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The Journal of Neuroscience, September 1, 1999, 19(17):7629-7639
Frequency-Dependent PSP Depression Contributes to Low-Pass
Temporal Filtering in Eigenmannia
Gary J.
Rose and
Eric S.
Fortune
Department of Biology, University of Utah, Salt Lake City, Utah
84112-0840
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ABSTRACT |
This study examined the contribution of frequency-dependent
short-term depression of PSP amplitude to low-pass temporal filtering in the weakly electric fish Eigenmannia. Behavioral and
neurophysiological methods were used. Decelerations of the electric
organ discharge frequency were measured in response to continuous and
discontinuous electrosensory stimuli. Decelerations were strongest
(median = 4.7 Hz; range, 3.5-5.9 Hz) at continuous beat rates of
~5 Hz and weakest (median = 0.4 Hz; range, 0.0-0.8 Hz) at beat
rates of 30 Hz. Gating 20 or 30 Hz stimuli at a rate of 5 Hz, however, elicited decelerations that were sixfold greater than that of continuous stimuli at these beat rates (median = 2.6 Hz; range, 2.0-4.7 Hz for 30 Hz). These results support the hypothesis that short-term processes enhance low-pass filtering by reducing responses to fast beat rates. This hypothesis was tested by recording
intracellularly the responses of 33 midbrain neurons to continuous and
discontinuous stimuli. Results indicate that short-term depression of
PSP amplitude primarily accounts for the steady-state low-pass
filtering of these neurons beyond that contributed by their passive and
active membrane properties. Previous results demonstrate that passive properties can contribute up to 7 dB of low-pass filtering; PSP depression can add up to an additional 12.5 dB (median = 4.5). PSP
depression increased in magnitude with stimulus frequency and showed a
prominent short-term component (t1 = 66 msec at 30 Hz). Initial PSP amplitude recovered fully after a gap of
150 msec for most neurons. Remarkably, recovery of PSP amplitude could be produced by inserting a brief low-temporal frequency component in
the stimulus.
Key words:
whole-cell patch; sensory processing; adaptation; torus
semicircularis; jamming avoidance response; synaptic depression; plasticity
 |
INTRODUCTION |
A fundamental function of sensory
systems is to extract biologically relevant information. Although in
many systems there is a good understanding of the stimulus selectivity
of sensory neurons in particular central regions, there is
comparatively little known about the mechanisms that are responsible
for generating these filtering properties.
The electrosensory system of the weakly electric fish
Eigenmannia is well suited for investigating how central
filters are generated. Behavioral and neurophysiological studies have
clearly identified the filtering and computational processes that
underlie electrosensory behaviors. One particularly well studied
behavior is the jamming avoidance response (JAR), which persists in
neurophysiological preparations. In the JAR, Eigenmannia
adjusts the frequency of its electric organ discharges (EODs) to avoid
detrimental interference from EODs of neighboring fish. When two fish
of similar EOD frequencies approach, the combination of their EODs
produce amplitude and phase modulations that can interfere with both
animals' ability to electrolocate (Matsubara and Heiligenberg, 1978
).
Modulations ("beat rates") of 3-8 Hz are most detrimental to
electrolocation and elicit the largest JARs (Bullock et al., 1972
;
Heiligenberg et al., 1978
; Partridge et al., 1981
; Bastian and Yuthas,
1984
), whereas beat rates of >20 Hz do not impair electrolocation.
During a JAR, the fish with the lower initial EOD frequency lowers its frequency while the other fish raises its frequency, thereby increasing the beat rate to values that have little effect on electrolocation.
These behavioral observations indicate that Eigenmannia
selectively extracts patterns of afferent activity that reflect slow modulations of signal amplitude. Selectivity for beat rates of 3-8 Hz
emerges at the midbrain (see Fig. 1B), where
most neurons respond poorly to rates of 20 Hz or more (Partridge et
al., 1981
). The rejection of fast temporal frequency information in the
torus is also found in the phylogenetically older ampullary
electrosensory system (Fortune and Rose, 1997a
). The mechanisms that
underlie the low-pass temporal-filtering properties of toral neurons
are incompletely understood.
Both passive and active membrane properties contribute to the low-pass
temporal-filtering characteristics of toral neurons (Fortune and Rose,
1997b
). Rarely, however, do passive and active membrane properties
account entirely for the filtering characteristics of toral neurons to
sensory stimuli. For these neurons, PSP amplitude declined by as much
as 20 dB as either the beat rate or the sinusoidal frequency of the
stimulus was varied from 2 to 30 Hz, even when the role of
voltage-dependent conductances was minimized.
In addition to active and passive membrane properties, frequency- and
time-dependent processes could, theoretically, contribute to the
temporal-filtering properties of neurons; synaptic depression (Zucker,
1989
) is one mechanism for achieving such attenuation. At stimulus
onset, PSP amplitude would be a function of a neuron's passive and
active membrane properties. As the high-frequency stimulus is
maintained, however, PSP amplitude might be attenuated until a steady
state is reached. This hypothesis was examined using both behavioral
and neurophysiological techniques. Results indicate that
frequency-dependent depression of PSP amplitude ("PSP depression")
enhances low-pass temporal filtering.
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MATERIALS AND METHODS |
Experimental procedures were similar to those described
previously (Heiligenberg and Rose, 1985
; Rose and Call, 1993
; Fortune and Rose, 1997a
,b
). Fish, ~1-year-old, of the genus
Eigenmannia were used. Animal husbandry, anesthesia, and
surgical procedures were performed under the guidelines established by
the Society for Neuroscience. For experiments, a fish's EOD was
measured and then attenuated (~1000 fold) by intramuscular injection
of Flaxedil (4 µg/gm of fish). Additional injections of Flaxedil were
made during the experiment as necessary to maintain the attenuation of
the EOD. The fish's EOD was replaced by a sinusoidal mimic (S1) that
was delivered through electrodes placed at the tail and in the mouth.
The amplitude and frequency of the S1 were adjusted to approximate the
fish's EOD before the injection of Flaxedil. Additional electrosensory
stimuli were delivered through an array of carbon electrodes that
surrounded the fish (Fig.
1A). In five fish,
behavioral experiments (see below) were performed under these
conditions before surgery.

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Figure 1.
Schematic diagrams of the stimulation apparatus
and ascending electrosensory pathways. A, A sinusoidal
mimic of the subject's EOD (S1) is presented through
electrodes placed at the tail and in the mouth. Jamming and other
signals (S2) can be presented through pairs of carbon
electrodes surrounding the fish and numbered 1-4 and
1'-4'. S2 signals also can be electronically
added to the S1 signal. B, Ampullary and
tuberous electrosensory systems have parallel projections. Ampullary
and P-type tuberous afferents project into the electrosensory lateral
line lobe, forming synapses on basilar pyramidal neurons and granule
neurons (small dots). Granule neurons in
turn have inhibitory synapses on nonbasilar pyramidal neurons. Basilar
and nonbasilar pyramidal neurons respond ~180° out-of-phase with
respect to the stimulus; they are known as E and I units, respectively.
In the tuberous system, E units respond to rises in stimulus amplitude,
and I units respond to decreases. Pyramidal neurons project into
various laminae in the dorsal torus semicircularis. Recordings were
made in layers 2-5.
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At the conclusion of the experiment, not >4 hr after the first neuron
was filled, animals were deeply anesthetized by the flow of 2% (w/v)
urethane across the gills. Animals were perfused transcardially with
saline-heparin solution followed by 4% (w/v) paraformaldehyde in 0.2 M phosphate buffer, pH 7.4. After perfusion, the brain was
removed and stored at 4°C overnight in the paraformaldehyde solution.
Sections, 100 µm thick, were cut on a vibratome and reacted using an
avidin-biotin peroxidase kit (Vector Laboratories, Burlingame, CA).
Sections were dehydrated, cleared in xylenes, mounted on slides, and coverslipped.
Behavioral procedures. After injection of Flaxedil, the
fish's EOD was replaced by a sinusoidal mimic (S1) that was delivered through electrodes placed at the tail and in the mouth (Fig.
1A). The residual EOD was recorded differentially via
a suction electrode fitted to the tail and amplified (model P15D; Grass
Instruments). EOD frequency was measured to an accuracy of 0.1 Hz using
a window discriminator (SA Instrumentation) and a frequency counter (BK 1822). The fish's resting EOD frequency, measured in the presence of
the S1 alone, was determined before and after each experimental stimulus was presented. EOD frequency was monitored until it reached a
stable level, usually >1 min for each stimulus. Water temperature was
held at 25°C.
Experimental stimuli were generated by electronically adding a second
sinusoidal signal (S2) to the S1. The frequency of the S2 was 1, 2, 5, 10, 20, or 30 Hz above or below the frequency of the S1 (Fig.
2A), which produces a
signal that "beats" at a rate equal to the frequency difference
between the S1 and S2. Two classes of experimental stimuli were used:
"continuous" and "discontinuous." For continuous experimental
stimuli, the S2 signal was presented and maintained until the fish had
reached a stable EOD frequency. Discontinuous stimuli were generated by
gating the S2 signal on and off at a rate of 5 Hz; the frequency of the S2 was 10, 20, or 30 Hz above or below the S1 frequency. The stimulus waveform that results from gating, at a rate of 5 Hz, an S2 that is 20 Hz greater than the S1 frequency is shown in Figure
2B. The starting phase of the S2 signals was adjusted
such that the amplitude of the combined (S1 + S2) signal started at the
amplitude of the S1 alone, thereby minimizing sharp transients in
stimulus amplitude.

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Figure 2.
Behavioral evidence of short-term PSP depression.
A, B, Oscillograms of continuous electrosensory stimuli
with beat rates of 5 Hz (A; top) and 20 Hz (A; bottom) and of a discontinuous stimulus with a
beat rate of 20 Hz that is gated at a rate of 5 Hz
(B). Responses to the stimulus in
B are the open symbols
above 20 Hz in C. Dashed vertical lines represent the time for a
full cycle at 5 Hz, 200 msec. C, Magnitude of EOD
decelerations versus the beat rate for continuous
(closed symbols) and discontinuous
(open symbols) stimuli. The magnitude of
responses was normalized for each fish to the maximum deceleration
evoked from that fish. Each symbol type--e.g., triangles,
diamonds represents data from an individual fish. The
solid line is the mean response across
fish to continuous stimuli. The dashed line is the mean for discontinuous stimuli.
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The added S1 and S2 signals were delivered through the electrodes in
the mouth and at the tail. This stimulus arrangement elicited
decelerations of the EOD frequency from its resting level (Takizawa et
al., 1999
).
Intracellular recording procedures. Whole-cell patch
recordings were made as described in detail by Rose and Fortune (1996)
. Intracellular recordings were made from 33 neurons in the dorsal 5 layers of the torus semicircularis of adult Eigenmannia
(Fig. 1B). Patch pipettes were constructed from
borosilicate or aluminosilicate capillary glass [1 mm outer diameter
and 0.58 mm inner diameter (#5960; A-M Systems); 1 mm outer
diameter and 0.75 mm inner diameter (#5810; A-M Systems),
respectively] using a Flaming-Brown type puller (model P-97; Sutter
Instruments). Electrodes were pulled to resistances between 10 and 25 M
. Electrode tips were backfilled with a solution (pH = 7.4;
285 mOsm.) consisting of (values in mM): 100 potassium acetate or potassium gluconate, 2 KCl, 1 MgCl2, 5 EGTA, 10 HEPES, 20 KOH, and 43 biocytin.
Biocytin was replaced by mannitol in the solution used to fill pipette
shanks. Electrodes were mounted in a Plexiglas holder with a pressure
port. This port allowed the application of pressure pulses (40-80
msec; 40 psi) from a Picospritzer (General Valve, Fairfield, NJ) or the manual application of suction or pressure from a 30 cc syringe. The
electrode was advanced in 1.5 µm steps (Burleigh 6000 microdrive) through the dorsal 5 layers of the torus. Responses were amplified using an electrometer (model 767; World Precision Instruments, Sarasota, FL) and stored on videotape at 40 kHz with 16-bit resolution (model 3000; Vetter Instruments).
Recordings generally were made at several levels of negative holding
current. This procedure permitted PSPs to be observed in the absence of
spiking and other fluctuations associated with voltage-dependent
conductances; generally less than
0.2 nA was used. As in previous
studies (Fortune and Rose, 1997a
,b
), these holding currents did not,
with the exception in some neurons of the all-or-nothing components of
EPSPs, affect the temporal-filtering properties of neurons. In
addition, in the present study no qualitative differences in short-term
PSP depression were observed over this range of holding currents.
Resting potentials were between
55 and
75 mV. At the conclusion of
each intracellular recording, neurons were filled with biocytin by
applying 1-2 nA of positive DC for 1-3 min.
Stimuli for intracellular recordings. The search stimulus
was designed to elicit responses from both ampullary and tuberous neurons in the torus. The ampullary component of the search stimulus was a linear frequency sweep (2-30 Hz; 10 sec duration; 1-2 mV/cm at
the fish's head) that was added to the S1 and presented through the
electrodes in the mouth and at the tail. The tuberous component was the
S1 and a sine wave (S2) 4 Hz higher than the S1 frequency that was
delivered concurrently through one pair of the array of carbon
electrodes surrounding the fish. The addition of the S2 generated
broad-field amplitude and phase modulations at a rate equal to the
difference in frequencies of the S1 and S2; the modulation frequency is
known as the beat rate.
After a recording was established, the best stimulus (ampullary or
tuberous) and stimulus orientation (pairs of carbon electrodes surrounding the fish) were determined. Stimulus orientation was chosen
to elicit the strongest and most consistent responses from the neuron.
Eighteen neurons were tuberous, and 15 were ampullary. The data here
and in previous reports (Fortune and Rose, 1997a
,b
) indicate that
ampullary and tuberous neurons in the torus are indistinguishable on
the basis of their temporal-filtering properties, appearance of their
PSPs, and anatomy.
Responses were first recorded while the stimulus frequency (ampullary)
or beat rate (tuberous) was linearly scanned from ~2 to 30 Hz. These
"sensory scans" were 10 sec in duration. Subsequently "sensory
bursts" were delivered; the stimulus frequency (ampullary) or beat
rate (tuberous) was held at 5, 10, 20, or 30 Hz. The bursts were 1 sec
in duration and presented at an interval of 2 sec. For tuberous
stimulation, the S2 was gated on at the zero-crossing of an S1 cycle,
and its starting phase was adjusted differentially for E-type and
I-type units. For neurons that were excited primarily by amplitude
increases (E units), the stimulus burst began with an amplitude
decrease; the opposite relation held for I units. This stimulation
paradigm was used so that the first PSP elicited by the stimulus burst
was in response to the same magnitude of amplitude modulation as
subsequent PSPs. For ampullary stimulus bursts, only a single
low-frequency signal was presented. The starting phase of the signal
was adjusted such that the first quarter cycle of stimulation did not
excite the neuron. Rarely neurons were encountered that had both strong
E and I components of their responses. These neurons were excluded from
the analyses presented in this paper.
The time course of recovery from PSP depression was assessed by
systematically reducing the interval between the end of one stimulus
burst and the beginning of the next burst ("gap duration"). Each
stimulus burst was 952 msec in duration except for those with gaps >48
msec; beyond 48 msec, gap duration was increased by decreasing the
burst duration. Within each burst the beat rate or sinusoidal frequency
was held at 20 Hz. The starting and ending phase of the stimuli was
adjusted for each cell such that PSPs were not evoked by the first and
last quarter cycles of the stimulus burst.
Finally, whenever possible, the sensory stimulus was removed, and a 0.1 nA peak-to-peak sinusoidal current sweep, 2-30 Hz, was injected into
the soma via the recording electrode. Constant-frequency current bursts
with a positive-going peak amplitude of 0.1 nA, a duration of 1 sec,
and intervals of 1 sec were also used. Burst frequencies were 5, 10, 20, and 30 Hz. Negative holding current was used to hyperpolarize the
neuron so that positive-going sinusoidal current injection, 0 to +0.1
nA, produced depolarizations in the neuron that were similar to EPSPs
elicited by sensory stimuli.
Analysis of neurophysiological data. As in previous studies
(Fortune and Rose, 1997b
), the temporal-filtering profiles of neurons
were determined by Fourier analysis of segments of the intracellular
responses to sensory and current scans. The peak of the power spectrum
near to the stimulus frequency was used as a measure of the amplitude
of stimulus-related PSPs at that frequency. In repeated measures of PSP
amplitude using this methodology, we found that the values varied by
less than ± 0.5 dB; each value represents an average of the
responses to several stimulus cycles. PSP depression was measured by
comparing the PSP amplitude as measured by Fourier analysis of
responses to the initial 100 msec segment of a burst with that to a
segment of identical duration at the end of the burst. In some cases
PSP depression was activated in <50 msec. In those cases the
peak-to-peak amplitude (in millivolts) of PSPs was measured at the
beginning (Vi) and end (Ve) of the burst. The ratio of these values was
taken and expressed in decibels: dB = 20 log (Ve/Vi).
For sinusoidal current injection data, the voltage drop attributable to
the access resistance (electrode and patch resistances) was subtracted
from the total voltages recorded. Access resistance was measured as the
first exponential component in the voltage response to square-wave
current injection. This value was subtracted from the individual
voltage values for particular stimulation rates. Decibel values were
computed using the corrected amplitudes.
 |
RESULTS |
Behavior
To assess the potential role of short-term depression in temporal
filtering, we compared EOD deceleration responses (Takizawa et al.,
1999
) of five fish with continuous and discontinuous electrosensory stimuli. Discontinuous stimuli were designed to reduce or eliminate the
contribution of short-term processes that require up to 100 msec for activation.
Continuous beat rates of 5 Hz (Fig. 2A) elicited the
greatest (up to 6 Hz) decelerations in EOD frequency (Fig.
2C, solid line, closed
symbols). Responses to beat rates of 20 Hz and above were
~1/10 the maximum magnitude. These data are similar to those obtained
in a previous report (Takizawa et al., 1999
).
Subsequently, stimuli of 10, 20, and 30 Hz beat rate were presented in
a discontinuous pattern, 100 msec bursts alternating with 100 msec gaps
(Fig. 2B). The effects of this stimulus regimen resembled a continuous 5 Hz beat rate stimulus in that, at least for
E-type tuberous electrosensory neurons (those responding to amplitude
increases), activity should be restricted to the 100 msec segments in
which the amplitude of the signal was modulated. Discontinuous stimuli
elicited responses that were up to sixfold stronger than the continuous
stimuli at high beat rates (Fig. 2C, dashed
line, open symbols). These responses
were, however, only 60-70% the amplitude of those to the continuous 5 Hz beat stimuli. These data suggest that short-term processes (e.g.,
short-term depression) contributed to the generation of low-pass
filtering in this behavior.
Intracellular physiology
Strong low- and bandpass temporal-filtering, neural correlates of
the behavioral responses to continuous stimuli are well developed at
the level of the torus. This conclusion is supported by data from
previous studies in which the stimulus beat rate was scanned linearly
from 2 to 30 Hz over 10 sec. The hypothesis that short-term processes
contribute to low-pass temporal-filtering properties of neurons was
tested by recording the responses of 33 low- and bandpass toral neurons
to continuous and discontinuous sensory stimuli.
Neurons were divided into two groups based on a combination of
physiological and anatomical properties (Fortune and Rose, 1997b
). The
first group included 26 neurons that had voltage responses to injection
of sinusoidal current that declined by at least 2.6 dB over the range
2-30 Hz and/or had large, complex dendritic arbors with many spines
("spiny neurons"). The second group included 7 neurons that had
voltage responses to injection of sinusoidal current that declined by
<2.0 dB and/or had small, simple dendritic arbors with few or no
spines ("aspiny neurons").
The temporal-filtering properties of these neurons were first assessed
by recording responses to continuous stimuli in which the beat rate or
frequency of the stimulus was swept linearly from 2 to 30 Hz over 10 sec (sensory scans). For this stimulus regimen, neurons showed low-pass
filtering ranging from approximately a 2 dB reduction in PSP amplitude
to almost 20 dB (median = 10.5 dB). Only aspiny neurons had
low-pass filtering of <5 dB. Both aspiny and spiny neurons were found
that showed low-pass filtering in the range of 5 to ~9 dB. Only spiny
neurons, however, showed low-pass filtering of >9 dB.
Evidence of short-term PSP depression
The role of short-term depression of PSP amplitude in low-pass and
bandpass temporal filtering was assessed by comparison of PSP amplitude
at the beginnings and ends of sensory bursts. In these stimuli, the
beat rate or frequency was held constant at 5, 10, 20, or 30 Hz for 1 sec and repeated at a rate of 0.5 Hz.
PSP depression, a form of short-term plasticity, is defined here as a
reduction in the amplitude of PSPs over time to a stimulus of constant
frequency or beat rate, e.g., adaptation. Alternatively, neurons could
produce constant-amplitude PSPs over time or could show an increase in
PSP amplitude (facilitation). Approximately 60% of low- and bandpass
neurons showed >3 dB short-term depression of PSP amplitude. This PSP
depression was frequency dependent, increasing in magnitude with
stimulation frequency.
Figures 3 and
4 show primary data from aspiny and spiny
neurons, respectively. Figures 3A and 4A
show examples of neurons with little or no evidence of PSP depression,
and Figures 3B and 4B show examples with
strong PSP depression. In the case of aspiny neurons, which are
characterized by having little passive low-pass filtering, PSP
depression primarily accounted for their low-pass filtering to sensory
stimuli. Aspiny neurons without appreciable PSP depression had weak
(<5 dB) low-pass filtering over 2-30 Hz. The bandpass neuron shown in
Figure 3A exhibited ~2 dB of passive low-pass filtering
and 2 dB of PSP depression. These contributions add to match the 4 dB
of filtering observed in response to the continuous sensory scan. The
lack of response to the lowest frequency beat rates is at present
unexplained but is likely to result from filtering properties of their
afferents from the electrosensory lateral line lobe (ELL) (see Shumway,
1989
). The large PSP after the high-frequency stimulus in Figure
3A is also currently unexplained; the presence of such PSPs
is not correlated with the strength of PSP depression.

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Figure 3.
Responses of aspiny neurons to stimulus bursts.
A, Neuron with little or no PSP depression.
B, Neuron with strong PSP depression.
Traces are responses to sensory bursts of 5 Hz
(top trace) and 30 Hz (bottom trace) beat
rates. The relative amplitudes of PSPs (in decibels) are plotted versus
stimulation rate. Responses are to sensory scans (beat rate swept
linearly from 2 to 30 Hz; thick lines),
sinusoidal current injection
(frequency swept linearly from 2 to 30 Hz;
open circles), and stimulus bursts
(closed squares). Values, in decibels,
are normalized to the maximum PSP amplitude for each stimulus
condition. For bursts, values are the differences in the magnitude of
initial PSPs and last PSPs of each burst. These values therefore are a
measurement of PSP depression. The dotted line with open diamonds
indicates the combined effects of passive electrical filtering (as
determined by injection of sinusoidal current) and PSP
depression.
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Figure 4.
Responses of spiny neurons to sensory bursts.
A, Neuron with little or no PSP depression.
B, Neuron with strong PSP depression. Figure components
are described in Figure 3.
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Data from an aspiny neuron that exhibited strong PSP depression is
shown in Figure 3B. The amplitude of the initial PSP to a
high-frequency stimulus was almost equal in amplitude to PSPs elicited
by low-frequency stimuli. Within five beat cycles, <150 msec, the
amplitude of PSPs declined by >7 dB. In aspiny neurons the magnitude
of PSP depression was up to 7.5 dB (Fig.
5, closed circles).

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Figure 5.
Relation between magnitudes of low-pass filtering
(measured from responses to sensory scans) and PSP depression (measured
from responses to sensory bursts). Solid lines are linear regressions for data from aspiny
(closed circles) and spiny
(open circles) neurons.
Dotted lines represent the hypothesis
that all low-pass filtering beyond that attributable to membrane
properties of the neuron is caused by PSP depression. The
closed square is a datum that was omitted
from the regression analysis.
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Spiny neurons showed 5-20 dB low-pass filtering. Spiny neurons with
relatively weak low-pass filtering (5-9 dB) generally responded to
sensory bursts with PSPs that diminished little over time; i.e., PSP
amplitude was relatively constant throughout the duration of both low-
and high-frequency bursts (Fig. 4A). Nonetheless, there was an appreciable decrease in PSP amplitude as stimulus frequency was raised from 5 to 30 Hz. Injection of sinusoidal current
revealed that the passive electrical properties of
these neurons accounted for up to ~7 dB of this low-pass filtering
(Fig. 4A).
In contrast, for spiny neurons with strong low-pass filtering, PSP
amplitude decreased dramatically from the beginning to the end of
sensory bursts when the beat rate was 20 Hz or more (Fig.
4B). For this case, PSP amplitude fell to
steady-state values within ~200 msec; the fluctuations of PSP
amplitude throughout the remainder of the stimulus may be a feature
resulting from the mechanisms underlying short-term PSP depression (see below).
The total magnitude of low-pass filtering can be seen by comparison of
the amplitudes of the last few PSPs of the high- and low-frequency
responses shown in Figure 4B. The passive filtering properties of this neuron, as determined by sinusoidal current injection, accounted for only ~4 dB of the low-pass sensory
filtering. The effect of passive filtering is evident in the amplitudes
of the first PSPs of both traces in Figure
4B; the initial response to the low beat rate
stimulus was almost 4 dB greater than the initial response to the high
beat rate stimulus. For a beat rate of 30 Hz, the magnitude of
short-term PSP depression was ~12 dB and can be seen by comparing the
amplitude of the initial PSPs with that of the last PSPs (Fig.
4B).
Thus, the passive electrical properties of spiny neurons accounted for
a maximum of ~7 dB of their low-pass filtering over the range 2-30
Hz. The additional low-pass filtering appeared to result from
frequency-dependent short-term depression of PSP amplitude (Fig.
4B). In spiny neurons short-term PSP depression had
magnitudes of up to 12.5 dB (range, 0-12.5 dB; median = 4.5 dB)
(Fig. 5, open circles).
Contribution of short-term depression of PSP amplitude to low- and
bandpass filtering
The intracellular data shown above suggest that, when the role of
active membrane properties was minimized by passing hyperpolarizing current, low-pass filtering of sensory information resulted from a
combination of the passive electrical properties of neurons and the
frequency-dependent short-term depression of PSP amplitude. The
hypothesis that PSP depression accounts for all low-pass filtering of
sensory information beyond that contributed by the neuron's passive
and active membrane properties was evaluated.
The passive electrical low-pass filtering of spiny and aspiny neurons
is significantly different (Fortune and Rose, 1997b
). Most aspiny
neurons show 1-2 dB of passive low-pass filtering, and most spiny
neurons have 5-6 dB, excluding the contribution of active membrane
properties (Fortune and Rose, 1997b
). If all additional low-pass
filtering is a result of short-term PSP depression, the relation
between total low-pass filtering and the magnitude of short-term PSP
depression should have a slope of 1 with an intercept between 1 and 2 dB for aspiny and between 5 and 6 dB for spiny neurons.
Linear regressions of aspiny and spiny neurons recorded in this study
(Fig. 5) have slopes near 1 (aspiny, slope = 1.07;
r = 0.98; n = 6; spiny, slope = 0.92; r = 0.97; n = 21). A slope of 1 indicates that for every additional decibel of filtering beyond the
contribution of passive filtering there is 1 dB of filtering caused by
short-term PSP depression. These correlations did not result from
systematic differences in PSP amplitude. There was no correlation of
PSP amplitude to the magnitude of PSP depression across neurons. In
this analysis one datum was excluded (Fig. 5, closed
square); this neuron showed strong low-pass filtering but
little PSP depression. It is likely that the afferents of this neuron
were low-pass I-type neurons from the centromedial map of the ELL
(Shumway, 1989
).
Time course of short-term depression of PSP amplitude
The mean time course and frequency dependence of PSP depression
(Fig. 6A) were analyzed
for 10 neurons. Sensory stimuli were either beating or sinusoidal
signals, and frequencies of 5 Hz (open squares),
10 Hz (closed squares), 20 Hz (closed
circles), and 30 Hz (open circles)
were used. For each neuron, PSP amplitude was normalized with respect
to the largest PSP. PSP depression was greatest at stimulation
frequencies of 30 Hz and minimal at 5 Hz. For frequencies of 20 and 30 Hz, these data were well fit (R2= 0.94 and 0.91, respectively) by double-exponential functions having first-order time
constants of 111 msec (20 Hz) and 66 msec (30 Hz) and second-order time
constants of 23 sec (20 Hz) and 3.1 sec (30 Hz). Thus, stimulation at
30 Hz elicited greater and faster PSP depression than did stimulation
at 20 Hz, even though initial PSPs were generally smaller for 30 Hz
stimulation.

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Figure 6.
A, Time course and frequency
dependence of PSP depression. PSPs were elicited by delivering sensory
stimuli 1 sec in duration at 2 sec interstimulus intervals. Frequencies
or beat rates of stimulation were 5 Hz (open squares), 10 Hz (closed squares), 20 Hz (closed circles), or 30 Hz (open circles). For each neuron, PSP amplitudes were
normalized with respect to the largest (mean) PSP recorded for each
stimulus condition. The time (x-axis) of occurrence of
the first PSP in response to the stimulus was designated as the 0 point. Means and SEs are plotted. B, Intracellular
recordings from an ampullary neuron. Top and
bottom traces are responses to 30 Hz
sinusoidal signals of ~1 and 0.5 mV/cm, respectively.
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Although these analyses clearly show that PSP depression has a strong
short-term component, they do not adequately represent the "fine
structure" of the time course of depression. In general, the pattern
of frequency-dependent short-term depression of PSP amplitude generally
resembled that of a damped oscillation. This feature was prominent in
stimuli with large amplitudes (compare top and
bottom traces in Fig. 6B). For
the larger stimulus amplitude (Fig. 6B, top trace),
PSP amplitude was largest at the beginning of sensory bursts and
declined to a minimum of 1-2 mV within ~250 msec and then rebounded
to 2-3 mV over the next 250 msec. This waxing and waning of PSP
amplitude continued as long as the stimulus was maintained. At the
lower stimulus amplitude (Fig. 6B, bottom trace), the
magnitude of the initial decline in PSP amplitude was reduced. Further
analysis of the time course of recovery from depression will be studied
in future experiments in which direct stimulation of the afferents to
toral neurons permits analysis with regard to the roles of specific
mechanisms for synaptic plasticity.
Time course of recovery from short-term depression of
PSP amplitude
The time course of recovery from PSP depression was studied for
six neurons. Segments of responses from a tuberous neuron and an
ampullary neuron are shown in Figure 7,
A and B, respectively. For the tuberous neuron,
initial PSP amplitude recovered fully after a gap equal to or greater
than ~28 msec. For a gap of 16 msec, the amplitude of the initial PSP
was 81% of control values, and the second PSP was smaller than those
during the last 100 msec of the burst. As the gap was increased from 16 to 48 msec, the amplitude of the second PSP increased threefold,
whereas the amplitude of the initial PSP was relatively constant. This
neuron had the fastest recovery that was observed. The time course of this fluctuation in PSP amplitude, however, is a function of the duration of the gap. For the ampullary neuron, the recovery of full
amplitude was not complete for gap durations of <48-100 msec. Although the time course of PSP depression was similar for these two
neurons when the gap was 48 msec, it differed for the shorter gaps; for
gaps of 8-20 msec, the second PSP of this ampullary neuron was
actually slightly larger than the first.

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Figure 7.
Effects of stimulus gaps on recovery from PSP
depression. Averaged segments of recordings from a tuberous
(A) and an ampullary (B)
neuron. Stimuli were continuous except for gaps, 8-48 msec in
duration, in which stimulus amplitude was held constant (tuberous) or
set to 0 (ampullary) at ~1 sec intervals. Stimulus beat rate or
frequency was 20 Hz. Neurons were current clamped at 0.1 nA.
Traces are the averaged responses to 4-8 repetitions of
the stimulus.
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All six neurons studied showed full recovery of initial PSP
amplitude for gaps >100-150 msec (median = 96 msec; range,
46-150 msec) (Fig. 8). However, as shown
above, the time course of PSP depression appeared to be a complex
function of the gap interval.

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Figure 8.
Time course of recovery from PSP depression.
Recovery values represent the ratio of the amplitude of the first PSP
after a stimulus gap of 8-200 msec to that of the first PSP after a
stimulus gap of 1 sec. Data are from six neurons. Open circles are measurements from the neurons shown in
Figure 7A. Open squares
are from Figure 7B.
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Other experiments revealed that recovery from PSP depression was not
simply a function of gap duration. Interestingly, when the phase of the
stimulus was adjusted such that the gap was an excitatory stimulus, a
PSP was produced, and the depression process was reversed (Fig.
9). In the case shown in Figure
9A, gaps of 8-48 msec were inserted in the rising phase of
stimulus amplitude. Because this was primarily an E-type neuron
(excited by amplitude rises), a PSP was elicited during the gap.
Remarkably, for excitatory gaps of 16 msec or greater, the next rise in
stimulus amplitude, at the beginning of the next burst, evoked a PSP
that was of the same amplitude as PSPs at the onset of a stimulus burst
after a 1 sec gap. This "resetting" of the depression process
occurred despite the fact that the PSP peaks were
50 msec apart
throughout the stimulation and gap periods.

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Figure 9.
Resetting of PSP depression by a low-temporal
frequency excitatory stimulus. A, Responses of an E-type
toral neuron to 20 Hz beat rate stimuli in which 8-48 msec
constant-amplitude segments were embedded. Holding current was 0.3
nA. B, Responses of an I-type toral neuron to 20 Hz beat
rate stimuli in which similar duration constant-amplitude segments were
embedded. Holding current was 0.1 nA.
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The recordings displayed in Figure 9B show a similar
resetting of PSP amplitude for an I unit. In this case, a decrease in stimulus amplitude was the effective stimulus, and the PSP during the
gap was broadened on its leading edge. In contrast to that in Figure
9A, the PSP elicited by the gap was, for gaps of 16 msec or
greater, of nearly full (nondepressed) amplitude. For gaps of 48 msec
or greater, the subsequent PSP was at full amplitude. For gap durations
of 16 and 28 msec, successive PSP peaks were not separated by >51 msec
throughout the stimuli. Also, throughout these stimulation periods the
membrane potential only briefly (<10 msec) remained near that seen
when the gaps were ineffective stimuli. When the opposite phase gap
configuration was used, such that gaps were inserted into the falling
(in this case ineffective) phase of stimulus amplitude (Fig.
7A), full recovery of PSP amplitude occurred only when ~70
msec separated the last PSP in response to a burst from the first PSP
in the next burst.
Finally, we determined whether postsynaptic fluctuations in the
membrane potential were sufficient to induce depression. Voltage fluctuations were produced by injecting constant-frequency bursts of
sinusoidal current (0.1 nA peak-to-peak; 1 sec duration). The temporal
composition of these bursts was identical to that of sensory bursts.
Injection of sinusoidal current bursts never elicited short-term
depression even in neurons that showed strong PSP depression to sensory
stimuli (Fig. 10). If depression
resulted from a time-dependent increase in conductance, the amplitude
of these fluctuations and the hyperpolarization induced by the
0.1 nA
holding current should decrease over time. These data show that PSP
depression does not simply result from postsynaptic conductance changes
in response to high-frequency fluctuations in the membrane
potential.

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Figure 10.
Current injection alone does not elicit PSP
depression. A, Evidence of PSP depression in this
neuron. The bottom trace shows 6 dB of
depression to 30 Hz beat rate sensory stimuli. B,
Responses to positive-going 0.1 nA sinusoidal current injection. Note
that the amplitude of these voltage fluctuations did not change
throughout the current injection stimuli. Holding current was 0.1
nA.
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DISCUSSION |
We examined the role that frequency-dependent short-term
depression of PSP amplitude plays in behaviorally relevant temporal filtering. The principle findings were that (1) fast beat rates were more effective in eliciting decelerations of the fish's EOD when
presented discontinuously (at a rate of 5 Hz) versus continuously and
(2) PSP depression primarily accounts for the low-pass
temporal-filtering characteristics of toral neurons beyond that
attributable to their passive and active membrane properties.
Behavioral considerations
Mechanisms for generating low-pass temporal filtering are only
adaptive if they do not preclude detection of slow changes in signal
amplitude that are concurrent with fast temporal fluctuations. An
important question, therefore, is whether processes for PSP depression
impede responses to slow changes in signal amplitude that are
concurrent with or directly follow fast AMs.
Rose et al. (1994)
showed that superimposing fast modulations onto slow
modulations did not attenuate the slow PSPs of low-pass toral neurons.
Because PSP depression was not measured in that study, the findings
suggest, but do not prove, that PSP depression does not preclude
response to low-temporal frequency information.
Remarkably, the present study shows that even a brief low-temporal
frequency component, e.g., maintaining constant signal amplitude
(peak-to-peak) for as little as 16 msec, could evoke large PSPs and
partially reset the sensitivity of the cell to fast fluctuations of
signal amplitude. In these cases the strong response that occurred at
or followed the low-temporal frequency component could not be
accounted for simply by recovery time; PSP depression could be reset
even when the interval between successive PSP peaks was ~50 msec or less.
With these findings in mind, PSP depression can be viewed from a
"learning perspective." By sampling several beat cycles, the system
evaluates the temporal frequency of the stimulus and, over time,
attenuates its responses if the temporal frequency is above a
particular value. This PSP depression process, a potential substrate of
habituation, can then be reversed either by a sufficient gap or by a
low-temporal frequency (sensitizing) component in the stimulus. This
process may permit fish, therefore, to habituate to the rapid
fluctuations in signal amplitude, such as those resulting from jamming,
while preserving its capacity to respond to slow modulations, as are
experienced during electrolocation of objects. This process may also
allow for the detection of the low-frequency components resulting from
"chirps," brief (up to ~100 msec) interruptions in a fish's EOD
pattern, that are involved in social communication. Importantly, this
neural dishabituation does not occur in response to any change in the
temporal pattern of the stimulus. For example, PSP depression develops
while the stimulus beat rate was changed slowly from 2 to 30 Hz.
PSP depression may also contribute to the determination of direction of
relative movement of images over the sensory array. In the
electrosensory system, as in mammalian visual systems, selectivity for
the direction of stimulus movement (Reid at al., 1991
; Jagadeesh et
al., 1993
) is seen at sites, or postsynaptic to sites, in the
respective pathways in which low-pass filtering and short-term,
frequency-dependent depression/adaptation are also found
[electrosensory system (Bastian, 1982
; Heiligenberg and Rose, 1987
);
visual system (Orban et al., 1985
)]. In visual cortex, short-term
synaptic depression, apparently because of presynaptic processes,
underlies their adaptation properties (Varela et al., 1997
). These
findings have led investigators to postulate that adaptation
(short-term synaptic depression) might be a mechanism for generating
shifts in the timing of peak responses resulting from stimulation of
particular sites on the body surface. These temporal shifts could be
used in directional selectivity (Jagadeesh et al., 1993
; Chance et al.,
1998
). This hypothesis could be tested in the electrosensory system by
determining whether neurons that show strong PSP depression respond in
a directionally selective manner to the motion of electric images.
Finally, measurements in this study of the "AM deceleration
response" (Takizawa et al., 1999
) for continuous 20 Hz beat stimuli versus 20 Hz beat stimuli that were gated at 5 Hz provide strong evidence that frequency-dependent short-term depression of PSP amplitude is an important component of the AM filter. The stimulus that
was gated on and off at a rate of 5 Hz elicited responses that were
approximately sixfold stronger than those for the continuous stimulus.
This result suggests that PSP depression greatly enhanced the rejection
of sustained high-temporal frequency signals. For 5 Hz-gated stimuli,
the magnitude of deceleration responses declined by ~30% as the beat
rate was changed from 10 to 30 Hz. This finding probably reflects the
role of passive filtering properties of toral neurons (Fortune and Rose
1997b
). Amplification of PSP amplitude, attributable to active membrane
properties, at low beat rates (5 Hz) may account for the slightly
larger deceleration response at 5 Hz, relative to that of the 10 Hz
stimulus that was gated at a rate of 5 Hz.
Evidence of gain control
The detailed time course of PSP depression suggests that it might
be appropriately viewed as a gain-control process. For fast temporal
frequencies, in many cases, PSP amplitude was largest for the first few
beat cycles, quickly decreased to its lowest values within the next 100 msec, and then increased to near steady-state values. That is, during
the initial segment of the burst stimulus, the short-term depression
process overshot its intended set point. With lower stimulus amplitudes
or depths of modulation, the degree of overshooting the set point was
less. This gain-control hypothesis should be explored further in future
studies by testing over a wider range of stimulus amplitudes or
modulation depths and durations.
Gain control has been demonstrated in the responses of ELL pyramidal
neurons to stepwise increases or decreases in stimulus amplitude and is
mediated by the negative feedback projection from the N. praeeminentialis to the ELL (Bastian, 1986a
,b
). This descending control
system, however, appears to reduce the responses of ELL pyramidal cells
to very slow beat rates but does not give rise to low-pass temporal
filtering; ELL cells showing strong gain control nevertheless respond
well to fast beat rates. This conclusion is also supported by the
minimal low-pass filtering exhibited by most ELL neurons for beat rates
up to ~20 Hz (Bastian, 1981
; Shumway, 1989
). It appears likely,
therefore, that the frequency-dependent PSP depression demonstrated in
the present study occurs in the torus.
Recovery from PSP depression seems to be a complex process. The gap in
stimulation that was required for full recovery of initial PSP
amplitude, i.e., amplitude of the first PSP after the gap, was in most
cases ~100-150 msec. With stimulus gaps of this magnitude, however,
the amplitude of the second and third PSPs was strongly depressed
relative to control values (PSPs of the same rank after a 1 sec gap).
This result is consistent with the idea that synaptic efficacy and
synaptic reserve are distinct and under separate regulation (Galarreta
and Hestrin, 1998
). The time course for full recovery of response
appears to be related to the duration of the stimulus and was not
investigated systematically in the present study. For a stimulus
duration of ~1 sec, a gap of 1 sec was sufficient for full recovery;
however additional work is needed to determine the relationships
between stimulus pattern, duration, and consequent recovery times.
Mechanism of short-term PSP depression
The frequency-dependent depression of PSP amplitude in the
responses of toral neurons could be caused by cellular or network properties or both. For example, frequency-dependent synaptic depression, as has been shown in the mammalian neocortex (Galarreta and
Hestrin, 1998
), could underlie the rapid decline in PSP amplitude at
stimulation frequencies of 20-30 Hz. In cortical slices,
frequency-dependent synaptic depression is strongest for excitatory
synapses. In the absence of negative current clamp, the
stimulus-related depolarizations in the current study, if of sufficient
amplitude, triggered spikes and therefore can be considered to be
primarily EPSPs. Frequency-dependent synaptic depression is believed to
be a presynaptic process (Torii et al., 1997
) and therefore should not
be influenced or elicited by postsynaptic manipulations.
The finding that high-frequency fluctuations of the membrane potential
induced by current injection did not affect changes in the biophysical
properties of neurons or PSP depression is consistent with this idea.
Also, holding neurons at levels of current clamp of
0.1 to
approximately
0.3 nA failed to alter the magnitude of PSP depression.
Holding currents of this magnitude translated to ~10-30 mV of
hyperpolarization and significantly influenced PSP amplitude.
Presynaptic mechanisms that could underlie frequency-dependent synaptic
depression include depletion of readily releasable vesicles or
decreased efficacy of release, possibly involving inactivation of
voltage-gated calcium currents (Forsythe et al., 1998
). Postsynaptic
receptor desensitization (Jones and Westbrook, 1996
) could also
contribute to frequency-dependent depression of PSP amplitude.
 |
FOOTNOTES |
Received April 19, 1999; revised June 10, 1999; accepted June 11, 1999.
This work was supported by National Science Foundation Grants
IBN-9421039 and IBN-91156789 and by National Institutes of Health Fellowship 1-F32 NS 09779.
Correspondence should be addressed to Dr. Gary J. Rose, Department of
Biology, University of Utah, 257 South 1400 East, Salt Lake City, UT
84112-0840.
 |
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