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The Journal of Neuroscience, January 15, 2000, 20(2):626-638
Switching Off and On of Synaptic Sites at
Aplysia Sensorimotor Synapses
Sebastien
Royer,
Rosalind L.
Coulson, and
Marc
Klein
Clinical Research Institute of Montreal and University of Montreal,
Centre de Recherches en Sciences Neurologiques, Montreal, Quebec H2W
1R7, Canada
 |
ABSTRACT |
Using the highly plastic synapses between mechanoreceptor sensory
neurons and siphon motor neurons of Aplysia as a model, we have investigated whether switching off and on of individual synaptic release sites is a strategy that is used by neurons in forms
of short-term synaptic modulation with a time course of minutes to
hours. We have modified some of the techniques of classical quantal
analysis and examined the kinetics of synaptic depression under
different stimulation protocols to answer this question. Our analysis
shows that both synaptic depression caused by homosynaptic activity and
synaptic facilitation induced by an endogenous facilitatory transmitter
occur by means of the shutting off and turning on, respectively, of
synaptic sites, without intermediate changes in the probability of
release. Our findings imply that other forms of plasticity at these
synapses, such as post-tetanic potentiation, long-term facilitation,
and long-term potentiation, are also expressed by all-or-none changes
in activity at individual sites. We thus show that in addition to the
mechanisms of synaptic integration that are known to operate in single
cells and networks, neurons can exercise a further layer of fine
control, at the level of individual release sites.
Key words:
synaptic transmission; synaptic plasticity; synaptic
depression; synaptic facilitation; transmitter release; quantal
analysis; miniature synaptic potentials
 |
INTRODUCTION |
Synaptic phenomena such as long-term
potentiation and depression represent cellular mechanisms that may
contribute to learning (McKernan and Shinnick-Gallagher, 1997
; Murphy
and Glanzman, 1997
; Rogan et al., 1997
), as do short-term
processes such as homosynaptic depression and heterosynaptic
facilitation (Zucker, 1972
; Byrne et al., 1993
; Cohen et al., 1997
).
Although detailed mechanistic explanations for these phenomena are
lacking, evidence has been marshalled for such general possibilities as
changes in the probability of neurotransmitter release (Bolshakov and
Siegelbaum, 1994
; Stevens and Wang, 1994
) or the insertion or
activation of postsynaptic receptors (Isaac et al., 1995
; Liao et al.,
1995
). Other studies have reported that some synapses release no
neurotransmitter initially but can be recruited by various treatments
(Wojtowicz et al., 1991
; Charpier et al., 1995
; Wang et al., 1996
). We
have taken advantage of the favorable properties of sensorimotor
synapses of Aplysia to examine whether shifting of synapses
into and out of the active pool occurs in short-term synaptic plasticity.
Modulation of sensorimotor transmission in Aplysia
contributes to changes in its responsiveness to tactile stimulation
(Carew et al., 1983
; Walters and Byrne, 1983
; Byrne et al., 1993
;
Stopfer and Carew, 1996
; Cohen et al., 1997
). Homosynaptic depression is a progressive decline in transmitter release that occurs even at low
stimulation frequency (Castellucci and Kandel, 1974
). Heterosynaptic facilitation is the increase in transmitter release, mediated by
facilitatory transmitters such as serotonin (5HT), that follows a noxious stimulus (Brunelli et al., 1976
; Castellucci and Kandel, 1976
; Abrams et al., 1984
). These and other forms of synaptic modulation in the intact nervous system can be reconstituted in cultures with a single sensory neuron contacting a single motor neuron
(Schacher et al., 1990
; Klein, 1993
, 1994
; Lin and Glanzman, 1994
). Reconstitution in culture facilitates quantal analysis by
permitting unequivocal identification of the source of synaptic input
(Dale and Kandel, 1990
; Eliot et al., 1994
). We present here an
analysis of homosynaptic depression and 5HT-induced facilitation beginning with synapses in cell culture and then extending the analysis
to intact ganglia.
Our analysis consists of two parts. In the first part, we use a
modified quantal analysis to distinguish between graded changes at
synapses and selective, all-or-none switching between release states.
In the second part, we support our conclusion of all-or-none switching
by examining the kinetics of synaptic depression and recovery with
various stimulation protocols.
Our results show that the connection between a sensory neuron and a
motor neuron comprises more than one subpopulation of synapses. One
group of synapses undergoes rapid depression and facilitation. These
synapses respond once or a few times to a presynaptic impulse and fully
recover the ability to transmit only after several hours of rest; they
can, however, be rapidly reactivated by tetanization or the
introduction of facilitatory neurotransmitters. A second subpopulation
transmits stably and is less affected by modulatory treatments. The
third subpopulation is silent until recruited by facilitatory
treatments. We conclude that short-term plasticity in this system is
achieved through all-or-none switching off and on of individual sites
of synaptic transmission.
 |
MATERIALS AND METHODS |
Preparation. Adult Aplysia californica
(75
150 gm; Marine Specimens Unlimited, Pacific Palisades, CA, and
Alacrity Marine Biological Services, Redondo Beach, CA) were
anesthetized by injection of 50
100 ml of 385 mM
(isotonic) MgCl2. For recordings in ganglia, abdominal ganglia were extracted, pinned to the bottom of dishes coated
with Sylgard, and desheathed in a high magnesium solution [1:1
isotonic MgCl2 to artificial seawater (ASW),
composition given below]. For cultures, tail sensory neurons (Walters
et al., 1983
) and siphon motor neurons [LFS neurons (Frost and
Kandel, 1995
] were isolated and maintained as previously described
(Klein, 1994
; Coulson and Klein, 1997
). Sensory and motor neurons were maintained in separate Petri dishes at room temperature (21
24°C) in
10% Aplysia hemolymph in Leibovitz L15 culture medium (Life Technologies, Grand Island, NY) supplemented with salts (Schacher and
Proshansky, 1983
). Under these conditions, the neurons retract their
processes and become spherical in shape after 1
3 d. A single sensory
neuron was then manipulated into contact with each motor neuron, and
the pairs were left to incubate at least 1 d, by which time the
EPSP amplitude has reached a plateau (Coulson and Klein, 1997
).
Electrophysiological recording. An Axoclamp 2A amplifier
(Axon Instruments) and borosilicate glass micropipettes (tip resistance 10
20 M
) filled with 2 M potassium acetate, pH 7.5, were used for intracellular recordings. In some experiments on cultured synapses, the presynaptic electrode was filled with 2 M
potassium chloride. Recordings were performed in ASW [(in
mM): 460 NaCl, 10 KCl, 11 CaCl2, 55 MgCl2, and 10 HEPES, pH 7.5] or in high calcium solution [in mM) 368 NaCl, 8 KCl, 80 CaCl2, 48 MgCl2, and 10 HEPES, pH 7.5] in experiments on cultured synapses and in high
divalent cation solution [(in mM): 368 NaCl, 8 KCl, 14 CaCl2, 114 MgCl2, and 10 HEPES, pH 7.5] (Trudeau and Castellucci, 1992
) in most of the
experiments on intact ganglia. Postsynaptic neurons were LFS siphon
motor neurons in all experiments both in ganglia and in cultures.
In experiments examining the kinetics of synaptic depression and
recovery, impalements were performed in zero calcium solution (identical to ASW except for substitution of
MgCl2 for CaCl2) to avoid
transmitter release on impalement of the presynaptic neuron, and then
ASW or high calcium solution was perfused into the experimental
chamber. In some of the experiments examining the kinetics of
depression and recovery from depression, CNQX (6
20 µM)
was added to reduce the EPSP amplitudes and thereby avoid activation of
voltage-dependent currents. CNQX was used in the kinetic experiments
because the complete time course of depression had to include the very
first EPSPs in the experiment, and these could be as large as 50 or 60 mV without the blocker. In the quantal analysis experiments, in
contrast, the analysis was begun only after the initial rapid phase of
synaptic depression had already taken place, and CNQX was therefore not necessary.
Neuron type was confirmed by the response to release of hyperpolarizing
current (Eliot et al., 1994
). Throughout the experiments, the sensory
neuron was held at
50 mV, and the LFS motor neuron was hyperpolarized
to
80 mV in current clamp mode. Slow perfusion (~1 ml/min) was
maintained during the whole experiment for recordings in ganglia and
was turned on during rests in experiments on cultures. Serotonin [(10
µM) creatinine sulfate, 5HT; Sigma, St. Louis, MO) was
perfused into the chamber during rests from stimulation.
Data acquisition and analysis. Experiments were recorded on
a MacIntosh IIVX computer using the Axodata program (Axon Instruments), and EPSP amplitudes were measured with the Axograph program (Axon Instruments). EPSP amplitudes were measured by subtracting the average
of a 3 msec period at the base of the EPSP from the average of a 3 msec
period centered on the peak of the EPSP (Redman, 1990
). The variance of
the noise was determined by taking the difference between the averages
of two 3 msec periods separated by the same interval as that between
the baseline and the peak EPSP periods. In two experiments, an
electrical component (<0.5 mV) that persisted in the presence of
cadmium was observed and subtracted from the postsynaptic potential.
Data files were transferred to Microsoft Excel (version 7) and GraphPad
Prism (version 2) for analysis and plotting.
Quantal analysis and estimation of p and n. The
quantal amplitude, q, was determined from the asynchronous
release elicited by application of a hypertonic sucrose solution (250 or 500 mM sucrose in ASW) to the cultures. The
distribution of miniature amplitudes was skewed to the right, as has
been reported for other synapses (Bekkers et al., 1990
; Frerking and
Wilson, 1996
) and could be well fit by an equation based on a Gaussian
distribution of synaptic vesicle diameters (Bekkers et al., 1990
). The
mean mini amplitude in 20 cultures ranged from 0.35 to 1.42 mV (mean 0.717 ± 0.272 SD), with a coefficient of variation
(cv) that ranged from 0.52 to 0.99 (mean 0.699 ± 0.125 SD).
To fit the amplitude distributions of the evoked PSPs, the mini
distribution was convolved against itself n-1 times and
against the noise to obtain distributions resulting from the
simultaneous release of n quanta. The height of each of the
n components was then scaled so that the ensemble of the
respective areas was appropriate for any given value of p,
and the derived distribution that gave the best fit to the distribution
of the evoked PSPs (determined by minimizing the
2) was used to estimate the
experimental p and n. The goodness of fit was
determined from calculation of the
2
with the number of degrees of freedom equal to the number of bins minus
3. This method of fitting histograms of experimental data does not
depend on the presence of discrete peaks in the evoked amplitude distribution.
The second method we used for estimating p involves
calculation of p from the ratio of the variance to the mean
of the PSP with corrections for the noise and the quantal variance (see
next paragraph).
Quantal variance can arise from two sources: variability of the quantal
amplitude at each site (intrasite variability) as well as variability
between sites (intersite variability). The general expression relating
p to the mean and variance of the PSP includes terms for the
quantal cv that take into account the source of the quantal
variability:
|
(1)
|
[from Eq. 18 of Frerking and Wilson (1996)
, modified by
dividing the numerator and denominator of their left-hand term by µm2, the square of
the quantal amplitude in their notation] where V and
M are the variance and the mean of the PSP, q is
the quantal amplitude, cv is the coefficient of variation of
the quantal amplitude, and W is the fraction (which can
range from 0 to 1) of the quantal variance that originates from
intrasite variability. The two extreme cases occur when all of the
variability is either intrasite or intersite. When all of the
variability is within-site (W = 1), the expression for
p is:
|
(2)
|
and when all the variability is between-site (W = 0) the expression is:
|
(3)
|
For experiments in which we used mini amplitudes to estimate the
quantal parameters, we expressed the EPSP in terms of the quantal
content, m, where m = M/q.
Because the EPSP decreases with repeated stimulation as a result of
homosynaptic depression, we also devised a method for estimating
p for a progressively changing EPSP that we have called "sliding p." In this method, p is calculated from the
mean and the variance of the EPSP for successive groups of five evoked responses, moving one response at a time, using the above expressions (for an example see Fig. 5A,B).
Although the use of such small sample sizes would be expected to give
rise to a large scatter in successive estimates of p, any
overall trend in p in a given experiment should still be detectable.
To test the reliability of this method of estimating p, we
applied this analysis to 15 sets of simulated EPSP amplitudes for which
the slope of synaptic depression was similar to that observed in our
experiments (see Fig. 6A, broken line). We
then generated sets of parameters n and p such
that the monotonic decline in the simulated EPSP was attributable to
changes in n or p, or both. We generated 10 sets
of 15 simulated experiments for each of five combinations of changes in
n and p, where the rate of change of p
ranged from 0 to 100% of the rate of change of the quantal content, m. Specifically, we simulated homosynaptic depression which
was caused by changes only in p, only in n,
equally in p and n, or a combination of changes
in p and n such that one changed three times more
than the other. We then plotted the estimates of the changes in
p from the sliding p calculations against the
relative proportion of the simulated depression attributable to a
change in p (see Fig. 6A). In addition, we
examined the relation between p and m across all
the simulated experiments for each of the different conditions (see
Fig. 6B). The results indicate that this method yields estimates of p that are in excellent agreement with
the values given in the simulations. This method of estimating
p is very sensitive to changes in p, so that an
overall change in p in a simulation could be detected even
when as little as 25% of the change in the simulated response was
caused by a change in p.
To compare the change in the EPSP amplitude with the change in
p in our experiments, we normalized the slopes of the
respective regression lines by dividing by the y-intercept
(see Fig. 5B) and plotted the normalized slope of sliding
p against the normalized slope of sliding m (see
Fig. 5C).
In experiments for which we had no direct measurements of the quantal
amplitude and variance, we used the sliding value of V/M as an indication of whether p was
changing with synaptic depression and facilitation. This procedure is
justified by the fact that as long as the quantal amplitude and
variance remain constant, changes in the ratio of V to
M reflect changes in p according to the above
equations, independent of the source of the quantal variability. We
verified that the quantal parameters were unchanged by applying
hypertonic sucrose twice and comparing the mean amplitude and
cv of the miniature potentials elicited with each
application (see Results).
Except where noted otherwise, statistical comparisons were performed
using Student's t test. All the analysis programs were run
using Microsoft Excel.
Analysis of recovery from synaptic depression. Recovery from
depression was measured after 1, 3, or 10 stimuli. Ratios of the EPSPs
after rest to the first EPSPs of the experiments were plotted against
their respective rest intervals (0.5, 10, 30, 60, 120, and 300 sec) and
then fitted with a single exponential using Prism software (see Fig.
7). Cells were impaled in calcium-free medium to avoid transmitter
release during impalement. After introducing normal ASW medium, the
sensory neuron was stimulated 1, 3, or 10 times with an interstimulus
interval of 30 sec, and the test measurement to a single stimulus was
made after one of the rest intervals listed above. Each pair of cells
was used for only one measurement.
Modeling of kinetics of synaptic depression and recovery. A
given pair of neurons was used for only one experiment; averages therefore represent data taken from several pairs of neurons.
Homosynaptic depression was modeled assuming that each site releases
one quantum of neurotransmitter with a constant probability p and then recovers the ability to transmit with a time
constant
. An expression for the EPSP amplitude was derived that
takes into account sites that have released and have not yet recovered, sites that have released and recovered, and sites that have not released at all to previous stimuli. The expression was derived as follows.
The amplitude of the first EPSP of an experiment,
A1, is equal to the product of the
probability of release, p, and a maximal amplitude,
A0, proportional to the total number
of sites initially available for release:
At the time of the second stimulus, the EPSP consists of two
components: (1) a component contributed by sites that had not released
with the first stimulus, equal to
p(A0)(1
p) or
p(A1/p)(1
p), and (2) a component contributed by sites that had
released with the first stimulus and have recovered the ability to
release by the time of the second stimulus:
where
t is the interstimulus interval and
is
the time constant of recovery.
The amplitude of the second EPSP will then be:
At the third stimulus, the amplitude contributed by sites that
had not released with the second stimulus is:
The sites that have recovered the ability to release by time of
the third stimulus will include some sites that had released with the
second stimulus as well as some that had released with the first
stimulus but had not recovered by the time of the second stimulus,
resulting in a contribution of:
The amplitude of the third EPSP will then be:
The general expression for the EPSP is:
|
(4)
|
where Am is the amplitude of
the EPSP at the mth stimulus and
t is the
interstimulus interval.
We modified this expression to take into account the fact that each
stimulus also results in the shutting off of a fraction of the sites
that have released, as we demonstrate in Results. To account for our
data (see discussion of Figs. 7-9 in Results), we posited that the
fraction of sites that drops out with each stimulus declines
exponentially from an initial value
with a time constant
Z (expressed in terms of the number of stimuli), until a
steady state is reached in which a portion of the total number of sites
continues to release according to Equation 4.
Thus, the expression for the EPSP when switching off of sites is taken
into consideration is:
|
(5)
|
Starting with this expression, different models were implemented
by varying some of the parameters, as described in the text.
Minimization of the sum of the squared differences was used to fit the
different models to experimental data using Microsoft Excel.
 |
RESULTS |
In a series of experiments aimed at examining the time course of
the development of synaptic transmission and the potential for synaptic
regulation at Aplysia sensorimotor synapses in cell culture
(Coulson and Klein, 1997
), we observed a number of synaptic pairs that
showed extremely little variation in the evoked EPSP after the initial
homosynaptic depression (Fig. 1). In 14 of 50 experiments, the coefficient of variation of the depressed EPSP (estimated quantal content 2.37 ± 1.49 SD) was <0.35, and in
five of these it was <0.25. The small variability of the EPSP in
combination with the low quantal content suggests that release in the
steady state reflected the activity of a small number of sites
transmitting with a high probability. This observation is not
consistent with the idea that homosynaptic depression proceeds by a
gradual decrease in the probability of release at all release sites
equally, but suggests rather that individual sites are turned off while
other sites remain active.

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Figure 1.
Small variability of depressed EPSPs and large
facilitation by 5HT. Records of successive groups of monosynaptic
potentials from a sensorimotor pair in culture
(A) and plot of the whole experiment
(B). C, Magnified
view of EPSPs 4-15 showing the small variation in amplitude.
Stimulation was interrupted for 5 min after EPSP 15, and two more EPSPs
(data not shown) were elicited before addition of 5HT. The
interstimulus interval was 30 sec. Calibration bars: A,
2 mV, 10 msec; C, 1 mV, 10 msec.
|
|
The possibility that release at individual sites is controlled in an
all-or-none manner is supported by the facilitation of transmission. In
the same study, we reported some pairs that showed no evoked release
before addition of the endogenous facilitatory transmitter 5HT, with
clearly detectable responses afterward, indicating the presence of
inactive synapses that were recruited in synaptic facilitation. In
addition, in experiments like that of Figure 1, the EPSP increased
many-fold in amplitude on application of 5HT, despite the small amount
of variability in the EPSP before facilitation. This observation too
suggests the presence of a population of synaptic release sites that
contributes little or nothing to the depressed EPSP and is then
recruited on application of 5HT. The results collectively suggest that
homosynaptic depression as well as 5HT-induced facilitation proceed by
means of a switching off and on of individual release sites rather than
by a graded change in their release properties. The purpose of the
following analysis is to test this hypothesis in a quantitative manner.
Amplitude and amplitude distribution of quantal
synaptic potentials
We have modified the techniques of cell culture in
Aplysia to enable us to form soma-to-soma synapses (Klein,
1994
) (see Materials and Methods), which have two further important
advantages for quantal analysis. First, the electrical distance from
the recording site to the site of synaptic action is short, thus
reducing problems associated with electrotonic distortion of the shapes
of synaptic potentials, as well as the likelihood of
conduc- tion block at branch points of presynaptic neurites.
Second, such cultures form physiological synapses progressively during
the 12-15 hr after pairing and therefore permit the examination of the
properties of small numbers of synaptic sites in early cultures. We
have shown (Coulson and Klein, 1997
) that short-term synaptic
modulation is present at the earliest times after synapse formation and
that, with the exception of the amplitude of the synaptic potentials, the early synapses do not differ significantly in their properties from
later synapses or from synapses formed using the conventional culture
configuration. Finally, further facilitating quantal analysis, we use
as the postsynaptic elements at these synapses small siphon motor
neurons [LFS neurons (Frost and Kandel, 1995
)] in which the quantal
synaptic potential is often large relative to the recording noise,
sometimes reaching an amplitude of 2 or 3 mV or more.
We determined the quantal amplitude by eliciting asynchronous release
with hypertonic sucrose (Materials and Methods). Because it has been
proposed that the transmitter release caused by exposure to hypertonic
solutions is independent of calcium (Dale and Kandel, 1990
; Rosenmund
and Stevens, 1996
), the possibility arises that different pools of
transmitter might be mobilized by depolarization-induced calcium entry
and by hypertonic sucrose. If this were the case, it would not be
appropriate to use the quantal parameters derived from sucrose
applications to analyze release evoked with action potentials. To
address the possibility that the quantal amplitude q as
determined from application of sucrose might differ from that elicited
by depolarization and calcium entry, we compared the amplitude and
variance of minis elicited with sucrose with those of the minis
elicited with a weak depolarization of the presynaptic neuron in the
same pair of neurons. There was no difference between the mean values
of the miniature amplitude using these two methods of eliciting
asynchronous release (Table 1). Although the coefficients of variation of the miniature distributions were not
identical, the cv of the minis elicited with sucrose
differed from that of the minis elicited with depolarization by <7%
on average (Table 1).
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Table 1.
Comparison of miniature postsynaptic potentials elicited by
application of hypertonic sucrose and by weak depolarization of the
presynaptic neuron
|
|
The amplitude distribution of EPSPs evoked with action potentials
at sensorimotor synapses is consistent with a binomial model of
transmitter release
If switching between release states occurs, and if release behaves
as a binomial process, then quantal analysis should reveal that both
synaptic depression and facilitation are accompanied by changes in the
apparent number of release sites, or the binomial parameter
n, rather than by a change in the apparent probability of
release, or binomial p.
Quantal analysis requires that a sufficient number of synaptic
responses be recorded under steady-state conditions. Because the
synaptic processes that we were interested in analyzing involve changes
in the average amplitude of the synaptic response over time, it is
generally not possible to perform this kind of analysis on whole
experiments. We therefore limit the first part of our analysis to
periods during which the response remains fairly stationary, after the
major part of homosynaptic depression has already taken place. In all
of these experiments we used the distribution of miniature EPSPs evoked
with hypertonic sucrose to estimate the mean and variance of the
quantal unit, and we constructed the theoretical curves of the evoked
responses by convolving the mini distribution against itself and
against the noise (see Materials and Methods). Figure
2A shows examples of
experiments with stationary stretches in which amplitude histograms
could be fit adequately using binomial parameters. In 13 of 15 experiments, the binomial model gave a satisfactory fit
(p > 0.05). We have also reanalyzed previously
published amplitude histograms that were originally fit using Poisson
statistics (Castellucci and Kandel, 1974
) and found that some of them
were fit significantly better by binomial statistics (data not
shown).

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Figure 2.
Binomial fits of amplitude distributions of
sensorimotor EPSPs. A, Examples of amplitude histograms
and fits. In each column the top and
bottom amplitude histograms represent miniature synaptic
potentials evoked with hypertonic sucrose and evoked EPSPs from the
same pair of cells, respectively. Fits (solid lines) to
the mini distributions were performed using Equation 1 of Bekkers et
al. (1990) ; fits to the EPSP distributions were performed on the
assumption that evoked release follows a binomial distribution based on
the quantal parameters derived from the mini distribution in the same
pair of cells. The broken lines represent the underlying
distributions of noise (peak at zero) and convolutions of the
uniquantal distribution that resulted in the best fits, characterized
by the binomial parameters n and p shown
to the right of each graph. B,
C, Correlation between estimates of p
from histogram fits and from calculations. B, Estimates
of p derived from Equations 2 (all quantal variability
intrasite) and 3 (all quantal variability intersite) are plotted
against estimates of p from the best fits to histograms.
The line through the origin has a slope of 1, representing perfect agreement. C, Estimates of
p derived from Equation 1 (quantal variability
from both intrasite and intersite sources), with the fraction of
the total variability from intrasite variance equal to 0.65.
|
|
Although best fits to the amplitude histograms could be determined on
the basis of the
2 test (Materials and
Methods), other values of p and n could generally not be excluded because of the small number of events. Nevertheless, the fact that the fits were satisfactory indicates that these synapses
can be analyzed using a binomial model. To circumvent the problem posed
by the small number of responses available for amplitude histograms, we
took advantage of the fact that the binomial parameters p
and n can be calculated on the basis of the mean and the
variance of stretches of responses, as outlined in Materials and
Methods. Specifically, p can be calculated from the mean and the variance of the EPSP, together with the coefficient of variation of
the quantal unit (obtained from the distribution of the miniature amplitudes). As discussed in Materials and Methods, the source of the
variability in the quantal unit must be taken into account to make
these calculations. We initially calculated p based on the
two extreme cases, assuming that the quantal variability arises either
exclusively from within each release site (Eq. 2) or, alternatively, exclusively from between release sites (Eq. 3).
Before relying on calculated values of p, it is important
first to ensure that the parameters derived by calculation are
consistent with the amplitude distribution of the synaptic responses.
We therefore compared the calculated values with the p that
gave the best fit to the amplitude histogram in each case. As shown in
Figure 2B, the two ways of arriving at estimates of
p are in fair agreement.
The values of p calculated on the assumption that all of the
quantal variance is within-site are generally greater than the values
obtained from the histogram fits, whereas the p calculated on the assumption that all of the variance is between-site is generally
lower (Fig. 2B). This is to be expected if the
variance of the quantal amplitude is actually a composite of both
intrasite and intersite variability. We therefore looked for a
combination of the relative weights of the two kinds of variability
that would give a better match to the values obtained from the fits.
Using Equation 1, we found that a ratio in the weights of the intrasite to the intersite variability of ~0.65:0.35 gave a slope of 1 for the
line relating the calculated p to the p from the
fits, with an intercept close to zero (Fig. 2C) (correlation
coefficient 0.82, p < 0.0001). The values of
p obtained in this way were not different from those
obtained from the histogram fits (n = 15, t = 0.773, p = 0.452, paired
t test). The agreement between the two different ways of
estimating p supports the idea that transmission at these
synapses behaves according to a binomial model and justifies the use of
parameters derived from the calculations in examining the underlying
mechanisms of depression and facilitation.
It is not possible to determine from this kind of analysis whether the
parameter p represents a probability of release that is the
same for all release sites or a weighted average of different probabilities at different sites, with the higher probability sites
predominating. In the interests of simplicity, we will begin the
analysis assuming uniform p; nonetheless, as we will discuss below and at greater length in Discussion, our conclusions do not
depend on the assumption of uniformity in p across sites.
Estimation of p and n in stationary
experiments with known quantal parameters: synaptic depression cannot
be accounted for by a change in p
For the analysis of experiments with substantial stationary
periods, we took the estimates of p from the best fits and
from calculation using Equations 2 and 3 and compared these with the p that would be predicted if synaptic depression depended on
a change in p alone. For example, if the steady-state
depressed response was 20% of the first, undepressed EPSP of the
experiment, and if all the synapses contributed equally (uniform
p), then the p in the steady state would have to
be
0.2. We call this value "maximal p." If
p estimated from the binomial model was significantly
higher, this would indicate that the probability of release was
nonuniform, i.e., that a few high probability synapses were
contributing disproportionately to the overall response whereas other
synapses were releasing with a low probability. Depending on the
estimated value of p, it is possible to estimate how many of
the synapses are contributing significantly to the overall release and
whether others are effectively silent. In this way it is possible to
determine whether a uniform change in the probability of release can
account for synaptic depression and facilitation.
A summary of the estimated and the maximal p for all
experiments is shown in Figure 3. The
values of p obtained by fits or by calculation from the mean
and variance are much greater than the predicted maximal p
in practically all cases. This result implies that a change in a
uniform probability of release cannot account for synaptic
depression.

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Figure 3.
Comparison of derived p with
"maximal" p predicted from uniform decline in
p during homosynaptic depression. Binomial
p estimated from the best fit to amplitude histograms of
EPSPs (p fit) or from calculation
by Equations 2 (p intra) and 3 (p
inter) is generally much greater than that predicted if
homosynaptic depression were caused by a uniform decrease in
p at all release sites (maximal p).
Line has a slope of 1. See Results for definition of
maximal p.
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Examination of synaptic plasticity in stationary experiments
without known quantal parameters: synaptic depression and facilitation
are not associated with changes in p
In the next part of the analysis, we looked for changes in
p that might accompany synaptic plasticity in cases in which
we had no independent measures of the quantal amplitude and variance and there were two stationary periods between which the EPSP either depressed further as a result of continued stimulation or else facilitated as a result of application of 5HT. As can be seen from
Equation 1, the variance of the EPSP amplitude, V, divided by the mean, M, is linearly related to 1
p. As long as the quantal amplitude and cv and
the sources of quantal variability do not change between successive
episodes within an experiment (see below for evidence that the quantal
parameters are stable), any change in p will be reflected in
a change of the opposite sign in V/M, whereas if
p remains unchanged there will also be no change in V/M.
We observed no change in the ratio of the variance to the mean
and
therefore in p
on average, either with synaptic depression or with facilitation by 5HT (Fig. 4). In
29 experiments, the EPSP declined to 56 ± 18% of its earlier
amplitude with further depression (p < 0.001, paired t test), whereas the values of
V/M were 0.255 ± 0.249 with the initial
depression and 0.275 ± 0.231 after further depression
(p = 0.331, Wilcoxon signed rank test). On
application of 5HT in 10 experiments, the EPSP increased to 244 ± 101% of the pre-5HT amplitude (p < 0.001, paired t test), whereas V/M was
0.166 ± 148 before application of 5HT and 0.151 ± 0.110 afterward (p = 0.855, Wilcoxon signed rank
test). Thus, in neither synaptic depression nor facilitation is there a
change in p as calculated from the equations.

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Figure 4.
Absence of change in
p with synaptic depression or 5HT-induced
facilitation. EPSP amplitude (left) and ratio of the
variance to the mean (right) for stationary periods in
individual experiments (open circles) at earlier and
later times during progressive synaptic depression (29 experiments) and
before and after application of 5HT (10 experiments); filled
squares are means. Experiments on depression included 8 in
intact ganglia, 12 in cultures in normal ASW medium, and 9 in cultures
with high calcium medium. Because there was no difference among
the three groups, the results were pooled. Experiments with 5HT
included five in intact ganglia, three with normal ASW in culture, and
two with high calcium medium in culture. The absence of a change
in the average ratio of the variance to the mean in both
homosynaptic depression and 5HT-induced facilitation implies no change
in p.
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These conclusions hold only if the quantal amplitude and cv
do not change during an experiment. In agreement with reports by others
(Castellucci and Kandel, 1974
, 1976
; Dale and Kandel,1990
; Eliot et
al., 1994
), we found no change in the quantal parameters associated
with synaptic plasticity at these synapses. We examined the quantal
parameters derived from responses elicited by hypertonic sucrose both
before and after synaptic depression in four experiments and found no
change in either the quantal amplitude or the quantal cv
(before depression q = 0.748 ± 0.414 mV and
cv = 0.667 ± 0.140; after depression
q = 0.697 ± 0.418 mV and cv = 0.691 ± 0.124 afterward; p = 0.42 and 0.80 for
comparisons of amplitude and cv, respectively; paired
t test). We compared the mean and cv of the
miniatures in three experiments before and after application of 5HT and
found no significant differences (p = 0.69 and
0.44 for q and cv, respectively).
To test whether we could detect a change in V/M
when a change in p would be expected, we computed
V/M in experiments in culture in which we changed
the extracellular calcium concentration from the normal 11 mM to either 55 or 80 mM.
The mean V/M decreased (indicating an increase in
p) from 0.606 ± 0.565 in normal ASW to 0.276 ± 0.271 in high calcium (p = 0.016, Wilcoxon
signed rank test).
The apparent p obtained from calculations and histogram fits
could represent the combined contributions of different probabilities at different release sites, with the distribution of individual probabilities unknown. The apparent p in any one
measurement, therefore, may be a poor indication of the individual
probabilities. However, the only obvious way for the apparent
p to consistently remain unchanged in two measurements at
the same synapses in the face of a change in the quantal content is for
the contributions of the individual sites to increase or decrease to
the same extent at all sites, while the overall distribution of the
individual probabilities remains the same. It is possible in some cases
to find ad hoc combinations of p values for individual sites
that could yield the same apparent overall p for different
m, but there is no reason to suppose that these ad hoc
combinations of values for individual sites would be able to account
for a general and consistent finding of constant p despite
changing m. (This issue will be elaborated in Discussion).
There are two possibilities. Either apparent p reflects a
uniform probability of release at all contributing sites, and the
number of these sites changes, or else apparent p is the
result of a nonuniform distribution of individual probabilities that
does not change. The latter possibility implies that the number
of contributing sites goes up or down to the same extent for all sites,
independently of their respective individual probabilities. Both
possibilities necessitate the dropping out or recruitment of release
sites to account for synaptic depression and facilitation, respectively.
Analysis of nonstationary experiments: synaptic depression and
facilitation can be accounted for by changes in n
alone
Our observations in experiments with stationary periods in culture
led us to analyze experiments with larger numbers of responses both in
cultures and in intact ganglia to determine whether switching between
release states accounts for synaptic depression and facilitation generally. In most experiments on intact ganglia we used an
extracellular solution containing elevated concentrations of calcium
and magnesium ions to raise spike thresholds and thus to reduce or
eliminate any polysynaptic contribution to the EPSP. (We were also able to obtain apparent monosynaptic responses using normal seawater medium
in two cases.) This high divalent cation solution changes neither the
amplitude of the monosynaptic EPSPs from the sensory neurons nor the
kinetics of homosynaptic depression at the sensorimotor synapses
(Trudeau and Castellucci, 1992
). For synapses in culture, we used
artificial seawater with a high concentration of calcium in some of the
experiments (to increase the overall probability of release) and normal
seawater in the others.
To circumvent the problem of nonstationarity we used Equation 1 for the
analysis, as follows. For experiments in which we had estimates of the
quantal amplitude and cv based on asynchronous release
elicited with hypertonic sucrose, we computed sliding m and
sliding p as described in Materials and Methods. To compute sliding p, we assumed a ratio of 0.65:0.35 (Fig.
2C) in intrasite to intersite variability in the quantal
response. We then asked whether a decrease in p accompanied
synaptic depression.
After the initial rapid decline during the first few stimuli, further
synaptic depression is approximately linear (Fig.
5A). We compared the
normalized slopes of sliding m and sliding p for the linear portion of synaptic depression (ranging from 20 to 110 stimuli in different experiments) (Fig.
5A,B). There was no relation
between the normalized slopes of sliding m and of sliding p in individual experiments (Fig. 5C). Moreover,
the average slope of sliding p taken across all the
experiments was not significantly different from zero (
0.0044 ± 0.0247), whereas sliding m showed a consistent decline
(average slope
0.0113 ± 0.0097). Because experiments
with a low average p would have greater errors in calculation of p
which might obscure any underlying trend
in p
we also examined separately those experiments in which
the average p was >0.6 (seven of nine experiments) (Fig.
5C, open circles). The average slope of sliding
p was still not different from 0 (average slope positive,
0.0027 ± 0.0094). Finally, when we examined the slopes of sliding
p in individual experiments, it was either positive or not
significantly different from zero in eight of the nine cases. Thus,
because p does not change during synaptic depression, the
decline in the synaptic response is attributable to a reduction in
n. Once again, as noted in the previous section and in
Discussion, the possibility that the apparent p may reflect a nonuniform population of individual release probabilities does not
affect our conclusion that sites must be dropping out during depression.

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Figure 5.
Absence of change in sliding estimate of
p during homosynaptic depression. Plots in
A and B are from one experiment and
illustrate how the slopes of sliding m and
p were derived and normalized. Sliding p
(calculated from Eq. 1, with W = 0.65) and
m were determined for groups of five responses, moving
one response at a time. In A, the approximately linear
decline in sliding m was fit by linear regression, as
was the corresponding portion of the plot of sliding p.
B illustrates normalization of the slopes of sliding
m and p to permit direct comparison of
the slopes; the slopes were normalized by setting the respective
y-intercepts equal to 1. C is a plot of
the normalized slope of sliding p against the normalized
slope of sliding m in nine experiments on cultures in
normal ASW medium. The two filled circles represent
experiments in which the average p was ~0.3;
p in all of the other experiments was >0.6. The
line represents a slope of zero for sliding
p. D, For experiments without an
independent estimate of the quantal amplitude and variance, the
variance (V) and mean
(M) of the EPSP amplitude were used to
test for changes in p; no change in the ratio
V/M implies no change in p
(see Results). The line represents a slope of zero for
sliding V/M.
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For experiments in which we had no independent measure of the quantal
amplitude and cv, we performed a similar calculation, but
instead of computing sliding m and p, we used a
sliding estimate of M and V/M. We
compared the overall change in sliding V/M with the change in sliding M to determine whether the decrease in
the amplitude of the EPSP with synaptic depression was mirrored by an
increase in V/M, which would reflect a decrease
in p (Eq. 1). Because there was no obvious difference in the
rates of synaptic depression or in the slopes of sliding p
between synapses in intact ganglia and in soma-to-soma cultures, all
the results are presented together. Again, we saw no relation between
the decline in the EPSP amplitude and the normalized slope of
V/M (Fig. 5D). In 30 measurements
(14-66 stimuli), the average slope of sliding
V/M was 0.0016 ± 0.0217 (not different from
zero; t = 0.4, p > 0.6), whereas the
average slope of sliding M was
0.0222 ± 0.0116 (t = 10.48, p < 0.0001). In 24 of the
30 cases, the slope of sliding V/M was either
negative (indicating an increase in p) or not different from zero.
We used the same technique to determine whether facilitation by 5HT is
accompanied by an increase in p. In eight experiments, the
average values of sliding V/M before and after
5HT application were 0.115 ± 0.063 and 0.142 ± 0.077, respectively (p = 0.461, Wilcoxon signed rank
test), whereas the EPSP more than tripled in amplitude on average.
Thus, synaptic facilitation induced by 5HT, like synaptic depression,
is not accompanied by a change in p but can be accounted for
by an increase in the number of active synaptic sites.
As described in Materials and Methods, we tested the accuracy of the
method of sliding p by applying it to simulated data sets
with known n and p and found that the technique
could in fact detect changes in sliding p if they occurred
(Fig. 6). These simulations, together
with the decrease in sliding V/M that was associated with an increase in the extracellular calcium (above), indicate that our methods are capable of detecting both increases and
decreases in p.

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Figure 6.
Test of sliding p technique by
application to simulations with different contributions of declining
p to depression. A, Slope of calculated
sliding p as a function of different rates of decline in
p in simulations (n = 10 for each
condition). B, Slope of the relation between
p and m in simulations. The slope of this
relation varies with the contribution of declining p to
homosynaptic depression, ranging from close to 1 when all of the
depression is caused by a drop in p, to near 0 when
depression is attributable exclusively to a decline in
n. See Materials and Methods for details.
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A further conclusion from these experiments is that some release sites
are effectively silent even before undergoing synaptic depression. If
the probability of release remains constant during synaptic depression
and facilitation (see the next section for evidence that p
does not change even during the initial rapid phase of depression),
then a significant increase in the facilitated EPSP over the initial
EPSP implies the presence of inactive sites even before the induction
of homosynaptic depression (see Fig. 1 for example). Although we did
not perform experiments to examine directly other forms of plasticity,
our observation that p was high in many of the experiments
implies that other forms of synaptic facilitation at these
synapses
including frequency facilitation, post-tetanic potentiation,
and long-term potentiation
must also result primarily from increases
in the number of sites contributing to the overall synaptic response.
Kinetics of homosynaptic depression and recovery from depression:
synaptic sites switch between on and off states in an all-or-none
manner
A completely independent kind of analysis supports the idea that
homosynaptic depression is an all-or-none switching process. This
analysis involves examining the time course of recovery from depression. Recovery after a single stimulus takes place with a time
course consisting of a relatively rapid and an extremely slow phase.
The time constant of the rapid phase of recovery is on the order of
10-100 sec, whereas the slow recovery process is so slow as to be
unmeasurable out to at least 10 min. As the response depresses further
with additional stimulation, a progressively smaller fraction of the
initial response recovers with the fast time constant, and a
progressively larger fraction fails to recover (Fig.
7). This partial recovery is consistent
with the idea that only a portion of the synaptic sites recovers after
stimulation, with the rest remaining essentially inactive. In the
steady state, the active synaptic sites recover rapidly between stimuli
to the steady-state level, whereas the rest of the sites remain in the inactive state. Although the proportion of rapidly recovering sites
decreases with depression, the time constant of recovery does not
change significantly. This suggests the presence of only two pools of
synaptic sites, an "on" and an "off" pool, rather than a
continuously varying population.

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Figure 7.
Decline in recovery from depression with
progressive stimulation. Stimulation was stopped after 1, 3, or 10 stimuli in different experiments (each experiment was on a different
pair of cells), and recovery was examined by presenting a single
stimulus after 0.5, 10, 30, 60, 120, or 300 sec. Recovery relative to
the first EPSP of the experiment proceeds with an exponential time
course to a plateau that is below the level of the initial EPSP. The
plateau decreases with increasing number of stimuli, suggesting that an
increasing proportion of the sites is progressively switched off. Each
point is the average of four to seven separate experiments (error
bars indicate SD). The time constants of recovery based on the
exponential fits are 11.63, 20.11, and 40.03 sec after 1, 3, and 10 stimuli, respectively. Each of these values is within the 99%
confidence intervals of the other two.
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The graphs of Figure 7 also suggest that the proportion of sites that
drop out with each successive stimulus is not constant but rather
declines progressively. Thus, after one stimulus the EPSP has depressed
by ~29% (Fig. 7A). If the same amount of depression occurred with the second and third stimulus, then the recovery after
the third stimulus should be to only ~35% of the initial amplitude
rather than the 63% measured in Figure 7B, and recovery after the tenth stimulus (Fig. 7C) should be to ~3% of
the initial value. These calculations are conservative in that they
assume that all synaptic sites are subject to depression. If it is
assumed that some sites are not subject to depression, then the
discrepancy between the observed and the predicted depression is even greater.
A further indication that this switching model can account for synaptic
depression and facilitation comes from experiments in which the
depression run was interrupted by rests of varying duration, after
which stimulation was continued at either the same or a different
stimulation frequency. In these experiments we found that virtually all
aspects of the behavior of the responses were accurately predicted by a
model in which synapses do not undergo a graded change in their
properties but rather are subject to all-or-none switching off with
progressive stimulation (Eq. 4 and 5 in Materials and Methods).
The model was constructed as follows (see Materials and Methods for
more details). The first stimulus of an experiment causes release from
a fraction, equal to p, of the available release sites. Of
the sites that have released transmitter, some recover the ability to
release with a time constant
, whereas some switch into the off
state. The second stimulus then causes release from a fraction (again
equal to p) of the sites that had not released with the
first stimulus, as well as from the same fraction of sites that had
released to the first stimulus and had recovered by the time of the
second stimulus. The second stimulus also results in the switching off
of an additional fraction of sites. Release to subsequent stimuli is
treated analogously, with the provision that the fraction of sites that
switches into the off state decreases exponentially to zero. We allowed
both p and
, as well as the switching parameters
and
Z (Eq. 4 and 5 in Materials and Methods), to vary freely,
and, in addition, allowed p and
to change their values
during the course of a single experiment. The best fit of the predicted
values to the data was determined by minimizing the sum of the squared
errors (Table 2).
Using this model, we found that all of the responses of a given
experiment were best fit with constant values for p and
(Figs. 8A, 9) and that
values of
were in the same range as those measured in the recovery
experiments (i.e., on the order of tens of seconds). Synaptic
depression and recovery could not both be fit without introducing
switching into the model, whether
was kept constant, as would be
the case for a simple depletion model (Zucker and Bruner, 1977
; Liu and
Tsien, 1995
) (Fig. 8B), or allowed to increase
progressively, as might be the case if there were progressive depletion
of an upstream feeding pool of transmitter (von Gersdorff and Matthews,
1997
) (Fig. 8C). Not only was the initial decline well fit
with constant values for p and
, but the recovery after
rest and the time course of the subsequent decline were also accurately
predicted, whether the stimulation frequency was kept constant (Figs.
8A, 9A) or
changed (Fig. 9B). The only failure of the model to closely
fit the observed responses occurred when the rest was 10 sec or less
(Fig. 9A), presumably because frequency facilitation was
recruited at the short interstimulus intervals (Byrne, 1982
; Eliot et
al., 1994
).

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Figure 8.
Fits of homosynaptic depression and recovery
with a model incorporating switching off of release sites. Shown are
fits of a sample experiment with three different models of depression;
only the switching model fits both the kinetics of depression and
recovery after rest. Experiments were performed with interstimulus
intervals of 30 sec, with rests indicated by bars. For
the same experiment, EPSPs 1 to 15 were fit with three different models
(see Results for details). The solid curves for
stimuli 16 to 30 are predictions based on the parameters obtained from
best fits of stimuli 1 to 15 (Table 2). Only the model incorporating
switching off of synaptic sites is able both to fit the initial
depression and to predict the recovery and depression after rest.
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Figure 9.
A, Fits of depression and of
recovery after varying periods of rest with the switching model.
Experiments (circles) with 30 sec interstimulus
intervals and interspersed periods of rest of various durations were
fit with the switching model (solid and dashed
lines; see Table 2 for parameter values). Stimuli after 0.5 and
10 sec rests were followed by 60 and 50 sec rests, respectively, to
keep the average interstimulus interval constant. B,
Fits of experiments with changing interstimulus intervals. Each
plot represents a single experiment. The interstimulus
interval, initially 90 sec, was changed to 30 sec after 10 stimuli, as
indicated by the double lines. Rests after the first
EPSPs were 0.5 and 60 sec, respectively, and a second rest of 5 min was
introduced after EPSP 20 or 21. Fits are solid and
dashed lines. See Table 2 for parameter values that gave
the best fit.
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Of particular significance is the fact that both the initial rapid
phase of depression and the subsequent slow phase were well fit using
this model, indicating that the combination of recovery between stimuli
at some sites and the putative switching process can account for all
aspects of synaptic depression and that it is not necessary to invoke
two separate depression processes to account for the dual time course
of depression.
Another characteristic property of these synapses is that the EPSP
undergoes partial recovery with rest, but then declines back to the
previous steady-state level after only one or two stimuli. This
behavior too is accurately predicted by our model, simply as a
consequence of the fact that the rapidly recovering sites have enough
time to recover fully during the pause in the stimulation and then
revert to the steady-state level when stimulation is resumed at the
initial frequency. The synapses that had been switched into the
inactive state, on the other hand, do not recover appreciably if the
rest from stimulation is brief compared with the slow time constant of
recovery, which is on the order of hours.
Parameters
and
that gave the best fits (Table 2) were in
general agreement with those that could be independently estimated from
the experiments of Figure 7. Nonetheless,
, the fraction of sites
that drops out with each stimulus, tended to be smaller than the
depression to a single stimulus (Fig. 7A). Attempting to fit
the data without incorporating a progressive decline in
(i.e.,
without parameter Z; see Materials and Methods),
consistently yielded values for
and
that were greater and
smaller, respectively, than those used for the fits shown, and were
thus further from the values estimated from the experiments of Figure
7. Overall, the median
and
in 29 fits incorporating
Z were 82 msec and 0.13, respectively, whereas the median
values without Z were 124 msec and 0.07. In addition,
omitting Z led to a predicted depression that was
consistently greater than that observed (data not shown). We therefore
conclude that the fraction of sites that drops out with each stimulus
undergoes a progressive decline.
 |
DISCUSSION |
Our analysis indicates that synaptic depression and facilitation
involve switching of release sites between active and inactive states.
Entry into the inactive state is functionally equivalent to turning off
synaptic transmission, although it is difficult to distinguish between
a release probability of zero and very low, but non-zero, release
probabilities. Switching to the off state can occur with even a single
stimulus, and some sites are in the off state without previous
stimulation. Facilitation results from the switching on of synapses
that had been in the off state previously, whether they entered that
state as a result of homosynaptic depression or not. Interestingly, on
the basis of a completely different kind of analysis, it has been
proposed that 5HT increases synaptic transmission at neuromuscular
junctions of the crayfish by recruiting silent synapses (Wang and
Zucker, 1998
).
Synaptic facilitation by 5HT is mediated through two second-messenger
systems, those involving protein kinases A and C (Braha et al., 1990
;
Sacktor and Schwartz, 1990
; Ghirardi et al., 1992
; Sugita et al., 1992
;
Byrne et al., 1993
; Klein, 1993
). The biochemical cascades involving
these kinases act in different ways: PKA facilitates only synapses that
have not been severely depressed by previous stimulation, whereas PKC
enhances release even at depressed synapses (Braha et al., 1990
;
Ghirardi et al., 1992
; Klein, 1993
). Our analysis suggests that the two
kinases might differ in their ability to cause switching from the off
to the on release state, with PKC capable of inducing switching and PKA
able to increase release at active release sites but unable to cause
switching. This hypothesis implies that facilitation by PKA results
from an increase in p, which we did not observe with
facilitation by 5HT. However, in all of our experiments, 5HT was
applied to depressed synapses, where the contribution of PKA would be
minimal (Klein, 1993
). This hypothesis predicts that PKA would be
relatively ineffective at synapses with high p, a prediction
that could be tested by changing the extracellular calcium
concentration, for example.
Nonuniformity of p
One problem in attempting quantal analysis is the possibility that
p differs at different release sites (Hessler et al., 1993
; Rosenmund et al., 1993
). If the variance of p is
significant, the estimated p will be higher than the
(unweighted) average probability of release, and the estimated
n will be lower than the actual number of sites (Del
Castillo and Katz, 1954
). It is therefore possible that an apparent
change in n with no change in p could result from
changes in the probability of release at some sites, without sites
dropping out completely or being recruited. Two considerations argue
against our results being attributable to this possibility. First, we
observe no overall change in p despite large decreases in
m during homosynaptic depression (Figs. 4, 5). Although any
single pair of values of m and p can be accounted for on the basis of a nonuniform p with the consequent
underestimate of n, there is no obvious way of accounting
for a constant p in the face of changing m by
altering the distribution of p across release sites. Because
sliding p was computed on the basis of its linear relation
with V/M (Eq. 1-3), constant p
necessitates that V/M remains constant. Another
way of expressing this condition is:
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|
where pi is the
probability of release at the ith site. The only general way
this condition is met is if the relative distribution of p
at all sites remains the same, i.e., if the same proportion of sites
drops out for all values of p. If p is
nonuniform, this leads to the interesting conclusion that the shutting
off of a site is independent of release. This conclusion excludes all
depletion models. On the other hand, if p is uniform,
dropping out of sites may or may not depend on release.
A less general argument against the possibility that the apparent
change in n is the result of changes in nonuniform
p applies in a subset of our experiments. If the minimal
number of release sites is much greater than the estimated n
after synaptic depression, and, in addition, the estimated p
is high, the probability of release at a large proportion of the sites
must be close to zero (McLachlan, 1978
).
Studies of depression and facilitation at Aplysia
sensorimotor synapses
We find that the sensorimotor synapses undergo only
partial recovery with rest after as little as a single stimulus (Figs. 7-9). The amount of recovery in our experiments is comparable to that
reported by others both in intact ganglia (Walters and Byrne, 1985
;
Trudeau and Castellucci, 1992
; Nakanishi et al., 1997
) and in
conventional cultures using extracellular stimulation (Lin and
Glanzman, 1994
; Bao et al., 1997
). Five to 10 minutes
after one stimulus, the EPSP in the cultures averaged 0.78 of the
initial EPSP, after three stimuli it was 0.63, and after 8-10 stimuli it was 0.47. In intact ganglia, the EPSP averaged 0.80 after one stimulus, 0.64 after three stimuli, and 0.32 after 7-10 stimuli (only
two of the three studies in intact ganglia included more than six
stimuli). Our values (Fig. 7) were 0.72, 0.63, and 0.40, respectively.
All the analyses of depression and facilitation at Aplysia
sensorimotor synapses find that the quantal amplitude does not change
(Castellucci and Kandel, 1974
, 1976
; Dale and Kandel, 1990
; Eliot et
al., 1994
), a result that is commonly interpreted as indicating that
the changes in transmission result from changes in transmitter release.
Although it is theoretically possible for all of the postsynaptic
receptors at individual sites to be switched off and on as a unit, we
believe that the rapidity and reversibility of switching favors a
presynaptic locus of plasticity, as proposed in the earlier studies.
Other studies have examined the possible basis of homosynaptic
depression at these synapses. One report suggested that a progressive decrease in the amount of calcium entering the presynaptic terminals with each action potential might contribute to the depression of
release (Klein et al., 1980
). Because we find that changing external
calcium changes the probability of release, and repeated stimulation
does not, this mechanism appears unlikely.
Gingrich and Byrne (1985)
attempted to account for homosynaptic
depression as the depletion of a pool of transmitter whose refilling is
dependent on intracellular calcium. Their model could account for the
kinetics of depression as well as the effect of tetanization in
increasing transmission. However, this model could simulate the
recovery from a single depression run to only a limited extent
(Gingrich and Byrne, 1985
, their Fig. 3), and no attempt was made to
simulate subsequent bouts of homosynaptic depression.
In an ultrastructural study, Bailey and Chen (1988)
reported that
depletion of synaptic vesicles from the active zones accompanies homosynaptic depression, suggesting depletion of a releasable pool of
transmitter. In contrast, Eliot et al. (1994)
found that depression of
evoked transmission was not accompanied by a decrease in the frequency
of spontaneous release, suggesting to them that simple depletion of
vesicles from the active zones was not responsible for the depression
of the evoked responses.
We constructed our model on the assumption that switching off of
synapses occurs only after release, as would be the case for a
depletion model. However, as discussed earlier, our model does not
depend on this assumption. Our inference that some synapses are
inactive even in the absence of previous stimulation entails a
mechanism for the silencing of synapses that does not depend on
release. Furthermore, as discussed earlier, if p is not
uniform across release sites, our failure to observe a decrease in
p with synaptic depression implies that switching is
independent of release.
Distinct pools of synaptic sites
Although some synapses switch from an active to an inactive state
with repeated stimulation, a residual pool of synapses remains active
even after many stimuli. This difference among synapses suggests that a
single sensory neuron could express preferentially one or another type
of synapse with different targets. Synapses with different targets
could then show intrinsic quantitative or even qualitative differences
in synaptic transmission and plasticity, depending presumably on
interactions with the postsynaptic neuron (Davis and Murphey,
1994
).
Our findings indicate that the population of effectively transmitting
synapses is subject to rapid change and imply that changes in the
synaptic population are expressed in short-term learning processes. We
can suggest some possible advantages in being able to control
subpopulations of synapses in this manner. First, groups of synapses,
together with the behaviors they control, could be kept silent until
the appropriate circumstances call for their recruitment. In addition,
the switching of groups of release sites by a particular stimulus would
allow the nervous system to shape complex responses into the most
appropriate configurations for a given situation without the need for
the continued activation of dedicated modulatory pathways for small
groups of release sites. Switching of individual release sites thus
adds a layer of fine control to the mechanisms of integration known to
operate at the level of individual neurons and of neuronal assemblies.
 |
FOOTNOTES |
Received Oct. 4, 1999; accepted Nov. 4, 1999.
This work was supported in part by Grant OGP0138426 from the Natural
Sciences and Engineering Research Council of Canada and Grants MH 45397 and NS 36648 from the National Institutes of Health. We thank Harold
Atwood, Vincent Castellucci, Wayne Sossin, and Robert Zucker for their
helpful comments on earlier versions of this manuscript, Elisha Klein
for useful discussions, and Yali Zhao for help in data analysis.
Correspondence should be addressed to Dr. Marc Klein, Clinical Research
Institute of Montreal, 110 Pine Avenue West, Montreal, Quebec H2W 1R7,
Canada. E-mail: kleinm{at}ircm.qc.ca.
 |
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