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The Journal of Neuroscience, August 1, 2001, 21(15):5781-5793
Synaptic Heterogeneity and Stimulus-Induced Modulation of
Depression in Central Synapses
John D.
Hunter1 and
John G.
Milton1, 2
1 Committee on Neurobiology and
2 Department of Neurology, Committee on Computational
Neuroscience, University of Chicago, Chicago, Illinois 60615
 |
ABSTRACT |
Short-term plasticity is a pervasive feature of synapses. Synapses
exhibit many forms of plasticity operating over a range of time scales.
We develop an optimization method that allows rapid characterization of
synapses with multiple time scales of facilitation and depression.
Investigation of paired neurons that are postsynaptic to the same
identified interneuron in the buccal ganglion of Aplysia
reveals that the responses of the two neurons differ in the magnitude
of synaptic depression. Also, for single neurons, prolonged stimulation
of the presynaptic neuron causes stimulus-induced increases in the
early phase of synaptic depression. These observations can be described
by a model that incorporates two availability factors, e.g., depletable
vesicle pools or desensitizing receptor populations, with different
time courses of recovery, and a single facilitation component. This
model accurately predicts the responses to novel stimuli. The source of
synaptic heterogeneity is identified with variations in the relative
sizes of the two availability factors, and the stimulus-induced
decrement in the early synaptic response is explained by a slowing of
the recovery rate of one of the availability factors. The synaptic
heterogeneity and stimulus-induced modifications in synaptic depression
observed here emphasize that synaptic efficacy depends on both the
individual properties of synapses and their past history.
Key words:
central cholinergic synapses; Aplysia; depletion; desensitization; availability; optimization; model; stimulus
history effects
 |
INTRODUCTION |
A principle site of information
transfer in the nervous system is the synapse between two neurons. The
synapse is not a passive, static conduit. Rather, it depends on its
past history and may change on a spike-by-spike basis (Byrne,
1982
; Dittman and Regehr, 1998
; Stevens
and Wesseling, 1998
; Gomis et al., 1999
;
Neves and Lagnado, 1999
). Consequently, mathematical
modeling techniques are increasingly used to help unravel the
complexity of the synapse (Zengel and Magleby, 1982
).
The necessity of using these techniques arises because a large number
of mechanisms act in concert (Zucker, 1989
). Moreover,
the relative importance of each mechanism can change with the
statistical properties of the input spike train, such as frequency and
patterning (Wiersma and Adams, 1950
; Gillary and
Kennedy, 1969
; Wachtel and Kandel, 1971
;
Brezina et al., 2000a
). Modeling approaches can be used,
for example, to quantify and localize the effects of modulators
(Cleland and Selverston, 1997
; Jorge-Rivera et
al., 1998
); to quantify how synapses change with development
(Hill and Jin, 1998
); to understand neuromuscular control (Brezina et al., 2000a
); to elucidate the role
of synaptic dynamics in cortical gain control (Abbott et al.,
1997
), computation (Chance et al., 1998
), and
network synchrony (Abarbanel et al., 1996
; Neiman
et al., 1999
; Bressloff, 1999
; Tsodyks et
al., 2000
); and to develop rapid, computer-based methods for
screening pharmacological compounds.
An important step in synaptic modeling was the application of random
spike trains to collect data (Krausz and Friesen, 1977
). Appropriately chosen random stimulus trains contain intervals at all
time scales, and thus the relevant processes need not be identified a
priori. The Volterra method is a powerful technique that has
traditionally been used to analyze data collected with random spike
trains (Ogura, 1972
; Krausz, 1975
;
Krausz and Friesen, 1977
). However, the disadvantages of
this method are that it is difficult to collect sufficient data
and difficult to interpret the results (Hung et al.,
1977
; Berger et al., 1988
; Sclabassi et
al., 1988
).
To address these difficulties, Sen et al. (1996)
introduced "synaptic decoding." Optimization techniques are used to
fit models based on synaptic physiology to data collected with random
spike trains. Although this model has worked well in a neuromuscular junction, it cannot describe synapses with depletion and hence has
limited applicability for the study of central synapses (Sen et
al., 1996
; Chance et al., 1998
; Dittman
and Regehr, 1998
).
Here we extend the Sen et al. (1996)
model to synapses
with multiple availability factors, using their optimization
methodology. The term "availability factor" describes a synaptic
component that decrements with each action potential, recovers with a
characteristic time course, and scales the response multiplicatively.
This generic term can encompass a depletable vesicle pool or a
desensitizing population of receptors. The extension was required
because we observed that the synaptic responses of central neurons of
Aplysia could not be adequately described by synaptic models
that lacked multiple availability factors.
The simultaneous IPSC responses of Aplysia neurons
postsynaptic to buccal interneuron B4/5 (Gardner, 1990
)
are described by a synaptic model that incorporated two availability
factors: one rapidly recovering and the other slowly recovering
(hereafter referred to as the rapid and slow factors). The observation
that two neurons respond differently to stimulation of B4/5 is
explained by differences in the magnitudes of the rapid and slow
factors. We also observed in single neurons that prolonged stimulation of B4/5 increases synaptic depression in subsequent stimuli. These changes are explained by an activity-dependent slowing of the recovery
of the rapid factor. Our results are consistent with the physiology of
acetylcholine receptor desensitization in Aplysia. This
suggests that the available factor model, closely related to the
classic depletion model (Abbott et al., 1997
;
O'Donovan and Rinzel, 1997
; Markram et al.,
1998
), may be successfully applied to receptor desensitization.
 |
MATERIALS AND METHODS |
Aplysia electrophysiology. Aplysia care and
dissection were performed as described in Church and Lloyd
(1994)
. The ganglion was constantly perfused with artificial
seawater with high divalent cations; perfusion solution concentrations
were (in mM): 286 NaCl, 165 MgCl2, 10 KCl, 33 CaCl2, and 5 NaHCO3. The high
divalent solution raises the threshold for neural firing and is
required to quiet intrinsic network activity while allowing for the
investigation of specific synapses (Gardner,
1986
, 1990
). Because the
high calcium may influence synaptic dynamics, we do not know whether
the observations discussed below would be seen in an intact animal in
normal physiological saline.
Recordings of the two postsynaptic neurons were made in two-electrode
voltage-clamp mode with two AxoClamp 2B amplifiers (Axon Instruments,
Foster City, CA) with electrode resistances
4 M
and a holding
potential of
50 mV. The electrodes were filled with 3 M
K-acetate, 30 mM KCl, and 0.1% Fast Green. The presynaptic interneuron B4/5 was stimulated to fire action potentials with 8-10
msec step current pulses of 100-250 nA using a Getting Model 5A
microelectrode amplifier (Getting Instruments, San Diego, CA) in
current-clamp mode. B4/5 can mediate pure inhibitory, pure excitatory,
or diphasic inhibitory/excitatory conductances depending on the
follower cell (Gardner and Kandel, 1977
). We restricted our investigations to pure inhibitory follower cells [identified as
B3, B6, B8, or B9 in Gardner and Kandel (1977)
].
Data were low-pass filtered at 1 kHz with a Frequency Devices 902 low-pass filter (Frequency Devices, Haverhill, MA) and digitally sampled at 2 kHz. All recording and stimulation protocols were automated using an AD2210 A/D board (Real Time Devices, State College,
PA) interfaced with a personal computer controlled by custom software
(Hunter et al., 1998
). We present data from a total of
seven neurons in three animals. The n = 46 stimulus
trains used here had lengths of 2-10 min, mean frequencies of 2-10
Hz, and an exponential, a uniform, or a Gaussian distribution of intervals.
Availability model. The model described below is motivated
by the model presented in Sen et al. (1996)
. In the
model presented there, the amplitude of the i-th event is
given by an arbitrary nonlinear transformation of an underlying factor,
i.e., R(ti) = F(x(ti)) where x is an unspecified
underlying component and F is the nonlinear transformation.
Because x is governed by a linear convolution kernel, for
example, a sum of exponential functions with possibly different signs,
this model is quite general despite its notational simplicity and can
describe systems with multiple time scales of facilitation and
depression. However, as Sen et al. (1996)
note, this
formalism does not encompass the case in which the response is governed
by an availability factor, such as a depletable pool of vesicles. We
apply the Sen optimization methodology to an extended model that
incorporates multiple availability factors.
Our approach is mechanism independent so we use generic terminology:
"underlying component," "available factor," "fraction activated," and "response," and we leave the biological
correlates unspecified. Depending on the system, the underlying
component could be identified with presynaptic calcium accumulation,
the available factor with the store of readily releasable pool of vesicles, the fraction activated with the fraction of available vesicles released, and the response with presynaptic membrane capacitance. Alternatively, the components could be identified with
postsynaptic mechanisms, in which the underlying component is
neurotransmitter concentration in the synaptic cleft, the available factor is a population of desensitizing receptors, the fraction activated is the fraction of free receptors activated, and the response
is postsynaptic current.
Each incoming action potential arrives at time
ti and stimulates an underlying component,
x(ti). The underlying component sums linearly
according to a kernel Kx(t), which
governs its decay between action potentials:
|
(1)
|
Figure 1A shows the
time course of x(t) when Kx, shown in
Figure 2A, is an exponential function.

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Figure 1.
Simulation of the available factor model
determining IPSC response. A, Each incoming action potential
stimulates an underlying factor x, which decays with an
exponential time course and sums linearly. B, x at the time
of each action potential determines the activated fraction F
of the available factor, given by a Boltzmann function of x.
C, Availability is decremented by the amount activated and
recovers with an exponential time course. D, Response
R is proportional amount activated, indicated by the
downward steps in C. E, IPSCs are given by the
linear convolution of R with the postsynaptic response
kernel.
|
|
The underlying component at time ti determines
the fraction, F(x(ti)), of the available factor
that is activated. Figure 1B shows the fraction activated as
a function of time. In all of our investigations, we examined monotone
F, i.e., the fraction that is activated is an increasing
function of the underlying component. A possible choice of F
is the properly scaled Boltzmann or Hill function (Fig.
2C). For the models of our
data, however, the distribution of the underlying component was narrow,
and thus we could make the approximation F(x) =
x. This simplifies the model and reduces the number of
parameters needed to describe the data.

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Figure 2.
Example model functions. Plots of the functions
used in the simulation in Figure 1. A, Decay of x
is determined by a single exponential rate constant,
Kx( ) = exp(  ); = 50 s 1. B, The recovery of the depleted
factor is determined by a single exponential rate constant,
KA( ) = exp(  ) where is the
time since the last action potential; = 1 s 1. C, Fraction released is given by a
Boltzmann function of x, F(x) = 1/(1 + exp( (x x1/2))) with
x1/2 = 2 and = 2.
|
|
Availability is decremented at each spike ti by
the amount activated, and between spikes it recovers with a time course
given by a function KA(t).
Availability is a discontinuous function of time, with step changes at
the time of each action potential, as shown in Figure 1C. We
use the notation A
(ti) to
indicate the time limit approached from the left and
A+(ti) for the limit from the
right, which is the fraction available immediately after a spike.
Between spikes, availability recovers continuously according to:
|
(2)
|
KA(t) has a maximum of 1, which occurs at t = 0, and a minimum of 0, which occurs
at t =
. At each time ti, the
available factor will decrease by
F(x(ti))A
(ti),
giving the relation:
|
(3)
|
Using Equation 3, we can rewrite Equation 2 as:
|
(4)
|
where
A
. For the example
shown in Figure 1C, KA is an exponential
function (Fig. 2B).
The response R(ti) is proportional to the
product of F and
A
(ti):
|
(5)
|
where s is a scalar. The response, which is defined
for discrete points in time, is shown in Figure 1D; to
obtain the full continuous time response shown in Figure 1E,
the discrete time response must be convolved with the impulse response
kernel as discussed below.
The multiplicative relationship between F and
is
analogous to the finding that mean quantal content m is
given by the product of the probability of release p and the
number of quanta N in the quantal analysis of
Castillo and Katz (1954)
and is an essential feature of
depletion models (Liley and North, 1953
; Magleby
and Zengel, 1982
; O'Donovan and Rinzel, 1997
;
Varela et al., 1997
; Dittman and Regehr,
1998
).
Nonetheless, the formulation of the available factor model in Equation 5 may be inadequate to describe many synapses, because the dynamics may
be determined by multiple, largely independent factors. In the case
where N factors sum linearly, the single factor model is
extended in a straightforward way with:
|
(6)
|
Because the factors evolve independently, the availability of
the j-th factor obeys:
In our experiments, we observed for a given neuron that the
magnitude of the first IPSC response was approximately constant between
stimuli (see Results). Therefore, for some of our investigations, we
normalized the data so that the magnitude of the first IPSC was 1 and
imposed the constraint R(t1) = 1
with the restriction on the last scalar sN. For
the additive factors model given in Equation 6, this restriction
is:
|
(7)
|
This constraint reduces the number of parameters by one.
Alternatively, the factors may combine multiplicatively. For example,
Magleby and Zengel (1982)
found a multiplicative
relationship between augmentation and facilitation at the frog
neuromuscular junction, although they found an additive relationship
between the two components of facilitation. Varela et al.
(1997)
found that a model with two depression factors that
enter multiplicatively described the EPSCs in neocortical slices. In
such cases, the multiple factor model may be written as:
|
(8)
|
with the first amplitude normalization:
|
(9)
|
It is also straightforward to extend the model to nonindependent
factors, so that the underlying component governing one availability factor (e.g., neurotransmitter concentration in the cleft governing a
population of desensitizing receptors) is the response R of a multiple factor model (e.g., presynaptic calcium concentration governing multiple pools of vesicles).
Fitting the model to data. A number of steps are required to
fit the model to the data: (1) measure the impulse kernel K
of the postsynaptic neuron, (2) extract the magnitudes
ai of the IPSCs from the postsynaptic current
record, and (3) use a gradient descent method to optimize fit between
the model and the data. The impulse kernel K is simply the
average IPSC resulting from a single presynaptic action potential.
Gradient descent is a general method of minimizing a function with
derivatives that are known (Fletcher, 1987
); in this
case the error of a model prediction is minimized over the model
parameters. By first extracting the magnitudes of the IPSCs rather than
working with the entire current record, we were able to reduce the
computation time by two to three orders of magnitude for a 30 sec spike train.
A fundamental assumption of this modeling approach is that the measured
current response I(t) can be represented as a convolution of
inputs of amplitudes ai with a fixed impulse
response kernel K. That is:
|
(10)
|
where the index i ranges over the action potentials
at times ti
t. We plot a
sample current I(t) in Figure
3A. The extracted amplitudes
ai are shown as sticks in Figure 3B,
with the time-averaged kernel K shown as an inset
in that panel.

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Figure 3.
Extraction of the IPSC amplitudes. A,
The IPSCs recorded in a postsynaptic neuron in response to stimulating
the presynaptic interneuron B4/5 with a 5 Hz exponentially distributed
train of impulses. We show a segment out of the middle of the recording
from 20-22 sec. B, We extract the amplitudes
ai of each of the IPSCs and plot them as
vertical lines. The amplitudes are computed by subtracting
the currents from previous IPSCs, which are given by the convolution of
the previous events with the impulse response kernel, which is shown in
the inset of B. The small deflection seen in the
initial rising phase of the response kernel is a stimulus artifact; the
time scale for the response kernel is expanded (scale bar, 100 msec),
and the kernel is normalized to have a peak height of 1. C,
Verification of the assumption that the IPSCs can be represented by a
convolution of the amplitudes with a fixed impulse response kernel. The
rms error of the data minus the convolved data is ~3% of the
magnitude of the first spike; this is among the largest errors we had
in using the technique, and more than half of the error is attributable
to low-amplitude noise in the recordings between the IPSCs. The
low-amplitude noise after the IPSCs is caused by the noise in the
kernel, which we measured by averaging many responses.
|
|
This assumption motivating Equation 10 is not always true; for example,
it will fail in systems where the impulse response kernel is changing
during the stimulation. Two observations validate this assumption in
our data. First, we found that the spike-triggered average of the IPSC
waveform computed in the first half of a stimulus was indistinguishable
from that in the second half when both were normalized to the same
magnitude. Second, the current obtained by the right side of Equation 10 closely resembles the measured current. We validate this assumption
in Figure 3C for our data by showing that we can
reconstitute the original current I(t) by convolving the
amplitudes with the impulse response kernel. The root mean square (rms)
error comparing the actual current with the current obtained by
Equation 10 ranged from 1 to 3% of the amplitude of the first spike.
In all of the cases, more than half of this error is explained by small
amplitude current noise in the recordings.
Measuring the kernel. The impulse response kernel
K was computed from a spike-triggered average of the
responses to many action potentials; an example kernel is shown in
Figure 3. During a train of random, repetitive stimulation, we selected
spike times that had no events following them in the subsequent 150 msec (longer than the duration of a single IPSC). These spikes were
used to compute the spike-triggered average to avoid the corrupting
effects of subsequent events. The resultant averaged waveform was
normalized by its maximum value. We preferred using this measure to
using a fixed kernel obtained by averaging the responses to single
stimuli spaced far apart because the spike triggered average method can be used independently for each train without the need for performing additional experiments. See Figure 3B, inset, for a
sample spike-triggered average kernel.
Extracting the amplitudes. We used this kernel K
to extract the magnitudes of the IPSCs in a train by effectively
deconvolving it from the recorded current I(t). For each of
the i = 1 ... N action potentials, we measured the
time t*i of the peak current that occurs
in a narrow window after the time of the i-th action
potential at ti. We then iteratively computed the magnitude ai of the i-th IPSC
as:
In words, this says that the amplitude of any IPSC is given by
its peak current minus the contribution from previous IPSCs. The
amplitudes computed in this way are plotted as vertical
lines (sticks) in Figure 3B and others.
The use of peak current values to quantify IPSC amplitudes is valid
only if the synaptic response is slow relative to the sampling time. In
our experiments, the IPSCs lasted
100 msec, and the signal was
sampled every 0.5 msec; thus we are able to obtain accurate measures of
the peak times. This conclusion is validated in Figure 3, which shows
that with the kernel K and the extracted amplitudes
ai, we can reconstruct the original signal with
a high degree of fidelity.
Gradient descent optimization. To perform the optimization,
we used a gradient descent method to minimize the sum of the squared errors between the data and model predictions (Sen et al.,
1996
). If the ai are the IPSC amplitudes
as computed above, and R(ti) are the predicted
amplitudes (where R is an arbitrary function), we want
to minimize the error
:
|
(11)
|
The gradient descent algorithm uses the gradient of the error
to find the minimum of the function over the parameter space in the
neighborhood of an initial guess. For any given experiment, the
ai are constants. Thus only partial
derivatives of the model R are required to compute the
partial derivatives of the error; if
is a parameter governing
R:
|
(12)
|
The partial derivatives of R for the available factor
model are given in the Appendix.
The Levenberg-Marquardt algorithm (Fletcher, 1987
) was
used for all of the results presented here. This algorithm was obtained from the OptSolve++ optimization library (Tech-X, Boulder, CO). An
extension specialized for data fitting problems was written in C++,
which includes a parametric model class used to define an arbitrary
(differentiable) synaptic model for use with the optimization
algorithms. For 60 sec data segments, with N = 2 factors, the model generally converged within 100 iterations in <2 sec
on a Pentium III computer (800 MHz). We will provide the code which
implements the algorithms to researchers who wish to use them upon request.
Intrinsic neuronal variability. The goodness of the fit of
the model to the observed postsynaptic responses was evaluated relative
to the intrinsic neuronal variability to repeated stimulation. Ideally
the variability in the predictions of the model should be of the same
magnitude as the intrinsic neuronal variability. To estimate the
intrinsic neuronal variability, we stimulated the B4/5 interneuron to
produce a single action potential every 20-30 sec. The magnitude of
the resultant 10 consecutive IPSCs was measured. Fixing 1 response of
the 10, we computed the rms difference between the magnitude of that
response and the 9 others, normalized by the magnitude of the fixed
response. We then repeated this computation for each of the 10 responses and report the average of these values as the intrinsic
variability. The normalized rms error of the model predictions is
computed as:
and this error is compared with the measure of intrinsic variability.
 |
RESULTS |
Figure 4A shows the
response of a neuron postsynaptic to the interneuron B4/5, which was
stimulated to fire action potentials with an exponentially distributed
train with a mean rate of 10 Hz. The depression of the resultant IPSCs
(Fig. 4A, sticks) can be approximated as the sum of
two exponentials (solid line): one with a rate constant of
0.03 s
1, another with a rate constant of
1.81 s
1. In addition there is a facilitation to
short interspike intervals (ISIs) that can be well described by a
single exponential with a rate constant of 43.5 s
1. In Figure 4B the ratio of adjacent
IPSCs (dots) is plotted as a function of ISI. These three
influences on short-term plasticity, one time scale for facilitation
and two time scales of depression, were seen in all of the neurons
investigated that were postsynaptic to B4/5.

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Figure 4.
Postsynaptic response shows two rate constants of
depression and one of facilitation. A, The IPSCs
(sticks) recorded in a postsynaptic neuron in response to
stimulating the presynaptic interneuron B4/5 with a 10 Hz exponentially
distributed train of impulses. There are two time scales of depression,
one rapidly and the other slowly depressing. Solid line is
the best fit to a double exponential function with rate constants 0.03 and 1.81 s 1. The data are normalized by the
amplitude of the first IPSC. B, The ratio of the amplitude
of an IPSC to that preceding it (dots) plotted as a function
of interspike interval. Data are from the entire 120 sec stimulus train
of which the first 20 sec are plotted above. Solid line is
the best fit to a single exponential function with a rate constant of
43.5 s 1.
|
|
Linear model
The simplest model that incorporates two times scales of
depression and one of facilitation is linear. In the linear model, the
predicted amplitudes are given by the convolution of the impulse train
with a linear response function that is the sum of one positive (facilitatory) and two negative (depressing) exponentials with different rate constants:
|
(13)
|
where all of the parameters are positive. This is a special case
of Equation 5 where F(x) = x and
(ti) = 1. The number of parameters
can be reduced to 5 by imposing the normalization
R(t1) = 1. These three exponential
functions, and the distribution of the underlying component, are shown
in Figure 5, bottom
panels.

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Figure 5.
Linear model. IPSC amplitudes are proportional to
the convolution of the spike train with a linear response function
Kx, which is the sum of three exponential
processes: rapid depression, slow depression, and facilitation. The fit
is a reasonable first-order approximation with an rms error of 0.15. This is approximately twice as high as the intrinsic variability.
A, The vertical sticks are the IPSC magnitudes in
the first 10 sec of presynaptic stimulation with 10 Hz train of
exponentially distributed impulses; the dots are the best
fit of the linear model. B, Data versus model for the entire
60 sec modeled segment. C, D, When the model fit to the data
in A and B is used to predict the responses to a
novel random stimulus from a different statistical distribution with a
different mean frequency (5 Hz train of uniformly distributed
intervals), the error is dramatically worse. Bottom panels,
The density of the underlying component x and the
exponential functions that contribute to kernel
Kx: slow depression, rapid depression, and
facilitation. The data are normalized by the amplitude of the first
IPSC.
|
|
Figures 5A shows the first 10 sec of the IPSC response
(sticks) to a random stimulus train, and the model fit given
by the equation above is plotted with dots. The model versus
the data are plotted in Figure 5B, where the identity line
indicates a perfect fit. This linear model fits the data with an rms
error of 0.15. This is approximately twice the intrinsic neuronal
variability, rms error of 0.07 ± 0.02, n = 10 for
this neuron, which we measured by computing the variation in the
responses of the neuron to identical stimuli (see Materials and
Methods; we report mean ± SEM unless indicated otherwise).
To further test the adequacy of this model, we presented novel stimulus
trains having a different mean and interval distribution. The response
of the neuron to the novel train is made using the parameters estimated
from the training stimulus. An example is shown in Figure 5,
C and E. The error of the prediction was 0.67, more than nine times the intrinsic variability. Although the linear model provides an adequate fit to the data in Figure 5, it breaks down
entirely on the task of predicting novel stimuli. The data for multiple
predictions using the linear model is summarized in Figure
6, which shows that both the fit and all
predictions fall outside the range expected form the intrinsic neuronal
variability (indicated by the bounding box).

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Figure 6.
Model fits and prediction of novel stimuli for
four classes of models. Because the data clearly show three time scales
of short-term changes in synaptic efficacy (Fig. 4), we looked at
several ways in which these time scales can enter into the model
presented in Equation 6. Each of the models presented was trained on
the same stimulus, a 10 Hz exponential train (+). This model was then
used to predict the responses to novel stimuli ( ), which were spike
trains with different means and interval distributions. The
bounding box shows the range of the intrinsic variability
(mean ± 1.96 SD) of the neuron in response to identical stimuli.
Although several models provide good fits to the data, the two additive
availability factors model is significantly better at predicting
responses to novel stimuli. An example of the data for the worst case
(linear model) and best case (two additive factors model) is shown in
Figures 5 and 7. The number of parameters for the four models shown are
5 (linear), 7 (linear w/transform), and 6 (two
factors additive or multiplicative).
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|
Nonlinear transform model
To accurately describe the excitatory junction potential response
to repeated stimulation in neuromuscular synapses of the crab, the
introduction of a nonlinear transformation (polynomial) of the
underlying linear process is a critical step (Sen et al., 1996
). Therefore, we investigated a nonlinear transformation
F(x(ti)) given by the Boltzmann function. For
values of x below the saturation point, the Boltzmann
function has an approximately polynomial shape, but saturates for large
values of x. This satisfies the intuitive requirement that
the response is bounded. Here again, the availability
(ti) = 1 is constant.
Figure 6 shows that this model does a much better job than the
linear model, with a fit within the bounds expected from the intrinsic
variability of the synaptic response. Again, however, the predictions
of responses to novel stimuli are poor.
Availability models
The nonlinear transform model is not designed to handle synapses
with availability factors (Sen et al., 1996
). We
investigated all three of the possible one available factor models
that incorporate two time scales of depression. The time scales
of depression can be modeled as an accumulation of inhibition in the
underlying component x by adding an additional exponential
term to the kernel Kx. Alternatively, they can
enter into the availability recovery function
KA. Although these three models were able to
accurately fit the training stimulus, the mean prediction error,
comparable for each model, was approximately rms = 0.2 (range
rms = 0.08-0.33; data not shown). This value is roughly four
times the intrinsic variability for this neuron.
Because the prediction errors of the models with only one availability
factor were considerable higher than the intrinsic variability, we
investigated a two-factors model with rapidly and slowly recovering
availability factors (Fig. 7). This model is given in Equation 6 with n = 2:
|
(14)
|
In Figure 7A, the first 10 sec of IPSCs resulting from
the training stimulus (same as above) are shown as sticks,
and the best fit of the model is shown as dots; the full
record of data versus model is shown in Figure 7B. Not only
does the model fit the responses to the training stimulus train to
within the intrinsic neuronal variability, it also does markedly better
at predicting the responses to novel stimuli, as shown in Figure 7,
C and D. The data from the fit and multiple
predictions are shown in Figure 6.

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Figure 7.
Two-factors model. Plot conventions are described
in Figure 5. The model here from Equation 6 provides a twofold better
fit (A, B) to the same data in Figure 5 and a fourfold
better prediction (C, D) of novel data. Bottom
panels, Left, The fraction of the rapid and slow
factors activated as a function of the underlying component. The
inset is the density of the underlying component
x, with an arbitrary vertical scale. We used the scalar
approximation (dashed lines) to the Boltzmann functions
(solid lines) to reduce the number of parameters to six so
that comparisons between models would be fair. The approximation is
quite good over the density of x. Middle, The
functions KA governing the recovery of the rapid
and slow factors; right, the function
Kx governing the underlying component. The data
are normalized by the amplitude of the first IPSC.
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We also considered a model in which the two factors combine
multiplicatively. Varela et al. (1997)
also found two
time constants of depression and one of facilitation in excitatory
synapses in the neocortex. A multiplicative relationship between the
factors described their data. In the neuromuscular junction of frog,
there is a multiplicative relationship between augmentation and
facilitation (Magleby and Zengel, 1982
). Figure 6 shows
that the predictions and fit of the two-factors multiplicative model,
although better than the linear or linear with transform models, does
not fit the data or predict novel stimuli as well as the two-factors
additive model. For the rest of the investigations below, we will
consider only the two-additive factors model, which we refer to simply as the "two-factors model."
It should be noted that the number of parameters in the two-factors
model (6) is similar to the number of parameters in the other models
(5, 6, or 7). It may seem surprising that the two-factors model has the
same number of parameters as the one-factor model, rather than twice as
many. To describe two time components of depression and one component
of facilitation requires several rate constant and amplitude
parameters. The difference between the one- and two-factors models is
simply where these parameters enter the model. Thus the substantial
improvement in the description of the data cannot be attributed to the
addition of free parameters.
Rest-time effects
For all experiments, the two-additive factors model consistently
predicted the neuronal responses to novel stimuli better than the
linear, nonlinear transform, one-factor, or multiplicative models. On
closer inspection of the prediction errors of the two-factors model
(Figure 6, third column), however, we noted that there was still considerable variability in the goodness of fit. Investigating the possibility that this difference could be attributed to changes in
the neuronal state on the time scale of minutes between experiments, we
collected a large number of stimulus responses in which we varied the
rest-time between stimuli from just under 2 min to >1 hr. Each of the
stimuli were long trains lasting several minutes.
Figure 8A-C shows the
response of a neuron to three consecutive stimulus trains drawn from
interval distributions having the same mean frequency (5 Hz). In Figure
8A, the neuron has rested for >30 min; in Figure 8,
B and C, the rest-time was only 2 min. In all
cases, there is a slow prolonged decrease in the response throughout
the duration of the stimulus train. For the short rest-times, however,
an initial rapidly decrementing response of the neuron appears that was
not apparent for the rested neuron. Thus the rest-time between stimuli
appears to be an important determinant of the extent of synaptic
depression in early responses.

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Figure 8.
Responses of a single neuron to three consecutive
stimulations of the interneuron B4/5. The left panels show
the current traces of the first 5 sec of a much longer stimulation. The
right panels show the amplitudes of IPSCs over the entire
stimulus on semilogarithmic axes. All of the stimuli have a mean ISI of
200 msec: A and B show the response to a uniform
distribution of intervals with an ISI SD = 0.11 sec;
C and D show the response to an exponential
distribution of intervals with = 0.19 sec; E and
F show the response to a Gaussian distribution of intervals
with = 0.078 sec. The smaller variance seen in F
compared with B and D presumably arises from the
smaller variance in the interval distribution. Note the development on
a rapidly depressing component in the first few seconds of the stimulus
in the middle and bottom panels, which is not
present in the top panel. The top panel is a
rested synapse, with >30 min elapsed since the previous stimulus (data
not shown), whereas the middle and bottom panels
are comparatively non-rested, with a 2 min elapsed since the
preceding stimulus. Evidence presented below indicates that the
development of a rapidly depressing component is stimulus induced and
not dependent on the statistical distribution of the inputs. The
apparent increases in the variability of the IPSC amplitudes with time
is an illusion created by the use of a logarithmic x-axis.
The outliers below the bulk of the responses toward the end of stimuli
in B are an artifact. Because these artifacts occurred
rarely ( 1/1000 IPSCs), we did not try to remove them from the
analysis pool.
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Figure 9 summarizes the prediction error
over 20 novel stimuli. The point marked training stimulus
indicates the data shown in the top panels of Figure 10. The
error in the prediction of the responses to 20 stimuli is plotted as a
function of stimulus order (Fig. 9A) and rest-time (Fig.
9B). The prediction error is not dependent on stimulus
order; the errors appear random as a function of order. However, there
is a strong effect of rest-time. For experiments with similar
rest-times, indicated by the bounding box in Figure
9B, the error in the prediction falls within the expected
range given by the intrinsic variability for all points save two.

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Figure 9.
Error in prediction varies with rest-time, not
stimulus order. We performed 20 separate stimulations of the same
neuron with inputs drawn from different statistical distributions (2 or
5 Hz with exponential, Gaussian, or uniform distribution of intervals).
We took 1 of these 20 and trained a two-factors model (training
stimulus). A, rms error of the predictions plotted as a
function of sequential stimulus number; the error does not vary
systematically with order. B, rms error as a function of
time since last stimulus (rest-time). The largest prediction
errors occur for rest-times far from that of the training stimulus. The
bounding box shows a region where we expect the predictions
to be good: the range on the abscissa is given by the
rest-time of the training stimulus ± 1 min; the range on the
ordinate is given be the mean ± 1.96 SDs of the
intrinsic variability.
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The training stimulus, with a rest time of
2 min, is shown in Figure
10A, where the IPSCs are
plotted as sticks and the model fits are plotted as
dots. Examples of the responses and predictions for two
novel stimuli with similar rest-times are shown in Figure 10,
C and E. The rms prediction error drops to the
order of the intrinsic variability. For each of these three examples,
the model predictions versus the measured data for the full segment is
plotted to the right.

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Figure 10.
Two-factors model predicts responses to novel
stimuli. Plot conventions are described in Figure 5. The novel stimuli
have a different mean frequency or interval distribution than that used
to build the model. The novel stimulus sets were chosen so that their
rest-time was similar to that of the training stimulus. A,
B, The parameters were determined from the training stimulus.
C, D, Model predicts responses to a novel 2 Hz exponentially
distributed train. E, F, Model predicts responses to a novel
5 Hz Gaussian distributed train. The data are normalized by the
amplitude of the first IPSC.
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We next determined whether the changes in the response of the neuron
attributable to rest-time could be isolated to one of the
model components. The observation that the amplitude of the first
spike is approximately constant, seen in the raw data in Figure 8, is
supported in Figure 11A,
where the first spike amplitude over 20 stimulus sets is plotted as a
function of rest-time. The proportion of variance in the first IPSC
amplitude explained by rest-time is R2 = 2%, clearly indicating that the first IPSC does not vary with rest-time.

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Figure 11.
First IPSC amplitude and recovery time constant
of rapidly recovering availability factor as a function of rest-time.
A, Amplitude of first event. B, Recovery rate
constant.
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This puts a severe constraint on which parameters can change with
rest-time. Namely, only parameters governing recovery can change
without systematically altering first IPSC amplitude. Thus, if we
assume that only one parameter is changing with rest-time (see
Discussion), this leaves the parameters governing
Kx, KA1, and
KA2 as candidates. These kernels govern the
decay of the underlying component, the recovery rate of the rapid
factor, and the recovery rate of the slow factor. The rate constants
for these three kernels are
x,
A1, and
A2.
The procedure to identify the parameter that varied with rest-time is
as follows. By sharing five of the six model parameters between
stimuli, and allowing one (
x,
A1, or
A2) to
vary freely, we simultaneously fit the model to all stimuli over the
range of rest-times. We found that only
A1 was
sufficient to account for the changing response with rest-time, with an
overall rms error of 0.05 ± 0.007, n = 20
equivalent to the intrinsic variability. The rms error obtained when
only
A1 was allowed to vary was significantly lower
than that obtained with either
A2 or
x (Student's t test; p < 0.01;
n = 20). The latter two were statistically indistinguishable.
Figure 11B shows the recovery time constant as a function of
rest-time. For short times, the time constant is small (with one exception) and grows with longer rest-times. There is, however, considerable variability with long rest-times. The simplest explanation consistent with our observations is that presynaptic stimulation of
B4/5 slows the rate of recovery of the rapid factor.
How are two neurons different?
Figure 12, A and
B, shows IPSCs recorded simultaneously in two neurons
postsynaptic to the B4/5, which was stimulated to fire action
potentials with a 5 Hz Poisson stimulus. Despite the fact that both
neurons are postsynaptic to the same interneuron, their responses are
quantitatively different. In particular, for one of the neurons, the
depression of the IPSC amplitudes in the early response is clearly
larger.

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Figure 12.
Responses of two postsynaptic neurons recorded
simultaneously in response to stimulation of B4/5. A, B,
IPSCs from a 10 sec segment of a random stimulus train. The amplitude
of the currents in both neurons is normalized by the first event to
facilitate comparison. Both neurons show similar features, notably an
initial rapid depression and a sustained slow depression, as well as
short-term facilitation after short interspike intervals. The rapid
onset of depression in the lower neuron, however, is more pronounced.
C-I, Plots of the parameter values from one neuron versus
the other. The neuron with the smaller average IPSC in each pair is
assigned plotted along the ordinate, and other neuron in the
pair is plotted along the abscissa. A full two-additive
factors model was fit to each neuron in the pair, and the values for
each of the seven parameters are plotted. Multiple stimuli for each
pair are plotted with the symbols ×, , and , indicating the
neuron pair. Values that fall along the identity line indicate that
both neurons in the pair have identical values for that
parameter.
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A useful way to estimate the difference between the IPSC amplitudes of
the two neurons is to again use the rms error. Identifying one of the
trains with the "prediction," the rms error of the second relative
to the first is 0.25. This error is approximately five times the
intrinsic neuronal variability (0.05 and 0.06 for the neurons in Fig.
12). The average rms difference between the two neurons in all pairs
investigated, normalizing the IPSCs in each train by the first, is
0.20 ± 0.03, n = 13. Thus the differences in the
response between the two neurons cannot be explained simply in terms of
random variations in neuronal response.
To quantify the differences between the neurons in terms of the model,
we fit the parameters of the model to each neuron pair for all pairs.
Unlike the case above, in which we investigated how a single neuron
changes with rest-time, in the two-neuron case the amplitude of the
first IPSC is not the same between neurons. So we did not constrain the
investigation to rate constants. Instead, we modeled each postsynaptic
neuron independently.
For each pair of simultaneously recorded responses, we assigned the
response with the smaller average IPSC to be neuron 1 and the other to
be neuron 2. The values for each of the parameters are plotted in
Figure 12C-I, in which the parameter value for neuron 1 is
plotted along the abscissa and the value for neuron 2 is plotted along
the ordinate. The line of identity indicates the values where the two
neurons have the same value for the parameter plotted. The left
column (C, E, G) shows the parameters for the rapid factor,
and the right column (D, F, H) shows the parameters for the slow factor. The data are taken from 13 stimuli in three neuron
pairs (plotted with the symbols ×,
, and
). A given neuron may
change from stimulus to stimulus, as noted in the discussion of
rest-time effects above. For both scalar factors
s1 and s2, the
values for neuron 2 are consistently larger than for neuron 1, falling
above the line of identity (Fig. 12C,D); this is
particularly apparent for s2. Although there is
considerable scatter about the line of identity for the other
parameters, there are no consistent differences between neuron pairs.
We then tested to see whether variations s1 and
s2 alone could account for the different
responses by constraining the model for each pair to share all
parameters except s1 and
s2. If the model can fit the data to within the
bounds expected by the intrinsic variability with this constraint, then
this suggests that these two parameters are sufficient to explain
interneuronal variation. With these constraints, the average fit rms
error was 0.07 ± 0.01, n = 13, which is within
the intrinsic variability bounds. These observations suggest that the
main difference between the two neurons can be accounted for by the
amount of current carried by the rapid and slow factors.
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DISCUSSION |
One of the fundamental issues in the study of neural computation
is the information flow across the synapse. The model presented here
accurately describes the output of a central synapse to a wide range of
synaptic inputs, varying in mean and interval distributions. Although
the model does not identify the locus of these factors, this
distinction may not be important for the study of computation and
information transfer, because it is the total synapse that is the
operative unit. The model does identify, however, how many availability
factors are required to describe the synapse, their relative sizes, and
recovery kinetics. It also provides a means to assess how these
quantities change with experimental perturbations. Many different
possible mechanisms can give rise to similar qualitative behavior.
Thus, a mechanism-independent means of quantifying synaptic properties
is useful.
Our results imply the existence of two availability factors at the B4/5
synapse of Aplysia. The smaller factor is characterized by a
high probability of activation and a recovery time of the order of
seconds. This factor governs the rapid depression seen in the early
IPSC response. Changes in the recovery rate of this factor can explain
the effects of rest-time on neuronal response. The larger factor is
characterized by a lower probability of activation and recovers with a
time course on the order of tens of seconds. This factor generates the
long slow decay of the response seen throughout the several hundred
seconds of stimulation. These observations are qualitatively similar to
those of Varela et al. (1997)
in visual cortex, who also
observed two time scales of depression and one of facilitation.
We have shown that a model of the Aplysia central synapse
that incorporates these two availability factors together with a single
facilitation component describes the response of the neurons to both
training and novel spike trains. This model does not distinguish between availability factors located presynaptically from those located
postsynaptically. The fact that both factors share the same underlying
component and are otherwise independent, however, suggests that they
are on the same side of the synapse. In other systems, there is
abundant evidence supporting the existence of multiple pools of
vesicles (Mennerick and Matthews, 1996
; Silver et
al., 1998
; Gomis et al., 1999
; Burrone
and Lagnado, 2000
; Stevens and Williams, 2000
);
for reviews, see Zucker (1996)
and Neher (1998)
. Although we cannot exclude the possibility that the
dynamics observed in our preparation arise from presynaptic depression or vesicle depletion, we have chosen to discuss our results in the
context of the known properties of Aplysia acetylcholine
receptors (AChRs) in B4/5 follower neurons.
In Aplysia, early work indicated the presence of at least
two pharmacologically distinct AChRs, with different desensitization sensitivities (Tauc and Gerschenfeld, 1961
; Tauc
and Bruner, 1963
; Kehoe, 1969
). In the buccal
ganglion follower cells of B4/5, two different AChRs on the same neuron
have different rates of desensitization to repeated stimulation of
B4/5; this can be mimicked with ionophoretic acetylcholine (ACh)
application (Gardner and Kandel, 1977
). Selective antagonization of one of two classes of pharmacologically distinct AChRs, each of which mediate an inhibitory Cl
conductance, reveals that one rapidly desensitizes to tonic ACh application, whereas the other slowly desensitizes (Kehoe and McIntosh, 1998
). In the cholinergic buccal neurons that
Kehoe and McIntosh (1998)
investigated, it appeared that
the two receptor populations were present in different proportions. The
multicomponent response is by no means limited to Aplysia,
but rather is a common feature of postsynaptic responses
(Feigenspan and Bormann, 1994
; Elson and
Selverston, 1995
; McGehee and Role, 1995
).
Thus the evidence on desensitization of AChRs in Aplysia is
consistent with our observations. There are two populations of inhibitory receptors with different desensitization sensitivities, and
there is neuronal variation in the proportion of these two populations.
This is consistent with the model findings that the sizes of the two
availability factors varied between neurons. We also found that
stimulation of B4/5 led to a more rapid depression of the early
responses in subsequent trains. In the model, this was identified with
a slowing of the rate of recovery of the rapidly recovering factor.
Under the desensitization hypothesis, this predicts that repeated
application of ACh slows the recovery from desensitization for the
rapidly desensitizing inhibitory AChRs.
Although it might be anticipated that in a prolonged train the shape of
the IPSC waveform would change during receptor desensitization (which
we did not observe), this does not always occur. For example, in
central GABAergic synapses, there is a slow GABAA receptor desensitization that affects only the IPSC amplitude (Overstreet et al., 2000
). Additionally, the rapid effects of
acetylcholinesterase at buccal cholinergic synapses may serve to block
such actions of acetylcholine (Simonneau and Tauc, 1987
;
Fossier et al., 1990
).
Our conclusion that stimulation modulates the recovery rate of the
rapid factor is based on the assumption that only one parameter is
changing with rest-time. Other explanations are possible. If more than
one parameter is allowed to vary simultaneously, then the
stimulus-induced changes can be explained, for example, by allowing the
sizes of both factors to vary with rest-time. As long as the relative
sizes are constrained so that the amplitude of the first IPSC is
approximately constant, the stimulus-induced modulation of depression
can be modeled as an increase in the proportion of the rapid factor
(data not shown). This raises the possibility that differential
sensitivity to the stimulus-induced changes contributes to the observed
synaptic heterogeneity. Such stimulus-dependent control of receptor
expression is observed in other systems, where the cycling of receptors
shows differential sensitivity to stimulus modulation depending on
receptor type (Turrigiano et al., 1998
; Akaaboune
et al., 1999
; Ehlers, 2000
).
It is experimentally challenging to measure the properties of synapses
in which the stimuli themselves alter the synaptic response to
subsequent stimuli. We observed that long trains of stimuli had effects
on synaptic depression that persisted over a time scale of minutes.
These effects cannot be readily quantified using paired-pulse
stimulation, for example, because the effect decays during the time it
takes to measure it. Protocols that measure synaptic properties at
longer time scales magnify the difficulties. Although it is
possible in some specialized systems to eliminate this con