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The Journal of Neuroscience, January 15, 2002, 22(2):584-591
Redundancy Reduction and Sustained Firing with Stochastic
Depressing Synapses
Mark S.
Goldman1, 3,
Pedro
Maldonado4, and
L. F.
Abbott1, 2
1 Volen Center and 2 Department of Biology,
Brandeis University, Waltham, Massachusetts 02454, 3 Department of Physics, Harvard University, Cambridge,
Massachusetts 02138, and 4 Facultad de Medicina, Instituto
de Ciencias Biomedicas, Universidad de Chile, Santiago, Chile
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ABSTRACT |
Many synapses in the CNS transmit only a fraction of the action
potentials that reach them. Although unreliable, such synapses do not
transmit completely randomly, because the probability of transmission
depends on the recent history of synaptic activity. We examine how a
variety of spike trains, including examples recorded from area V1 of
monkeys freely viewing natural scenes, are transmitted through a
realistic model synapse with activity-dependent depression arising from
vesicle depletion or postrelease refractoriness. The resulting
sequences of transmitted spikes are significantly less correlated, and
hence less redundant, than the presynaptic spike trains that generate
them. The spike trains we analyze, which are typical of those recorded
in a variety of brain regions, have positive autocorrelations because
of the occurrence of variable length periods of sustained firing at
approximately constant rates. Sustained firing may, at first, seem
inconsistent with input from depressing synapses. We show, however,
that such a pattern of activity can arise if the postsynaptic neuron is
driven by a fixed population of direct, "feedforward" inputs
accompanied by a variable number of delayed, "reverberatory"
inputs. This leads to a prediction for the number and latency
distribution of the inputs that typically drive a cortical neuron.
Key words:
synaptic depression; natural stimuli; information theory; redundancy; correlation; V1
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INTRODUCTION |
Information transfer across many
central synapses seems remarkably ineffective because of frequent
synaptic transmission failures (Stevens and Wang, 1995 ; Murthy et al.,
1997 ). However, if presynaptic spike trains encode information
redundantly, unreliable transmission can save resources by allowing a
synapse to filter out redundant aspects of its inputs. Spike
sequence-dependent filtering can arise because the probability of
release for most synapses is modulated by activity-dependent processes
(Zucker, 1989 ). As a result, the sequence of transmissions can, in
principal, be less redundant than the presynaptic spike train.
Many recorded spike trains display temporal autocorrelations over time
scales of hundreds of milliseconds, indicative of redundant coding (Dan
et al., 1996 ; Baddeley et al., 1997 ). This redundancy can limit the
amount of information carried by a neural system (Barlow, 1961 ; Atick,
1992 ). Spike train autocorrelations may reflect intrinsic properties of
the spiking neuron, such as bursting, or features of its inputs. In
sensory areas, temporal autocorrelations may be generated by mechanisms
of sensory acquisition, such as saccadic eye movements, whisking, and
sniffing, that sample at frequencies of a few to several hertz.
In the first part of this article, we study the transmission of four
types of spike trains through a model synapse constructed to match data
on synaptic depression in slice preparations from various brain regions
(Abbott et al., 1997 ; Hjelmstad et al., 1997 ; Thomson and Deuchars,
1997 ; Tsodyks and Markram, 1997 ; Varela et al., 1997 ; Dobrunz and
Stevens, 1999 ; Dittman et al., 2000 ). The four types are: (1) a Poisson
spike train, (2) a spike train based on a simple model of visually
evoked activity during free viewing (which we call the saccade
model), (3) a model spike train based on experimentally recorded
bursting neurons, and (4) spike trains recorded in area V1 of awake
monkeys freely viewing natural scenes. Our results indicate that
activity-dependent, stochastic synapses can reduce spike train
redundancy by removing autocorrelations within these trains.
In the second part of the article, we study how sustained firing can be
generated in neurons receiving input through depressing synapses. The
correlations in the spike trains we study arise from periods of
sustained firing typically lasting for hundreds of milliseconds.
Depressing synapses that receive such input tend to produce transient
rather than sustained synaptic currents. Despite this, we show that a
reasonable model of the total input to a neuron that includes both
immediate and delayed components can generated sustained periods of firing.
The overall claim of this work is that activity-dependent, stochastic
synapses remove autocorrelations from presynaptic spike trains, but
that cross-correlations among multiple inputs reintroduce autocorrelations into postsynaptic spike trains. Thus, it might appear
that the benefits of stochastic filtering at single synapses are undone
by the multiple inputs to a neuron. However, as we analyze further in
the Discussion, this is not the case. Even when multiple inputs
reintroduce autocorrelations into postsynaptic spike trains, the
ability of depressing synapses to enhance important temporal features
of the input is not lost. Furthermore, noisy input signals that arrive
synchronously across many inputs can be averaged instantaneously,
something that could only be done at the single-input level by lengthy
temporal averaging.
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MATERIALS AND METHODS |
Experimental procedures
Subjects and surgical procedures. Two adult female
rhesus monkeys (Macaca mulatta) weighing 7-10 kg served as
subjects for this study. A pair of scleral search coils were implanted
for monitoring eye position (Judge et al., 1980 ). During the same surgery, a recording chamber was mounted over the opercular surface of
the striate cortex. A small craniotomy (5 × 10 mm) was made in
the bone overlying one cortical hemisphere. All surgical procedures were performed at the California Regional Primate Research Center and
were supervised by the attending veterinary staff. Surgical and
experimental techniques were in accordance with institutional and
National Institutes of Health guidelines.
Behavioral training. For receptive field
characterization, the monkeys were trained to maintain their gaze
within 1.0° of a fixation spot, in the presence of moving or
stationary visual stimuli, for up to 3 sec. Successful trials were
rewarded with a drop of diluted apple juice. Access to water was
restricted during behavioral training and recording. After receptive
field characterization was completed, natural stimuli were presented for 3 sec, and the monkeys were allowed to freely view the natural scene.
Recording techniques. Electrophysiological signals were
recorded with custom-fabricated nichrome tetrodes separated by either 250 µm or 3-4 mm. The signals were amplified, bandpass-filtered (0.6-6 kHz), and digitized (30 kHz/channel) using custom software. After recording, individual units were resolved from the multiunit activity through principal components analysis of waveforms or by
clustering spikes on the basis of peak-to-peak amplitude, peak time,
and spike width, as described by Gray et al. (1995) . The extracted
spike trains were stored at 1 msec resolution. The eye coil signals
were digitized (1 kHz/channel) and stored using custom software.
Stimuli. Visual stimuli consisted of natural scenes,
composed primarily of landscapes, presented with a slide projector and projected from behind the animals onto a screen located 1 m in front of them. Receptive field location and properties were measured using single or multiple light bars or square wave gratings (0.5-3.0 cycles/°) presented on a computer monitor with a dark background and
ranging in mean luminance from 0.003 to 12 cd/m2.
Modeling Procedures
Synaptic depression. Several models of synaptic
depression were tested, and all gave qualitatively similar results.
Here, we present results from a simple stochastic model of a single active zone (Vere-Jones, 1966 ; Matveev and Wang, 2000 ). Although we
formally model a single active zone, our results extend to single
synapses with multiple independent active zones or multiple synapses
receiving synchronous input, provided that the active zones have the
same characteristics and that their outputs add without saturation.
The active zone is assumed to have N vesicles available for
release, where N cannot exceed a maximum number
Nmax. On arrival of a presynaptic
action potential, each of the N available vesicles has a
probability p of being released, with the restriction that not more than one vesicle can be released per action potential (Korn
and Faber, 1991 ; Stevens and Wang, 1995 ). This gives the synaptic
transmission probability, P = 1 (1 p)N. When a vesicle is released, N is
decreased by 1, causing synaptic depression attributable to vesicle
depletion. Each released vesicle has an independent, constant
probability per unit time, 1/ D, of being
replenished. On average, this yields exponential recovery from
depletion with time constant D. For the
Poisson and saccade model spike trains (Figs. 1, 2),
Nmax = 3. In the studies involving the
model bursting neuron and real V1 neuron spike trains (Figs. 3, 5),
Nmax = 1. Nmax in this model governs the
strength of depression immediately after vesicle release (strongest
depression for Nmax = 1) and
represents an "effective" number of vesicles that takes into
account both the possibility of having a population of vesicles with
heterogeneous probabilities of release and the postrelease refractoriness thought to occur across an active zone (Dittman et al.,
2000 ). For purposes of comparison, we also consider a model in which
synaptic transmission occurs with constant probability.
To study the effects of multiple inputs, we use a deterministic rate
model of depression (Abbott et al., 1997 ; Tsodyks and Markram, 1997 ).
In this model, the steady-state probability of release for a
presynaptic spike train generated by a Poisson process at rate
r is:
|
(1)
|
If the presynaptic rate changes suddenly from
r0 to
r1 at time 0, the transmission
probability decays exponentially from Pss(r0)
to
Pss(r1):
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(2)
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Spike trains. Spike trains generated by the saccade
model are produced by a piecewise, constant-rate Poisson process that simulates the response of a visual neuron during a sequence of saccades
to different targets. After each simulated saccade, the model generates
a Poisson spike train at a constant rate until the time of the next
saccade. A new Poisson rate is chosen independently at each
saccade from an exponential distribution with a mean of 15 Hz (Levy and
Baxter, 1996 ; Baddeley et al., 1997 ). The saccade durations were chosen
to fit an observed distribution of intersaccade intervals,
tsacc (Viviani, 1990 ), using the
function (exp[(4.55 Hz) tsacc] + exp[8.82 (54.28 Hz)tsacc]) 1.
This distribution peaks at 192 msec and has a mean intersaccade interval of 365 msec.
The model burst train is adopted from a fit to bursting cells recorded
in area MT of monkeys performing a visual discrimination task, as
described by Bair et al. (1994) . Interburst intervals were chosen from
an exponential distribution with a mean of 31 msec, with intervals
shorter than a minimum duration discarded and chosen again. The minimum
interburst interval was chosen randomly from a Gaussian distribution
with a mean of 16 msec and an SD of 7 msec, clipped at 0. The durations
of individual bursts were chosen from a Gaussian distribution with a
mean of 5.2 msec and an SD of 1.1 msec. Within the bursts, spikes were
generated with Gaussian-distributed interspike intervals with a mean of
1.8 msec and an SD of 0.5 msec. The burst duration and interspike
interval distributions were clipped at 0.
For the real V1 spike trains, twenty 5 sec responses recorded in each
cell were concatenated to make a 100 sec train. The transmission
autocorrelations for these trains were computed from enough repetitions
to gather 100,000 presynaptic spikes. Model results were also based on
100,000 presynaptic spikes.
Integrate-and-fire neuron. We used a leaky
integrate-and-fire model neuron to generate the postsynaptic responses
used in Figure 6. Synaptic transmissions produced an excitatory
postsynaptic conductance with an instantaneous rise and exponential
decay with a time constant of 2 msec. Neuronal and synaptic parameters
were chosen so that the postsynaptic neuron had an approximate balance of excitatory input and effectively inhibitory decay to rest (Shadlen and Newsome, 1994 ; Troyer and Miller, 1997 ) and had matching input and
output average firing rates. For all simulations, we used a membrane
time constant m = 30 msec and spike threshold
Vth = 55 mV. For simulations with
1000 synaptic inputs, the resting potential
Vrest = 68 mV, and the reset voltage
Vreset = 58 mV. Each synaptic
transmission increased the synaptic conductance by
gsyn = 2.5% of the
resting membrane conductance. For simulations with 30 synaptic inputs,
Vrest = 65 mV,
Vreset = 60 mV, and gsyn = 55% for runs that used
dynamic synapses, and Vrest = 63 mV,
Vreset = 59 mV, and
gsyn = 39% for runs that used
constant-probability synapses.
Autocorrelations. Autocorrelations, representing a
normalized probability density of two spikes being separated by a time , are defined by:
|
(3)
|
and satisfy 1 A( ) < . and indicate time averaging. In practice, the autocorrelation is
computed by dividing time into discrete bins, with
s(t) equal to the number of presynaptic or
transmitted spikes within the bin containing the time t
divided by the bin width. For reference, A( ) = 1 indicates that, each time a spike occurs in a train, it is twice as
likely as average that another spike will arrive a time later (to
within a bin width). A( ) = 1 indicates that a
spike is never followed by a spike occurring a time later (to
within a bin width).
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RESULTS |
Transmission autocorrelations
We are interested in how efficiently the sequence of action
potentials transmitted by an activity-dependent, stochastic synapse encodes the information carried by the full presynaptic spike train.
Unfortunately, a full information calculation is beyond the range of
existing methods because of the long correlation times of the spike
trains we consider. Instead, we use decorrelation as an approximate
indication of the maximization of transmitted information at fixed
average transmission probability. This approximation is accurate for
high signal-to-noise ratios in the synaptic transmissions, meaning
that, for multiple presentations of the same stimulus, the sequence of
spikes that gets transmitted is approximately the same for each
presentation. Specifically, we compare the autocorrelation of spike
sequences arriving at a synapse with the autocorrelation of the
sequence of spikes transmitted through the synapse and use the level of
autocorrelation as an approximate measure of redundancy (Barlow, 1961 ;
Atick, 1992 ). Within this approximation, redundancy reduction is
equivalent to reducing the magnitude of autocorrelations.
Synaptic failures add negative autocorrelations to Poisson
spike trains
We begin by examining how the model synapse transmits spike trains
generated by a homogeneous Poisson process, which are uncorrelated (Fig. 1A). Figure 1,
B and C, shows the results of sending Poisson spike trains through a stochastic synapse with constant transmission probability (Fig. 1B) or with vesicle depletion (Fig.
1C). Each synapse transmits 23% of the incoming spikes.
Transmission with constant probability thins the presynaptic spike
train but does not change its autocorrelations; therefore, it produces
an uncorrelated sequence of transmissions (Fig. 1B).
In contrast, the transmissions through the depleting synapse have
negative autocorrelations, reflecting the dynamics of the
activity-dependent transmission process (Fig. 1C). The
correlation time for the negative autocorrelations is a decreasing
function of rate, and it is shorter than the refilling time constant
D. This is because, in the presence of
presynaptic input, the rate of recovery to the partially depleted state
seen during activity is controlled in parallel by the vesicle refilling process and the rate-dependent vesicle release process. This leads to a
recovery rate that is an approximately additive combination of the
refilling and vesicle depletion rates.

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Figure 1.
The activity-dependent dynamics of vesicle
depletion add negative autocorrelations to sequences of synaptic
transmissions. A, Autocorrelation of a Poisson spike
train of average rate 15 Hz. B, Autocorrelation of the
transmissions of this spike train through a model synapse with a
constant probability of transmission. C, Autocorrelation
of the transmissions of the Poisson train through a model synapse with
p = 0.2 and D = 500 msec. In
both B and C,
Nmax = 3, and 23% of presynaptic
spikes were transmitted.
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Synaptic failures remove positive autocorrelations from saccade
model spike trains
We next consider more realistic spike trains with positive
autocorrelations, using a model that simulates the responses of a
visual neuron during a sequence of saccades to different targets (see
Materials and Methods). Spike trains produced by the saccade model have
positive autocorrelations that are nearly exponential, with a decay
time constant corr = 235 msec (Fig.
2A, black
line). Positive spike train autocorrelations indicate that, each
time a spike arrives at the synapse, there is a greater than average probability that additional spikes will arrive over a subsequent time
of order corr. Synapses with vesicle depletion
remove positive autocorrelations, because their dynamics have the
complementary property that each time a spike is transmitted, future
spikes are less likely to be transmitted over a time determined by the vesicle recovery dynamics, D. The
decorrelation is optimal when D ~ corr (Fig. 2A, black
bars), but nearly complete decorrelation occurs over a hundreds of
milliseconds range of D.

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Figure 2.
Decorrelation of a saccade model spike train by a
stochastic synapse with vesicle depletion. A,
Autocorrelation of the presynaptic saccade model train of average rate
15 Hz (black line) and of the transmissions through a
model synapse with p = 0.5 and
D = 350 msec (black bars).
Thirty-three percent of presynaptic spikes were transmitted.
B, Autocorrelation of the transmissions through a model
synapse with p = 0.5 and D = 70 msec (black line) or 1750 msec (gray
line). Sixty-five and 10% of presynaptic spikes were
transmitted, respectively. C, Autocorrelation of the
transmissions through a model synapse with p = 0.5 and D = 350 msec when the average presynaptic rate
is 3 Hz (black line) or 75 Hz (gray
line). Sixty-nine and 10% of presynaptic spikes were
transmitted, respectively. D, Autocorrelation of the
transmissions through a model synapse with D = 350 msec and p = 0.1 (black line) or 1.0 (gray line). Seventeen and 38% of presynaptic
spikes were transmitted, respectively. In A,
B, and D, the average presynaptic rate is
15 Hz. In A-D, Nmax = 3.
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A synapse with much shorter vesicle refilling time constant
D approaches the nondecorrelating behavior of
a synapse with constant transmission probability (Fig.
2B, black line). A synapse with much
longer D not only produces small negative
autocorrelations but also greatly degrades the spike train by
transmitting only a small fraction (10%) of presynaptic spikes (Fig.
2B, gray line). With the synaptic
parameters set to decorrelate the 15 Hz presynaptic train, as in Figure
2A, black bars, significant lowering of
the presynaptic firing rate reduces the decorrelating effect because of
the greater recovery of the synapse between presynaptic spikes (Fig.
2C, black line). However, increases in the
presynaptic firing rate have little effect on the statistics of the
transmitted train, even for large increases (Fig. 2C,
gray line). At higher rates, the decorrelation effect
appears to be dominated by the time constant of depression, rather than
by the faster, rate-dependent time constant that governs the negative
autocorrelations observed for Poisson trains. Changing the
single-vesicle release probability p is similar to changing
the presynaptic firing rate except for a reduced sensitivity to
reductions in p that results from the nonlinear dependence
of the transmission rate on p. As a result, the effect of
both positive and negative changes in p on autocorrelations is weak (Fig. 2D). This indicates that the
activity-dependent vesicle depletion and replenishment processes, not
the vesicle release probability, govern the observed decorrelation.
Synaptic failures remove positive autocorrelations from
burst trains
A model burst train was adopted from the work of Bair et al.
(1994) , who modeled the burst firing of cells recorded in area MT of
awake monkeys (see Materials and Methods). The autocorrelations for
these spike trains are positive at short times because of the
relatively regular spiking during the bursts and negative for longer
intervals because of interburst intervals (Fig.
3A).

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Figure 3.
Removal of positive autocorrelations from a model
burst train by a stochastic synapse with activity-dependent
transmission failures. A, The presynaptic burst train
has strong positive autocorrelations followed by near-maximal negative
autocorrelations. B, Autocorrelation of the
transmissions through a model synapse with D = 15 msec, p = 0.5, and
Nmax = 1 (left) or 3 (right). Twenty-six and 67% of presynaptic spikes were
transmitted, respectively.
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The three-vesicle model (Nmax = 3)
used for Figures 1 and 2 does not produce enough depression to remove
the large positive autocorrelations characteristic of the burst trains
(Fig. 3B, right). To increase the amount of
depression, we reduced Nmax to 1. We
also decreased the recovery time constant D to
a value just less than the mean of the minimum interburst interval to match the shorter autocorrelation time of the burst trains. This removes the burst-associated positive autocorrelations in the spike
train without adding excessive negative autocorrelations at longer
times (Fig. 3B, left). A strong and rapidly
recovering form of depression such as this has been hypothesized to be
caused by refractoriness of the entire active zone rather than vesicle depletion (Hjelmstad et al., 1997 ; Thomson and Deuchars, 1997 ; Dittman
et al., 2000 ). The single-vesicle model, by having zero transmission
probability immediately after a spike, simulates this process within a
simple exponential recovery model.
Synaptic failures remove positive autocorrelations from V1 spike
trains recorded from monkeys freely viewing natural scenes
Spike trains were recorded from area V1 of awake monkeys freely
viewing natural scenes. Various response types were observed (Fig.
4). Some neurons fired in a pattern that
was qualitatively similar to that of the model saccade trains,
maintaining a stimulus-dependent firing rate during fixations (Fig. 4,
cells 1, 5). Others appeared to have more bursty
behavior or a mixture of bursting and irregular firing behavior, with
bursts often appearing at the beginning or end of fixations (Fig. 4,
cell 14). All cells studied exhibited strong positive
autocorrelations that decayed over various time scales. A few cells had
strong positive autocorrelations for small and small negative
autocorrelations for intermediate . Generally, the large positive
autocorrelations in all trains tended to decay more rapidly than those
of the model saccade trains (Fig. 2).

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Figure 4.
Spike trains recorded from area V1 of a monkey
freely viewing natural scenes. Traces 1-14 show the
responses of 14 different neurons, and traces V and
H indicate the horizontal and vertical eye
positions.
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We analyze three spike trains that approximately sample the types of
autocorrelations observed: one with strong positive short-time autocorrelations and a long tail of weaker positive
autocorrelations (Figs. 4, cell 13,
5, right, black
line), one with positive autocorrelations of an intermediate
duration (Figs. 4, cell 1, 5, middle,
black line), and one with strong but short positive
autocorrelations (Figs. 4, cell 14, 5, left,
black line). To test the robustness of the decorrelating
effect, we examined transmission for each of these spike trains using a
model synapse with a fixed set of parameters
(Nmax = 1; D = 150 msec; p = 1.0). These parameters are consistent
with a combination of the refractory and vesicle depletion forms of
depression found in slice preparations (Abbott et al., 1997 ; Hjelmstad
et al., 1997 ; Thomson and Deuchars, 1997 ; Tsodyks and Markram, 1997 ;
Varela et al., 1997 ; Dittman et al., 2000 ). The sequence of
transmissions from the model synapses is significantly less correlated
than the input spike sequence for all three trains (Fig. 5, black
bars), although the long-tail autocorrelations (Fig. 5,
left, black bars) are not entirely removed, and a
negative autocorrelation is introduced into the train with low firing
rate and short-time autocorrelations (Fig. 5, right, black bars). Considering the range of different spike train
statistics exhibited by these trains, decorrelation appears to be a
robust effect.

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Figure 5.
Decorrelation of three typical spike trains
recorded from freely viewing monkeys. Black lines, Spike
trains from three recorded neurons showing strong positive
autocorrelations of differing magnitudes and time scales. Average
firing rates were left, 15.2 Hz; middle,
12.5 Hz; and right, 3.2 Hz. Black bars,
Corresponding autocorrelation of the transmissions through a model
synapse with Nmax=1, p =1,
and D = 150 msec. Percentages of presynaptic spikes
transmitted were left, 19%; middle,
27%; and right, 52%. The left,
middle, and right panels correspond to
neurons 14, 1, and 13, respectively, in Figure 4.
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Sustained firing with depressing synaptic input
Although depressing synapses decorrelate their inputs, neuronal
firing is autocorrelated, as we have discussed. If synapses decorrelate
their inputs, how can this be consistent with autocorrelated neuronal
firing? Here we provide an illustrative example of how delayed
recurrent input can resolve this apparent inconsistency.
Correlations arise in the saccade model and V1 spike trains, as well as
in other spike trains from animals viewing natural scenes (Baddeley et
al., 1997 ), from sustained periods of approximately constant firing at
a variety of rates over variable-length periods, with sudden steps
between these rates. We will show how autocorrelations may reappear in
the spike train of a postsynaptic neuron by showing how such periods of
sustained firing can occur.
The basic idea for maintaining sustaining firing is to recruit
additional inputs over time to compensate for the drive lost because of
synaptic depression. This is done by postulating that a group of
Nff direct inputs change rates rapidly
and approximately synchronously (compared with
D) in response to a stimulus. This response is
then followed by a set of Nrev delayed
inputs that change their rates later with various latencies. In this
arrangement (shown schematically in Fig.
6C), the coincident inputs
produce the initial step in the postsynaptic rate, and the delayed
inputs compensate for the depression of the coincident group of inputs, maintaining a sustained firing rate. In the context of a visually responsive neuron, this has a natural interpretation in terms of rapid,
feedforward input immediately after a saccade, followed by a set of
reverberatory inputs that arrive with variable latencies. We therefore
refer to the immediate, synchronous inputs as feedforward and call the
delayed inputs reverberatory.

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Figure 6.
Matching of input and output firing rates and
autocorrelations. A, Comparison of the postsynaptic
firing rate (solid line) of an integrate-and-fire neuron
receiving 30 inputs (as described in Results and in
C) with the firing rate of one of its feedforward inputs
(dashed line). The slight discrepancy between the input
and postsynaptic firing rates for the initial lower-rate segment arises
because the integrate-and-fire neuron fires more rapidly at low rates
than the linear model used in the calculation of the matching
conditions. B, Autocorrelation of one of 333 presynaptic
spike trains generated from the saccade model (black
line) and of the corresponding transmissions through one of the
model synapses (Nmax = 3;
p = 0.25; and D = 350 msec;
black bars). The other 667 presynaptic inputs were
generated by a 15 Hz constant-rate Poisson process. C,
Schematic of the pattern of arrivals of an identical change in rate for
the 333 saccade model afferents to the integrate-and-fire model neuron.
For the simulations, we have defined a fixed order in which neurons
switch rates for each simulated saccade. D,
Autocorrelation of the spike train generated by the postsynaptic neuron
(average rate, 15 Hz). The smaller autocorrelations in the first
two time bins reflect the postspike dynamics of the
integrate-and-fire neuron, an effect not included in the input
trains.
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In the Appendix, we show that a postsynaptic neuron will duplicate a
step in the firing rates of its inputs from an initial rate
r0 to a final rate
r1 provided that the numbers of
feedforward and reverberatory inputs are given by:
|
(4)
|
and provided that the latencies of the reverberatory inputs are
distributed exponentially with mean latency equal to
D. Here, k is a constant of
proportionality relating the firing rate of the postsynaptic neuron to
the rate at which it receives synaptic transmissions. Equation 4
implies that we require a fixed number of synchronously rate-switching
feedforward inputs and a number of delayed, reverberatory inputs that
increase linearly with the firing rate. This seems reasonable because a
stronger feedforward response is likely to recruit a proportionally
larger population of recurrently excited neurons. Substituting values
for the parameters into these equations gives an estimate for the
number of responsive inputs to a neuron. Assuming that
1/k = 20 EPSPs per spike, as would be the case if the
average EPSP caused a 0.5 mV depolarization and the difference between
the reset and firing threshold potentials of the postsynaptic neuron
was 10 mV (Shadlen and Newsome, 1994 ), and
r1 = 15 Hz, D = 380 msec, and p = 0.6 (Varela et al., 1997 ), we find
Nff ~ 35 feedforward inputs and
Nrev ~ 115 reverberatory inputs.
This gives a total of Nff + Nrev ~ 150 responsive inputs, a
number similar to what has been estimated on the basis of a different
argument using a consistent feedforward cortical model (Shadlen and
Newsome, 1998 ).
Figure 6A shows the results of applying this input
scheme to a leaky integrate-and-fire neuron (see Materials and Methods) with 30 inputs that jump from 10 to 30 Hz. The postsynaptic firing rate
(obtained by averaging over 100 repeats) reproduces the step in input
firing rates quite well and is sustained after the initial upward step.
Figure 6B-D demonstrates that this arrangement of
inputs also leads to a matching of the autocorrelations of spike train
of the postsynaptic neuron (Fig. 6D) to that of its
presynaptic inputs (one of which is shown in Fig. 6B,
black line). The autocorrelated postsynaptic firing occurs
despite the fact that the individual synaptic transmissions are
uncorrelated (Fig. 6B, black bars) and
reflects sustained periods of constant-rate firing that occur when
fluctuations produced by feedforward inputs are extended over
time by the reverberatory afferents. Such consistency of input
and output spiking statistics is necessary because of the strongly
recurrent nature of cortical circuits, in which a large fraction of the
inputs to a neuron come from neurons in the same local region with
similar firing statistics (Shadlen and Newsome, 1994 ).
The results shown in Figure 6B-D come from a
1000-input simulation, with one-third of the inputs generated by the
saccade model at an average rate of 15 Hz and the other two-thirds of the inputs, modeling background activity, generated from a
constant-rate Poisson process at 15 Hz. We fixed the number of saccade
model inputs at 333 and, at each saccade, assigned a fraction
Nrev/Nff = pr1 D of
these inputs to be reverberatory (i.e., to have delayed transitions in
firing rate). We did this because varying the total number of inputs at
each saccade in accordance with Equation 4 would require a model of how
reverberatory inputs are recruited from the background. We verified
that this approximation had only a small effect on the ability of the
model to reproduce input steps as in Figure 6A.
Similar results were obtained for the integrate-and-fire neuron with 30 saccade model inputs used for Figure 6A. The
background input in the 1000-input model primarily adds a baseline
level of depolarization, and its summed contribution is primarily
uncorrelated, although each individual input produces negatively
autocorrelated transmissions (Fig. 1), because the arrival times of the
inputs are uncorrelated.
Finally, we are not claiming that the particular model we have
presented is a unique solution to the problem of generating sustained
firing and autocorrelations. Rather, it provides an existence proof
that these patterns of firing are not inconsistent with the idea of
decorrelation by synaptic depression at individual synapses.
 |
DISCUSSION |
Autocorrelations in recorded spike trains suggest redundant
representation of information (Barlow, 1961 ; Atick, 1992 ). We have
shown that activity-dependent, stochastic synaptic transmission can
reduce this redundancy by removing autocorrelations (Figs. 2, 3, 5).
The tuning of synaptic time constants does not need to be precise to
achieve a significant decorrelating effect (Figs. 2, 5). Although
decorrelation is not strictly equivalent to information maximization,
it is an effective method of compressing the information in a redundant
signal. Furthermore, activity-dependent failures reduce total
transmissions, allowing for a more efficient use of synaptic resources.
In studying the optimal decoding of bursty spike trains recorded from
area MT during motion discrimination, Bair et al. (1994) found that the
best prediction of a monkey's responses was obtained when individual
spikes and individual bursts were weighted equally. This finding could
reflect transmission through synapses with a strong refractory form of
depression that allows transmission of an isolated spike or the first
spike of a burst with equal fidelity but that prevents subsequent,
redundant spikes in the burst from being transmitted.
We have focused on the role of synaptic depression in spike train
decorrelation, but other short-term processes such as spike rate
adaptation (Liu and Wang, 2001 ), synaptic facilitation (Lisman, 1997 ),
and postsynaptic receptor dynamics could allow more general filtering
of spike trains (Maass and Zador, 1999 ). In general, the forms and time
scales of short-term dynamics in different brain regions may be tuned
to the statistics of the spike trains in those regions.
Although synaptic depression removes autocorrelations at individual
synapses, neuronal spike trains exhibit autocorrelations that we have
shown may arise from the timing of and cross-correlations between
different inputs (Fig. 6). Thus, it might seem that the benefits of
decorrelation at single synapses are canceled by the effect of
cross-correlations across synapses. However, decorrelating individual synaptic inputs and then generating sustained firing from
the arrangement of inputs we have discussed may have several computational advantages. Depression in the feedforward connections and
synchrony across these inputs could allow a relatively small number of
feedforward inputs to have a relatively large influence on the firing
of the postsynaptic neuron during postsaccadic changes in firing rate.
Synchrony across the feedforward group of inputs may also remove noise
inherent in stochastic synaptic transmissions. Such spatial averaging
of synaptic noise, unlike temporal averaging, is instantaneous,
permitting fast and reliable responses to new inputs.
Cross-correlations among the reverberatory inputs may reflect positive
feedback loops in the highly recurrent cortical circuitry. Depression
in recurrent cortical connections may exist in part to dampen runaway
excitation in such circuitry (Thomson and Deuchars, 1994 ).
More generally, depressing synapses may underlie a mode of neuronal
computation in which individual postsynaptic spikes emphasize specific
temporal features of individual inputs, rather than responding equally
to all presynaptic spikes arriving along a particular input (Dobrunz
and Stevens, 1999 ). Whereas simpler models of neurons consider them as
nonselective integrators of their inputs, a postsynaptic neuron with
decorrelating synapses preferentially reflects interesting (i.e.,
nonredundant) features of its individual inputs. For the example of a
neuron receiving saccade model input as in Figure 6, the postsynaptic
spikes produced by a neuron with depressing synapses preferentially
reflect the jumps in firing rate that are the most prominent feature of
this input (Goldman, 2000 ). In this manner, decorrelating synaptic
inputs can provide a neuron with a matched filter that is tuned to the
statistics of its individual inputs (Abbott et al., 1997 ; Maass and
Zador, 1999 ).
The results in this article depend on an approximate coincidence of
time scales for several processes. The decay time constant for the
autocorrelations in the saccade spike trains,
corr, is directly related to the
characteristic time scale of the intersaccade intervals,
sacc. These autocorrelations can be removed by
stochastic depressing synapses with a recovery time,
D ~ corr, in the
same range as has been seen experimentally (Abbott et al., 1997 ;
Tsodyks and Markram, 1997 ; Varela et al., 1997 ). The consistency of
presynaptic and postsynaptic firing statistics results from matching
the characteristic spread in the latencies of reverberatory inputs,
delay ~ D, which
implies a corresponding time scale for network activity. Together, this
suggests that D ~ corr ~ delay sets a
basic time scale for cortical processing.
 |
FOOTNOTES |
Received July 20, 2001; revised Oct. 26, 2001; accepted Oct. 23, 2001.
This work was supported by National Institutes of Health Grant MH58754,
National Science Foundation Grant IBN-9817194, the Sloan Center for
Theoretical Neurobiology at Brandeis University, and the W. M. Keck Foundation. Experiments were performed in the laboratory of
Charlie Gray, and we thank him for his assistance. We thank Sacha
Nelson, Geoff Hinton, Ken Sugino, and John Birmingham for helpful discussions.
Correspondence should be addressed to Dr. Mark Goldman, Brain and
Cognitive Sciences, Massachusetts Institute of Technology, E25-210, 45 Carleton Street, Cambridge, MA 02139. E-mail:
mark_g{at}mit.edu.
 |
APPENDIX |
Number of synchronous and delayed inputs and distribution of
latencies for matched input-output responses
Here we show how sustained firing after a steplike rise in input
rates can be generated when synapses depress.
We postulate a group of Nff direct
feedforward inputs and a set of Nrev
delayed reverberatory inputs that all increase their firing rates from
an initial rate r0 to a final rate
r1. The feedforward inputs jump to the
rate r1 immediately, whereas the
reverberatory inputs remain at rate r0
for variable delay or latency periods and then jump to rate
r1. Immediately after the feedforward
inputs have jumped, the probability of release for all synapses is
Pss(r0) because of the preceding period of sustained firing at rate
r0 (see Materials and Methods). At
this time, the feedforward synapses transmit collectively at a rate
Pss(r0)r1Nff
because their presynaptic inputs fire at rate
r1. The reverberatory inputs transmit
at a total rate
Pss(r0)r0Nrev
because their input rates have not yet changed from
r0.
We assume that the firing rate of the postsynaptic neuron is
proportional to the rate at which it receives synaptic transmissions, with a proportionality constant k. Then the presynaptic
firing rate immediately after the jump in the rates of the feedforward inputs is, adding together the contributions of both feedforward and
reverberatory inputs:
|
(5)
|
Now consider the firing rate of the postsynaptic neuron long after
the initial jump in rates, when the feedforward and reverberatory inputs are all firing at rate r1. At this time,
the probability of release at all Nff + Nrev synapses is
Pss(r1)
because of the sustained firing at rate
r1. Thus, the transmission rate at
each synapse is
Pss(r1)r1,
and the postsynaptic firing rate is:
|
(6)
|
We now determine the conditions under which the firing rates at
the beginning (Eq. 5) and end (Eq. 6) of the period in question match
the input firing rate, that is, rpost = r1. Using Equation 1 for
Pss, we find:
|
(7)
|
which can be verified by substitution into Equations 5 and 6.
We next extend this result to times intermediate between the beginning
and end of the period. Suppose that the
Nff feedforward synapses transition
from rate r0 to
r1 at time t = 0. At
later times, these synapses transmit at a total rate (using Eq. 2):
The transmission rate for a reverberatory synapse that changes its
rate at time tstep, rather than at
time 0, is
r0Pss(r0) for t < tstep and:
for t tstep.
We now show that sustained firing at a constant rate is maintained by a
set of delayed, reverberatory inputs that have a latency distribution
exp( tstep/ delay)/ delay,
with delay a constant to be determined. Here
tstep indicates the time when the rate of a delayed input jumps from r0 to
r1. Adding up the contributions from
the feedforward and reverberatory inputs, we can write the postsynaptic
firing rate at time t > 0 as:
Although the algebra is a bit tedious, doing the integrals and
using the results of Equation 7, we find that
rpost(t) = r1 if delay = D. Note that the time constant governing the
decay of arrivals of steps matches the depression time constant
D, not the effective time constant
DPss(r1)/p
that appears in the exponentials throughout the calculation and governs
the decay of the feedforward group of inputs.
 |
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