
(Fig. 4C, middle).
Similarly, when the temporal reference was instead response onset there was no
significant difference between the distances traveled in cold and warm after
100 msec (Fig. 4C,
right). This minimization of the differential in performance reflects the fact
that warm animals began to decelerate at
27 msec, whereas in colder fish
deceleration was delayed by
24 msec
(Fig. 2C).
Nevertheless, the observed difference within the initial 100 msec after
stimulus onset might be of biological relevance because this is a common
strike time of piscivores attacking prey
(Webb, 1978b
).
A vital property of the C-start is its directionality (i.e., the ability of
the fish to turn away from the auditory stimulus source), at least in
open-field conditions (Eaton and Emberley,
1991
).Thus, we analyzed the effects of cooling on response
directionality for fish that were in the middle of the tank and had a clear
directional choice (i.e., with only one body side facing the underwater
loudspeaker). In the majority of trials the initial C-bend was directed away
from the loudspeaker and turns toward the stimulus were rare. However, as
shown in Figure 5, the
percentage of turns toward the stimulus increased significantly (p
< 0.01;
2 test) in the cold, from 14% at
18°C(N = 24; n = 66) to 36% at 8°C (N = 27;
n = 62). In addition, temperature also affected other aspects of the
C-start escape trajectory. As noted, one camera recorded the escape behavior
of three animals in the tank, which in many trials included sequences with at
least one fish close to the wall. We treated fish located within a distance of
two-thirds of a body length from the wall as having an obstructed path away
from the stimulus (Fig. 5). In
such an instance a startled goldfish at 18°C typically performed a C-bend
away from the wall, even if that meant turning toward the auditory stimulus,
and "inappropriate" turns into the wall were observed in only 2 of
32 cases (6%). However, at 8°C this ratio increased to 18 of 92 cases
(20%) (Fig. 5).
The apparent role of the M-cells in triggering C-starts makes behavioral
responsiveness, specifically the probability of eliciting a C-start, another
important indicator of the activity in the escape network during acute
temperature exposure. Responsiveness was tested by using a randomized order of
stimulus intensities presented at random time intervals (see Materials and
Methods). The same presentation pattern was used for all the experiments, and
there was no sign of habituation or sensitization with this paradigm.
Individual C-starts of all three animals in a given trial were counted and
transformed into a trial probability (i.e., 0, 0.33, 0.67, or 1), and each
group of fish was tested in warm and cold. Under these conditions, cooling
significantly increased the mean relative frequency for sound-evoked C-starts
by
33% compared with warm (31.5 ± 2.4 vs 23.5 ± 2.2%;
F = 4.76; df = 1, 275; p < 0.03). The left graph in
Figure 6A demonstrates
this finding for pooled data over the entire range of auditory stimuli used,
whereas the right illustrates that the increase in escape probability in the
cold was found for distinct intensities. At both temperatures, response
probability and stimulus intensity showed a roughly logarithmic relationship
(Fig. 6A, right), but
because of the inherent variability of the stimulus amplitude at different
areas of the experimental tank and the limited intensity range of the
underwater loudspeaker, absolute response threshold or saturation intensity
could not be established.

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Figure 6. A, Relationship between escape responsiveness and acute
temperature exposure. Left, Bar plots of mean relative frequencies of
sound-evoked C-starts calculated from individual experimental trials with
three animals each at 18 (red) and 8°C (blue). For the right part of the
graph the same data were separated into four distinct intensity bins ranging
from 140 to 148, 149 to 156, 157 to 164, 165 to 170 dB, respectively.
B, Bar plots of the frequencies (%) with which 0, 1, 2, or 3 fish
responded per trial (solid) at the two experimental temperatures, compared
with the predicted distributions (hatched), assuming a simple binomial model
(see Results for details and statistics).
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We considered the possibility that the three fish might not respond
independently in one or both temperature conditions by performing simple
binomial analyses of the response distributions (frequencies of 0, 1, 2, and 3
escapes per trial) in the cold and warm. Specifically, the data were fit with
the expression:
where px is the probability of x escapes
in a trial, p is the average probability of escapes per fish, and
n = 3 fish. As shown in Figure
6B, both experimental distributions conformed to the
binomial predictions (p > 0.05;
2 test), with the
derived escape probabilities equivalent to those found for the two populations
(p warm = 0.235; p cold = 0.295). Thus, in each temperature
condition the three fish responded independently and with the same average
probability, which are basic properties of a simple binomial.
Effects of cooling on the M-cell synaptic responses and membrane
properties
The sound-evoked C-starts are presumably triggered by the activation of
auditory afferents that have mixed electrical and chemical excitatory synapses
on the distal lateral dendrite of the M-cell
(Furshpan, 1964
; Lin and
Faber,
1988a
,b
).
To correlate the observed effects of cooling on the escape behavior with
physiological changes in this network, intracellular responses to sound clicks
and antidromic stimulation were recorded sequentially from the M-cell soma and
lateral dendrite (Fig.
7A). Because responses to posterior eighth-nerve
stimulation are generated in the dendrite, their amplitudes are maximal
distally and smaller in the soma, and the same relationship holds for
sound-evoked PSPs (Fig.
7B, dashed vs solid lines) (see also
Casagrand et al., 1999
). The
opposite is the case for the antidromic action potential, which is generated
at the initial segment of the axon-hillock region of the M-axon and propagates
passively (Furshpan and Furukawa,
1962
) into the soma and dendrite
(Fig. 7C). Thus, the
passive spread of these potentials along the dendrite is an indicator of its
cable properties.

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Figure 7. Temperature dependence of sound-evoked PSPs and passive membrane properties
of the M-cell. A, Schematic showing that M-cell potentials evoked by
antidromic and sound stimulation were recorded successively at up to four
different sites along the M-cell soma (1) and lateral dendrite (24) at
two different temperatures. B, Somatic (solid lines, site 1) and
distal dendritic (dashed lines, site 4) sound-evoked PSPs (left) and plot of
their decrement along the dendrite (right) at 18 (red) and 8°C (blue). The
recorded sound stimulus (above) has the same time scale as PSPs. C,
Somatic (solid lines) and distal dendritic (dashed lines) antidromic action
potentials (left) and their decrement along the dendrite (right) at 18 (red)
and 8°C (blue). Note that the decrement in amplitude between the two
recordings sites is reduced at 8°C, for both responses, which is reflected
in a distinct increase of the space constant. All traces in B and
C are averages of 10 sweeps. Plots indicate means ± SEM
(n = number of traces). AC, Center of the axon cap, which surrounds
the axon hillock and initial segment; AD, antidromic.
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At 18°C the sound-evoked PSPs have multiple peaks, which are most
clearly delineated with distal dendrite recordings and typically are at a
frequency twice that of the stimulus (Figs.
7B,
8B). The fast peaks
are spike-like and thus are comparable with those of the electrotonic
component of EPSPs evoked by direct stimulation of the posterior eighth nerve
(Lin and Faber, 1988a
). This
is consistent with the notion that these peaks are mediated by electrical
synapses, whereas the underlying depolarizing envelope is chemically mediated.
Acute cooling of the fish brain from 18 to 8°C produced distinct, but
reversible changes in the latency, waveform, and amplitude of the sound-evoked
PSPs. In the example of Figure
7B, the intradendritic PSP latency increased by 1.3 msec
at 8°C, whereas on average it increased by 1.5 ± 0.2 msec from 1.3
± 0.07 in the warm to 2.7 ± 0.2 msec in the cold (N =
6). In contrast, the conduction time of the antidromic action potential of the
M-axon increased by only 0.3 ± 0.02 msec (N = 6). Although the
eighth-nerve conduction velocity is slower than that of the M-axon, the
conduction distance is at least an order of magnitude shorter, which suggests
that the increased delay of the PSP was mainly synaptic in origin. Cooling to
8°C produced a substantial broadening of the antidromic spike, which
appears to be mostly attributed to a delayed and slowed spike repolarization
(Fig. 7C, left).
Similarly, cooling also simplified the waveform of the intradendritic PSP by
reducing the number of peaks of a typically multipeak response at 18°C
(Figs. 7B, left dashed
lines; 8B,C).

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Figure 8. Temperature dependence of M-cell responses and transfer resistance.
A, The M-cell was penetrated with two microelectrodes at a distal
dendritic site and the soma for simultaneous potential recording and current
injection at two different temperatures. B, Dendritic (upper left)
and somatic (lower left) recording of a sound-evoked PSP (300 Hz, 84 dB) and
corresponding antidromic spike (upper right and lower right, respectively) at
18°C. C, Same recordings as in B, but at 8°C.
D, Changes in somatic membrane potential produced by an 80 nA
dendritic current pulse in the hyperpolarizing and depolarizing directions at
18 (solid line) and 8°C (dashed line). Traces in BD are
averages of 10 sweeps. E, Plot of the corresponding
voltagecurrent relationship (V2 vs
I1) at 18 (solid line) and 8°C (dashed line).
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Despite the behavioral observation of a rise in escape probability with
cooling, the peak PSP amplitudes in the dendrite at 8 and 18°C were
comparable (Fig. 7B).
Overall, when average values were compared for four experiments with
sequential recordings from the two sites, there was a small but insignificant
increase (11%) in the dendritic peak PSP amplitude in the cold, and a larger
but significant increase in the somatic peak amplitude (24%; p <
0.05; paired t test). Thus, given the relatively greater effect at
the soma as opposed to the locus of synaptic input, we asked whether changes
in dendritic cable properties might contribute to the increased behavioral
responsiveness. Sequential measurements from multiple sites of PSP and
antidromic spike amplitudes (N = 3) showed that, indeed, cooling
changed the cable properties in the lateral dendrite, as indicated by a
reduced fractional decay of the PSP from dendrite to soma and less spatial
attenuation of the intradendritic spike when comparing responses obtained in
the cold and warm. Specifically, there was a significant increase of the mean
length constant
, from 275 ± 43 to 577 ± 20 µm
(p < 0.02; t test) in the orthodromic direction, and from
226 ± 38 to 346 ± 25 µm in the antidromic direction
(p < 0.03; t test)
(Fig. 7B,C). Thus,
although the sound-evoked PSP could be smaller at the cold than at the warmer
temperature when recorded at the dendritic locus of synaptic input, it could
nevertheless be larger in the soma (Fig.
7B). An additional mechanism for the increased behavioral
responsiveness could be a depolarization of the M-cell membrane induced by
cooling. However, within the temperature range tested the membrane potential
remained constant, being on average 77 ± 0.7 mV at 8°C and 78.5
± 1.1 mV at 18°C (N = 17).
The experiments described above required mapping response amplitudes
sequentially along the somadendrite membrane, changing the temperature
while maintaining intracellular recording and then repeating the mapping
procedure in reverse order. To control for the possibility that the repeated
penetrations of the cell compromised the integrity of the amplitude
measurements we performed another series of experiments (N = 2) in
which the intracellular responses were recorded simultaneously at the distal
dendrite and soma and the temperature was increased after collecting data at
8°C (Fig. 8A).
Representative recordings, shown in Figure
8, B and C, confirm that cooling decreased the
relative decay of the PSP, by 33%, and the antidromic spike, by 15%, compared
with warm. In the same experiments, hyperpolarizing and depolarizing current
pulses were injected through the intradendritic electrode, and the resulting
change in membrane potential was recorded in the soma to analyze the effects
of temperature on transfer resistance, defined as
Rt =
Vsoma/Idend
(Fig. 8D). By
comparing this measure in the two temperatures, we can obtain a direct
indication of the change in effectiveness at the soma of the same (synaptic)
current at its source, the dendrite. Comparing the slopes of the resulting V/I
plots at the two temperatures shows a clear increase in
Rt from 53 k
at 18°Cto85k
at
8°C (Fig. 8E). The
60% increase in Rt is consistent with the
50100% increase in
.
Taken together, the physiological results are consistent with the notion
that cooling increases the input resistance (Rin) in the
M-cell, and thus the same synaptic conductance change should produce larger
responses in the cold than in the warm. A good example of this effect is the
antidromic action potential, which is generated at the axon hillock and is
often larger in the cold at both recording sites compared with 18°C
(Fig. 8B,C).
Theoretically, the same sound-evoked dendritic PSP should be more effective at
the soma in the cold than in the warm in bringing the M-cell to threshold, and
this change in cable properties might also compensate for any reduction in the
synaptic coupling potential and excitatory conductance change.
To test this hypothesis functionally we measured the input resistance,
Rin, and M-cell excitability in the warm and cold
(n = 2) using two intrasomatic electrodes, for simultaneous voltage
recording and current injection (Fig.
9A). Cooling to 8°C increased Rin
by
120% and decreased the threshold current by more than half compared
with 18°C (Fig.
9B,C, top). Similarly, when a sound-evoked PSP was paired
with a current pulse, the added current needed to bring the M-cell to
threshold dropped by more then half with cooling
(Fig. 9B,C, bottom).
This indirect method of measuring threshold at different temperatures was
necessary because even with the maximum sound intensities (104 dB) the evoked
PSP was not sufficient to bring the M-cell to threshold at either temperature
in the electrophysiological studies. This might be attributable to an effect
of electrode penetration that likely decreases input resistance and thus
increases the threshold current in the M-cell, as well as to the use of an
anesthetized preparation. In addition, sound stimuli in air provide only the
pressure component of an auditory stimulus and lack the particle acceleration
component present when using underwater stimulation
(Popper and Fay, 1993
,
Casagrand et al., 1999
), which
could explain why even less-intense auditory stimuli were sufficient to elicit
a C-start in the behavioral experiments.

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Figure 9. Temperature dependence of the M-cell input resistance
(Rin). A, The cell was penetrated with two
intrasomatic electrodes for simultaneous potential recording and current
injection at two different temperatures (top). The resemblance of the two
sound-evoked PSPs indicates a close proximity of the electrodes (bottom,
18°C). B, M-cell action potential evoked, at threshold either by
a 91 nA depolarizing current pulse alone (top) or by a 66 nA current pulse
paired with a sound-evoked PSP (bottom) at 18°C. C, Same
threshold conditions at 8°C as in B, but with either a 41 nA
depolarizing current pulse alone (top) or by a 28 nA current pulse paired with
a sound-evoked PSP (bottom). The recorded sound stimuli (300 Hz, 75 dB) have
the same time scale as recordings. Note that cooling increases
Rin and lowers the threshold current.
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In addition to their monosynaptic excitation of the M-cell, auditory
afferents also activate a feedforward inhibitory network that regulates the
excitability of the neuron (Faber and
Korn, 1978
, Faber et al.,
1991
, Oda et al.,
1998
). A distinct sensitivity of cerebellar inhibitory circuits to
cooling has been shown previously in goldfish
(Friedlander et al., 1976
),
and experiments (n = 3) were performed to determine whether changes
in temperature also affect the M-cell inhibitory system and, thus, escape
responsiveness. In the M-cell, inhibitory responses are not associated with
frank potential changes, because unless the cell is experimentally loaded with
Cl, the IPSP equilibrium potential is close to the resting
potential (Faber and Korn,
1978
). Thus, the inhibitory synaptic conductance
(GIPSP) can be calculated from measurements of the
reduction (shunt) in the amplitude of a passively conducted test antidromic
action potential after the activation of the feedforward inhibitory network
(Fig. 10A). That is,
GIPSP = r/(1
r)Gm, where r is the fractional
reduction in spike height and Gm is the M-cell input
conductance (Faber and Korn,
1982
), which may change with the experimental condition. In our
experiments we recorded the time course of GIPSP at 8 and
18°C by stimulating the feedforward inhibitory network with a sound
stimulus (PSP) (Fig.
10A,B) followed by an antidromic test stimulus at
progressively longer time intervals ranging from 0.5 to 30 msec. The result of
a representative experiment, shown in
Figure 10B, indicates
that cooling markedly decreased the magnitude and onset of
GIPSP compared with warming
(Fig. 10B, middle).
In addition, the rise time of GIPSP increased in the cold,
with the consequence that the time window between the onset of a sound-evoked
PSP and the time of the peak inhibition is approximately twice as long in cold
as in warm (Fig.
10B). It should be noted that the magnitude of
GIPSP is expressed as a fraction of the input conductance
(Faber and Korn, 1982
), which
is also decreased by cooling. Thus, the reduction in the inhibitory
conductance is actually greater than suggested in
Figure 10B.
 |
Discussion
|
|---|
Temperature-induced changes of neuron properties and behavioral
responsiveness
The effects of acute temperature changes on the escape behavior of goldfish
and on the basic biophysical properties of the M-cell and its synaptic inputs
can provide insights about the mechanisms that may underlie the proper
expression of this behavior. Multiple mechanisms combine to increase M-cell
responsiveness to sound at lower temperatures. First, the input resistance of
the M-cell increased, so that weaker synaptic conductance changes yielded
dendritic responses comparable with those at the warmer temperature. Second,
the cable properties in the lateral dendrite were altered by cooling, as
indicated by a longer space constant and a reduced centripetal attenuation of
a given dendritic input. Third, cooling decreased the magnitude and delayed
the onset of feedforward inhibition of the M-cell. These cellular mechanisms
combine to explain the behavioral observation that C-starts are more easily
elicited in fish at colder temperatures, and they might serve to compensate
for the reduced or more sluggish execution of a vital response. Behavioral
hyperexcitability caused by acute cooling has been shown previously in
goldfish together with indications of a distinct temperature sensitivity of
cerebellar inhibitory interneurons
(Friedlander et al., 1976
).
Acute cooling also increases the escape jetting performance and the firing
rate in the squid giant and nongiant fiber pathways, and a
temperature-dependent reduction of central inhibition has been suggested as
the likely mechanism (Neumeister et al.,
2000
). In addition, the effects of temperature on membrane
properties, synaptic gain, and conduction delays, and their possible
implications for behavioral performance, are well documented
(Prosser and Nelson, 1981
;
Montgomery and MacDonald,
1990
). In the M-cell system, factors contributing to an increased
behavioral responsiveness may be correlated with acute behavioral compensation
for the negative effects on motor performance and directionality. For example,
the observed lowering of the escape threshold could effectively increase the
distance at which flight from an attacking predator is triggered in nature.
Indeed, such an inverse relationship between flight distance and temperature
has been described for lizards (Rand, 1964). In this context, it is
interesting to note that acute warming or heat shock has been shown to
increase the vulnerability of fish to predator attack
(Webb and Zhang, 1994
;
Yocom and Edsall, 1974
),
suggesting that warming increases the threshold in the M-cell system and
decreases escape responsiveness. This would confirm the specific sensitivity
of the M-cell system to acute temperature shifts and underlines the
significance of temperature for nervous system function and behavior
(Montgomery and MacDonald,
1990
).
The temperature-dependent changes in M-cell input resistance and dendritic
space constant are most likely caused by a reduction in resting K+
conductance. The M-cell membrane potential, which did not change with
temperature, was typically at approximately 78 mV, suggesting that the
membrane is close to the K+ equilibrium potential
(Faber and Korn, 1978
), and
Na+ and Cl conductances are quite low at rest. In
confirmation, neither Cl loading nor pharmacologically
blocking inhibition have detectable effects on M-cell membrane potential or
input conductance (Faber and Korn,
1988
). Moreover, the distinct broadening of the antidromic action
potential at 8°C (Figs. 7,
8,
9) is consistent with a greater
temperature sensitivity of currents underlying spike repolarization: namely, a
delayed onset and decreased magnitude of voltage-dependent potassium
conductance and/or slower inactivation kinetics of sodium channels
(Frankenhaeuser and Moore,
1963
, Klee et al.,
1974
). A similar spike broadening in the eighth-nerve afferents,
combined with the increased M-cell time constant caused by the doubling of the
input resistance, would account for the slower onset and prolonged duration of
the sound-evoked coupling potential in the cold. Comparable thermal
dependencies of excitable cells have been described for invertebrates
(Hodgkin and Katz, 1949
;
Winter, 1973
) and vertebrates
(Volgushev et al., 2000
). In
some other systems cooling also led to a depolarization of the cell membrane,
which we did not observe. In this context our results are comparable with the
temperature sensitivity of squid giant axon, which exhibits a similar increase
of spike duration with cooling, but no change in membrane potential between 5
and 20°C (Hodgkin and Katz,
1949
).
Temperature-induced effects on escape directionality
In addition to the increased behavioral responsiveness, other aspects of
the C-start also showed distinct temperature sensitivities that may be
correlated with electrophysiological changes in the M-cells and their
associated networks. There was a significant increase in apparent directional
errors in the cold environment, namely an increase in responses toward the
stimulus instead of away from it and a distinct increase in inappropriate
responses into the tank wall. In other words, cooling affects the directional
decision-making process underlying the escape. Although the neurobiological
mechanism by which the M-cell system solves the directional discrimination
task for an underwater auditory stimulus is not yet fully understood
(Popper and Fay, 1993
;
Eaton et al., 1995
,
Casagrand et al., 1999
), it
seems clear that the initial turn away from the stimulus is decided by a
single action potential in either the left or right M-cell
(Zottoli, 1977
;
Eaton et al., 1991
). Because
of its role as an all-or-none initiator of the response, the M-cell should
have a high firing threshold to avoid frequent and inappropriate responses.
The requirement for an instantaneous yet directional response, on the other
hand, would imply that a given stimulus brings both M-cells close to threshold
and that only a small bias of sensory-evoked excitation and/or inhibition in
the system determines which of the two M-cells reaches threshold. Indeed, the
firing threshold of the M-cell is relatively high (1520 mV above the
resting potential), and interactions between auditory-evoked excitatory and
inhibitory inputs (Faber and Korn,
1978
; Zottoli and Faber,
1980
; Oda et al.,
1998
) determine whether an M-cell reaches that point. Furthermore,
it has been suggested that an imbalance in the feedforward inhibition to the
two M-cells plays a role in determining escape direction
(Faber et al., 1991
;
Eaton et al., 1995
;
Hatta and Korn, 1999
). Our
physiological results showed that cooling lowered the behavioral threshold for
spike initiation in the M-cell, presumably because of the effects of an
increased membrane resistance; at the same time cooling delayed the onset and
magnitude of feedforward inhibition. Thus, the temporal window was broadened
during which the decision to respond is reached and the escape direction is
selected. These changes in the balance between the relative magnitude and
timing of excitation and inhibition in the system with cooling shifted the
directionality of the response to almost the level of chance, by bringing both
M-cells closer to threshold and at the same time reducing the proposed
discriminatory role of inhibition.
Temperature effects on motor performance
All of the kinematic parameters measured in this study show significant
slowing of C-start motor performance at 8°C compared with those recorded
at 18°C (Figs. 2,
3,
4). Similar effects of acute
cooling on escape motor performance have been described for goldfish and other
fish species (Webb, 1978b
;
Temple and Johnston, 1997
;
Johnson et al., 1998
). The
slowing is primarily attributable to an increase in the duration of the
propulsion stage, with corresponding reduced peak COM velocity and
acceleration values. The prolonged propulsion stage led to over-rotation and
thus had a direct influence on the escape trajectory and turning angle.
However, the initial C-start formation appears less affected by acute cooling
and shows similar velocity and acceleration values at both temperatures.
Although the C-start formation is closely correlated to the all-or-none
activity of one of the M-cells (Nissanov
and Eaton, 1989
), the more flexible and graded propulsion stage is
thought to involve other reticulospinal neurons
(Nissanov et al., 1990
). Thus,
the similarities in the kinematics of C-start formation would be consistent
with the idea that the M-cells triggered the responses studied at both
temperatures. This notion is also supported by the fact that the probability
of eliciting a C-start was significantly increased in the cold
(Fig. 6), because ablation of
the M-cells has been shown to decrease escape probability
(Zottoli et al., 1999
). In
addition, the C-start latency at 18°C was comparable with that reported
previously (Eaton et al.,
1977
).
C-start latency, measured as the time from stimulus onset to C-start
formation, increased, on average, by 15.8 msec with cooling
(Fig. 4). The physiological
results showed that this increment was distributed throughout the different
stages of the escape network; however, most of the increase appears to be
related to muscle activation. Table
1 dissects the C-start latency into its successive components,
namely presensory processing time from sound to PSP onset, M-cell processing
time, M-axon conduction time, time to muscle EMG activity, and muscle
contraction time. Our electrophysiological data on the first three components
indicate that the major source of the increased latency in the cold is caused
by slowing of muscle activation by
13 msec. However, equally important is
that the sensory and M-cell processing time are each increased by
100%.
This increase in the time allowed to reach a decision to respond and select
its direction is one consequence of coordinated changes in the network and
intrinsic M-cell properties that combine to support behavioral
hyperexcitability in the cold. More generally, our results suggest that both
the relative magnitudes of excitation and inhibition and their timing may
determine the expression of a behavior and its modification.
 |
Footnotes
|
|---|
Received Mar. 4, 2003;
revised Apr. 7, 2003;
accepted Apr. 9, 2003.
This work was supported by National Institutes of Health Grant NS 15335. We
thank Princess E. Osei-Bonsu for excellent technical assistance with the
behavioral experiments, Kamran Khodakhah and Alberto Pereda for comments on
this manuscript, and Haftan Eckholdt for help with the statistical
analysis.
Correspondence should be addressed to Dr. Thomas Preuss, Department of
Neuroscience, Albert Einstein College of Medicine of Yeshiva University, 1300
Morris Park Avenue, Bronx, NY 10461.E-mail:
tpreuss{at}aecom.yu.edu
Copyright © 2003 Society for Neuroscience
0270-6474/03/235617-10$15.00/0
 |
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