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The Journal of Neuroscience, November 15, 2002, 22(22):9708-9720
Limit on the Role of Activity in Controlling the Release-Ready
Supply of Synaptic Vesicles
John F.
Wesseling and
Donald C.
Lo
Department of Neurobiology, Duke University Medical Center, Durham,
North Carolina 27710
 |
ABSTRACT |
Typical fast chemical synapses in the brain weaken transiently
during normal high-frequency use after expending their presynaptic supply of release-ready vesicles. Although it takes several seconds for
the readily releasable pool (RRP) to refill during periods of rest, it
has been suggested that the replenishment process may be orders of
magnitude faster when synapses are active. Here, we measure this
replenishment rate at active Schaffer collateral terminals by
determining the maximum rate of release that can still be elicited when
the RRP is almost completely exhausted. On average, we find that spent
vesicles are replaced at a maximum unitary rate of 0.24/sec during
periods of intense activity. Because the replenishment rate is similar
during subsequent periods of rest, we conclude that no special
mechanism accelerates the mobilization of neurotransmitter in active
terminals beyond the previously reported, several-fold, residual
calcium-driven modulation that persists for several seconds after bouts
of intense synaptic activity. In the course of this analysis, we
provide new evidence supporting the hypothesis that a simple enzymatic
step limits the rate at which reserve synaptic vesicles become ready to
undergo exocytosis.
Key words:
synaptic physiology; presynaptic; synaptic vesicle; priming; short-term plasticity; readily releasable pool
 |
INTRODUCTION |
Recently there has been considerable
interest in measuring the time required for reserve synaptic vesicles
to become available to participate in neurotransmission at CNS synapses
(Stevens and Tsujimoto, 1995
; Rosenmund and Stevens, 1996
; Dobrunz and
Stevens, 1997
; Stevens and Wesseling, 1998
; Wu and Borst, 1999
; Pyle et al., 2000
). This work is important because a complete picture of the
molecular basis of synaptic function requires a clear understanding of
the kinetics of the various steps in the synaptic vesicle cycle, in
addition to the identification of the enzymes involved. It is also
important from a computational perspective, because the rate at which
vesicles become ready to participate in synaptic transmission is a key
element that determines the means by which information can be
transferred between neurons via synapses.
Typical presynaptic terminals contain hundreds of vesicles loaded with
chemical transmitter, but at any given time, only a few of them are
functionally available to be released quickly (Schikorski and Stevens,
1997
, 2001
). This release-ready subset of synaptic vesicles constitutes
the readily releasable pool (RRP). When their RRPs empty during
episodes of heavy use, synapses exhibit short-term depression,
transiently becoming less reliable at transmitting information because
they can no longer consistently provide neurotransmitter for
intercellular signaling (Elmqvist and Quastel, 1965
; Rosenmund and
Stevens, 1996
).
Previous studies have primarily measured the time it takes for the RRP
to refill during periods of rest, most finding that recovery from
depletion takes at least several seconds (Birks and MacIntosh, 1961
;
Elmqvist and Quastel, 1965
; Stevens and Tsujimoto, 1995
; Rosenmund and
Stevens, 1996
; Wu and Borst, 1999
). The residual calcium that is
cleared slowly from synaptic terminals after bouts of intense activity
has been shown to accelerate the replenishment process several-fold
(Dittman and Regehr, 1998
; Stevens and Wesseling, 1998
, 1999a
; Wang and
Kaczmarek, 1998
). In those studies, however, the replenishment rate was
monitored only during rest intervals that followed active episodes. It
has been suggested that there may be an additional, qualitatively
different activity-dependent mechanism that can accelerate the rate at
which neurotransmitter becomes available for release to a much greater
extent during periods of intense presynaptic activity (Kusano and
Landau, 1975
), perhaps via a rapid refilling of the spent release-ready
vesicles themselves (Pyle et al., 2000
).
In this study we examined the extent to which the RRP replenishment
rate can be accelerated to counteract short-term depression during
heavy synaptic use. Using stimulation protocols that were sufficient to
drive the RRPs of Schaffer collateral synapses into a near-empty steady
state, we found that neurotransmitter becomes available for release
only approximately two or three times as quickly when these synapses
are active as it does during periods of rest, as predicted from the
residual calcium-dependent type of replenishment-rate acceleration that
has been reported previously (Stevens and Wesseling, 1998
). We thus
conclude that there is no special mechanism that accelerates the
preparation of neurotransmitter for release in active terminals beyond
this type of modulation that persists for several seconds after bouts
of repetitive activity.
 |
MATERIALS AND METHODS |
All synaptic responses were measured from patch-clamped neurons
held in whole-cell voltage-clamp mode.
Preparation. Experiments were performed on transverse slices
prepared from the hippocampi of 2- to 3-week-old mice. Mice were anesthetized by inhalation of halothane and decapitated soon after the
disappearance of reflexive reactions to tail and foot pinches. Brains
were removed rapidly and bathed in a chilled solution that had most of
the sodium ions replaced with sucrose (in mM):
230 sucrose, 1.25 NaH2PO4,
26 NaHCO3, 10 glucose, 3.5 KCl, 2.6 MgCl2, and 1.3 CaCl2. The
cerebellum and brain stem were dissected away, and 400-µm-thick
coronal slices of the remaining brain were cut using a vibrating
microtome. Hippocampal segments were dissected free, and area CA3 was
removed for all experiments except those in which recordings were made
of antidromic action potentials. The hippocampal slices were then
gently washed three or four times in the physiological recording
solution containing (in mM): 120 NaCl, 1.25 NaH2PO4, 26 NaHCO3, 10 glucose 3.5 KCl, 2.6 CaCl2, 1.3 MgCl2,
picrotoxin (50 µM), and
D(
)APV (50 µM), except
where indicated. Recording solutions were bubbled with a mixture of 95% O2 and 5% CO2 for at
least 20 min before addition of CaCl2 and
MgCl2. The slices were maintained in an interface
slice chamber and humidified with the same gas mixture for between 2 and 10 hr before being transferred to the submerged recording chamber.
Recording. Slices were submerged in the recording chamber
with a nylon mesh affixed to a platinum anchor. The solution in the 0.5 ml recording chamber was exchanged 5-10 times per minute with
continuously bubbled recording solution. Most recordings were performed
using 3-5 M
pipettes, filled with saline containing (in
mM): 130 Cs-gluconate, 5 CsCl, 5 NaCl, 2 MgCl2, 2 MgATP, 0.2 LiGTP, 1 EGTA, 0.2 CaCl2, and 10 HEPES. For experiments in which action potentials were fired antidromically, a solution containing (in
mM) 140 K-gluconate, 9 NaCl, 1 MgCl2, 2 MgATP, 0.2 LiGTP, 1 EGTA, 0.2 CaCl2, and 10 HEPES was used instead.
Intracellular solutions were adjusted to pH 7.2 and an osmolarity of
290 mOsm.
Stimulation. A monopolar silver/silver chloride electrode
inserted into a glass pipette (tip diameter between 20 and 40 µm) and
filled with recording solution was used for evoking action potentials
in the Schaffer collaterals for all experiments presented here.
EPSCs were evoked by up to 1 mA of current for 100 µsec. The
more commonly used bipolar electrodes made of tungsten transiently became substantially less effective at eliciting action potentials over
the course of single trials and were deemed unsuitable for these
experiments. The experiment summarized in Figure 1B
provides a good test for whether a stimulating device introduces
unanticipated errors into the sorts of experiments detailed here.
Because small changes in stimulus intensity can lead to large changes
in the number of axons stimulated (Allen and Stevens, 1994
), we stress that it is not adequate to instead monitor only changes in the size of
the electrical artifact associated with each stimulus.
Minimal stimulator settings (see Fig. 7) were determined during
low-frequency stimulation as the strength needed to elicit successful
synaptic transmission less than half of the time. To ensure that
transmission failures did not result from nerve conduction failures
arising from axonal threshold fluctuations, minimal intensities were
used only if it was possible to both increase and decrease the stimulus
intensity by several percentages without noticeably changing the
probability of release.
Drugs. NBQX (3 µM) was added
to block glutamatergic transmission for antidromic action potential
recordings. Stock solutions of cyclothiazide (CTZ) (20 mM) were made in DMSO and used at final concentration of 100 µM where indicated.
Kynurenic acid (KYN) was added in powder form directly to the recording
solution and then dissolved by vigorous stirring for several hours.
Experimental design. In general, it was often possible to
repeat several trials of each experiment on individual preparations. To
allow the synapses to recover completely between trials, at least 3 or
4 min was allowed for rest before high-frequency stimulation was
initiated (4 min for most; 3 min for the minimal stimulation experiments). For the experiments documented in Figures
1A, 4, 5, 6, and 7, the experimental and control
trials were alternated. The order of the different types of trials
summarized in Figure 3 was shuffled. Data were accepted only if the
access resistance was stationary throughout individual trials and also
from trial to trial when the object was to compare synaptic response
sizes between trials (see Figs. 1A, 4, 6, and 7).
Analysis. Synaptic size was measured as the slope of the
rising phase of the postsynaptic response estimated by fitting the rising segment between 30 and 60% of the peak with a linear least squares fit. EPSCs recorded at
20 Hz were also measured as the current integral of the synaptic response to confirm that the relative
measurements of short-term depression were accurate. Because typical
synaptic responses took >25 msec to decay, measurements of synaptic
potentials recorded at 40 Hz were adjusted for the slope of the
baseline response over the 5 msec that preceded the stimulus artifact
(<15% of total measure). For 20 Hz stimulation, a similar correction
did not contribute substantially to the measure. Because the rising
phase of the smallest recordings made in 1000 µM KYN were significantly contaminated by the
stimulus artifact, the sizes of both the control and experimental
recordings that involved this concentration of KYN were quantified as
the current integral between 15 and 24 msec after the stimulus artifact.
 |
RESULTS |
We studied the rate at which vesicular packets of transmitter
become available for release at excitatory glutamatergic synapses between hippocampal Schaffer collaterals and the CA1 pyramidal neurons
in transverse slice preparations. When long-term changes are blocked
pharmacologically with NMDA receptor antagonists, activity does not
affect the sensitivity of the postsynaptic receptors at these synapses;
the size of the postsynaptic response elicited by the release of
transmitter quanta stays constant during periods of intense use
[Dobrunz and Stevens (1997)
; and see a series of control experiments
presented below]. This allowed us to monitor the rate of transmitter
release during Schaffer collateral stimulation with standard
electrophysiological recordings of postsynaptic CA1 neurons.
Sixty action potentials at 20 Hz exhaust the RRP
To measure the rate at which vesicles are prepared for exocytosis
in active terminals, we developed a stimulation protocol that was
sufficient to exhaust the RRP. Pilot experiments conducted on neurons
grown in cell culture [similar to those described in Rosenmund and
Stevens (1996)
] indicated that 40 or fewer action potentials in a
high-frequency train only partially emptied the RRPs of those synapses,
but that trains consisting of at least 60 action potentials were
sufficient to completely exhaust the pools (data not shown).
Because the technique used in the cell culture system to check RRP
fullness is not available in the slice preparation, an alternate test
was devised that involved switching the frequency of stimulation during
a repetitive train. Because readily releasable vesicles are
functionally defined as the ones that are triggered for exocytosis
directly by action potentials, increasing the stimulation rate when the
RRP is still partially full should cause the rate of exocytosis to
increase. Conversely, when the pool is empty, the synaptic strength is
limited by the time it takes for fresh quanta of transmitter to become
available for release, and that rate apparently does not change with
stimulus frequency (Eccles and Rall, 1951
; Curtis and Eccles, 1960
;
Elmqvist and Quastel, 1965
; Abbott et al., 1997
; Tsodyks and Markram,
1997
; Stevens and Wesseling, 1998
). We thus reasoned that if the RRP
was left empty by a train of 60 action potentials, subsequently
doubling the stimulation frequency would not change the overall rate of exocytosis.
Figure 1 shows that 60 action potentials
fired at 20 Hz nearly completely empty the RRPs of these synapses.
Schaffer collaterals were stimulated 60 times at 20 Hz and then 21 more
times either at 40 Hz or at 20 Hz as a control (Fig.
1A). During a brief settling time, the synaptic
strength recorded at 40 Hz depressed quickly to one-half that recorded
at 20 Hz (Fig. 1A, bottom versus top dashed lines). Because there were twice as many stimulations for each unit of time during the faster stimulation, the overall steady rate of release was the same at both frequencies. Thus, suddenly doubling the stimulus frequency to 40 Hz did not substantially increase
the rate of transmitter release, suggesting that 60 action potentials
at 20 Hz are sufficient to almost completely exhaust the RRP.

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Figure 1.
The RRP is emptied by 60 action potentials at 20 Hz. A, Schaffer collaterals were stimulated 60 times at
20 Hz and then 21 more times either at 40 or 20 Hz while
postsynaptic responses were recorded by patch clamping CA1 pyramidal
neuron somata. Fluctuations caused by the quantal nature of transmitter
release, including frequent transmission failures, dominated the
recordings during the 40 Hz stimulation, and so traces were averaged
across all experiments before being measured (each point represents the
average of 18 trials from 4 slices). The synaptic response sizes were
binned in groups of three, normalized by the size of the first
response, and plotted versus the stimulus number.
Diamonds represent responses of synapses stimulated at
20 Hz throughout; circles are from trials where the
frequency was doubled. The filled circles represent 20 Hz responses; the open circles are 40 Hz responses. The
value of the first bin is greater than 1 because of the short-term
enhancement apparent during the first several responses. The top
gray dashed line matches the steady-state response size for the
last 21 responses when recorded at 20 Hz; the bottom
line is drawn at exactly half that. Note that during the 40 Hz
stimulation, the synaptic strength quickly settled to half that
recorded at 20 Hz, matching the bottom dashed line and
indicating that the RRP is left exhausted by the first 60 action
potentials. Inset, The averages of the first 10 individual responses at 20 Hz, responses numbered 51-60 at 20 Hz, and
the first 10 responses at 40 Hz are all scaled by their peak size and
overlaid. Because the individual responses evoked at 40 Hz do not decay
away completely in the 25 msec interstimulus interval, the
corresponding tail of the average 20 Hz response was first scaled to
match the prestimulus artifact baseline and then subtracted from the
average 40 Hz response. Note that the shape of the EPSC did not change
during the experiment. B, The stimulus intensity was set
within the narrow threshold window as described in Results, and
antidromic action potentials were recorded in CA3 pyramidal neurons as
Schaffer collaterals were stimulated repetitively for 3 sec at 20 Hz
and then for 1 sec at 40 Hz. The average probability of action
potential firing given a stimulus (47 experiments, 2 neurons) was
calculated for each second of stimulation and plotted versus time. Note
that the firing probability did not change when the stimulus frequency
was doubled (compare bars 3 and
4).
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This logic is valid only if the stimulating apparatus successfully
evoked action potentials in the same axons after each stimulus. For
example, it is possible that 20 Hz might represent an upper limit on
the rate of action potential firing, in which case, increasing the
stimulation frequency to 40 Hz would not increase the overall spike-firing rate in individual Schaffer collaterals. To control for
this possibility, antidromic action potentials were recorded in the
cell bodies of CA3 pyramidal neurons during a frequency-switching stimulation protocol similar to the one used above. Using this approach, the stimulating apparatus was found to have no problem evoking action potentials up to rates of at least 40 Hz.
To test rigorously whether changing the stimulus frequency had an
effect on the excitability of Schaffer collaterals, we examined the
firing behavior of axons when they were stimulated with the minimum
strength that was required to evoke action potentials. By carefully
adjusting the stimulation strength, we found a narrow range of settings
in which a fraction of the stimuli would fail to trigger a regenerative
current. This threshold window allowed the quantification of very small
changes in axonal excitability over the course of the experiment
[Allen and Stevens (1994)
and references therein].
Figure 1B shows that the average probability of
firing did not change substantially during the experiment. Analysis was
limited to trials during which some, but not all, of the individual
stimuli during the first second of stimulation failed to elicit action potentials. No change was detected in the effective excitability of the
Schaffer collaterals when the stimulation frequency was switched from
20 to 40 Hz (Fig. 1B, compare bar 3 vs
bar 4). This experiment confirms that the stimulating
apparatus was effective at evoking action potentials in the Schaffer
collaterals at the frequencies used for this study. Taken together,
these results indicate that doubling the frequency of presynaptic
action potential firing did not substantially increase the rate of
exocytosis in these experiments, confirming that a 20 Hz train of 60 action potentials is sufficient to nearly completely exhaust the RRPs of these synapses.
Residual steady-state RRP fullness
How close to empty is the pool after 3 sec of 20 Hz stimulation?
The RRP is never expected to be truly empty for long periods because
the replenishment process continuously supplies fresh quanta of
transmitter to replace the spent ones. The average level of the
remaining steady-state fraction depends on both the pool replenishment
rate and the rate at which vesicles undergo exocytosis once they become
available. Below, we introduce a formal model of pool replenishment
that is used in the Appendix to show that doubling the stimulation
frequency should lower the standing steady-state fullness of the RRP by
a factor of ~2. As detailed in the Appendix, the steady-state levels
of fullness at both stimulation frequencies can be estimated from the
small, transient increase in the transmitter release rate that occurs
as the sizes of the individual responses settle to a new steady state
after the stimulus frequency is doubled. For the experiments documented
in Figure 1A, the brief release rate increase was
quantified from the small difference in the sum of the responses
elicited by 40 Hz stimulation compared with the corresponding sum of
responses during 20 Hz stimulation. The extra amount of release
elicited by the 40 Hz stimulation was <2% of the aggregate response
elicited by the first 60 stimuli. We show in the Appendix how this
predicts that the RRPs of these Schaffer collateral synapses were <5%
full after 60 stimulations at 20 Hz.
The RRP replenishment rate is slow at active synapses
The preliminary studies confirmed that our experimental
preparation was appropriate for measuring the replenishment rate of the
RRP at active synapses by showing that trains of at least 60 stimuli
(20 Hz) are sufficient to drive the RRP into a near-empty steady state.
Because synaptic vesicles can undergo exocytosis only after having been
readied for release, the rate at which fresh transmitter becomes
available defines the sustained rate of release when the RRP is in such
a state. Likewise, the overall rate of transmitter release must be
equivalent to the rate of RRP replenishment so long as stimulation is
rapid enough to keep the pool in the near-empty steady state. An
estimate of the rate constant for RRP replenishment can be determined
by dividing this sustained rate of release from exhausted terminals by
the total capacity of their RRPs.
Lower bound for replenishment rate
The sum of all the responses evoked by the first 60 action
potentials in a 20 Hz train yields an overestimate of the RRP capacity. Because such a stimulus train leaves the RRP nearly empty, the sum of
the responses must reflect release of the entire content of the pool,
an amount that is equivalent to the RRP capacity if stimulation is
initiated when the RRP is full. The replenishment process is
continuous, however, so some fraction of the cumulative response
reflects release of transmitter that became available during the 3 sec
of stimulation.
The average response size during subsequent 20 Hz stimulation is
directly proportional to the amount of pool replenishment that occurs
during the brief interstimulus intervals, because each action potential
leaves the RRP just as depleted as the previous one. Dividing the
average response size during the fourth second of 20 Hz stimulation by
the sum of the response sizes elicited by the first 60 action
potentials yields a value of 0.75% for the data plotted in Figure
2A (14 slices). Because
there are 20 action potentials per second, this translates into a
standard rate constant of 0.15/sec. This would be the value of the RRP replenishment rate constant if no replenishment occurred during the
first 3 sec of stimulation, and the sum of the first 60 responses was
thereby directly proportional to the pool capacity. However, because
the sum of the responses during the first 3 sec of stimulation is an
overestimate of the true RRP capacity, 0.15/sec represents a lower
bound for the RRP replenishment rate constant at active Schaffer
collateral synapses.

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Figure 2.
Readily releasable vesicles are replaced slowly
during 20 Hz stimulation. A, Average relative synaptic
strength is plotted as the Schaffer collaterals are stimulated at 20 Hz
for 4 sec (each response was normalized by the size of the response to
the first stimulus; experiments are from 14 slices). The
dashed gray line represents the fraction of the synaptic
response that is predicted to result from the exocytosis of vesicles
that became available for release during the experiment (as derived in
the Appendix). B, Working model of RRP replenishment.
Left panel, In the resting synapse the spontaneous rate
of exocytosis is low, and the RRP fills completely. The pool has a
maximum capacity, and the high-energy barrier that keeps vesicles from
fusing spontaneously is the rate-limiting element that controls how
quickly synaptic vesicles undergo exocytosis. Right
panel, Episodes of high-frequency activity drive exocytosis
quickly enough to exhaust the RRP. With the pool empty, the rate at
which new vesicles are made available limits the rate of transmitter
release; the energy barrier to fusion prevents vesicles from undergoing
exocytosis in the interval between action potentials, but as long as
the high-frequency spike train continues, the barrier is no longer the
rate-limiting element in the exocytic/endocytic cycle. This model
accounts only for rate-limiting steps in the exocytic/endocytic cycle
during the first several seconds of heavy use. Thereafter an additional
element plays a role in controlling the dynamics of neurotransmitter
mobilization. Endocytosis does not play a rate-limiting role in this
scheme and is not represented here. C, The simultaneous
solutions for Equations 1A and 3A (Appendix) are plotted for the data
shown in A. The two independent equations relate the
rate constant of pool replenishment to the fraction of the full pool
triggered to release by isolated action potentials (fusion efficiency).
When the corresponding values for the two parameters are plotted
against each other, the resulting lines intersect where the refilling
rate constant equals 0.24/sec and the initial fusion efficiency is
0.044. Equation 1A depends only on the steady-state response size after
the pool has reached a near-empty steady state and is represented by
the gray diagonal line. Equation 3A depends on the
changing rate at which transmitter was released over the complete
course of the experiment and is represented by the black
line. D, The initial fusion efficiency and the
pool replenishment rate constant were estimated separately by
simultaneously solving Equations 1A and 3A for each of the 14 experiments summarized in A and plotted versus each
other. Note that there is no evident correlation between these two
parameters.
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Upper bound for replenishment rate
An upper bound can be calculated by assuming that the amount of
RRP replenishment during each of the first 3 sec of stimulation is the
same as it is during the fourth second when the refreshment rate can be
estimated as the rate of exocytosis. If so, the release of freshly
prepared transmitter would account for ~45% of the sum of responses
elicited during the first 3 sec of stimulation. Excluding this fraction
yields a rate constant for RRP replenishment of 0.28/sec. The release
of replacement neurotransmitter is responsible for <45% of the
cumulative quantity released, however, because the amount of
replenishment during the first 2 sec of stimulation when the RRP is
still partially full must be less than the corresponding quantity when
almost all the release sites are vacant. The actual rate constant
describing RRP replenishment therefore must fall somewhere between the
lower 0.15/sec estimate and 0.28/sec.
We note that this upper bound is based on the generally accepted
classic concept that a functionally definable RRP does indeed exist
(Elmqvist and Quastel, 1965
) and that the short-term depression observed during the first several seconds of heavy use is not caused
instead by a progressive reduction in the ability of presynaptic terminals to mobilize other internal transmitter stores. It is likely
that this is a valid principle because most of the alternative possibilities can be ruled out on the basis of data published previously elsewhere (Rosenmund and Stevens, 1996
; Dobrunz and Stevens,
1997
; Stevens and Wesseling, 1999a
). Below, we provide an additional
set of experiments designed to test even more thoroughly the integrity
of the RRP itself.
A simple kinetic model for RRP replenishment
First, and to pinpoint the RRP replenishment rate constant within
the range determined above, we present a quantitative model that allows
us to gauge how much of the cumulative synaptic response was caused by
the release of transmitter that became available during the experiments
described above. Our simple model is depicted schematically in Figure
2B and is represented formally by Equation 1:
|
(1)
|
where the rate constant of pool filling,
, is the parameter
that we evaluate,
is the unitary rate of exocytosis,
n represents the number of vesicles available for release,
and N is the capacity of the RRP (i.e., the total
number of release sites in the RRP).
Equation 1 describes a realistic general model of RRP dynamics during
the first several seconds of high-frequency use. It assumes a pool of a
fixed size (N) containing individual sites that fill
independently with first-order kinetics. The differential equation is
equivalent to the one used to characterize the kinetics of pool
replenishment in one of the earliest papers describing the time course
of RRP refilling at central synapses (Stevens and Tsujimoto, 1995
).
Several nontrivial predictions of the model have since been tested, and
it remains the simplest scheme that is consistent with what is known
about the kinetics of RRP replenishment. For example, the rate at which
vesicles leave the RRP without undergoing exocytosis has been shown to
be slow compared with the rate of pool filling (Murthy and Stevens,
1999
). This, along with other observations (Stevens and Wesseling,
1998
, 1999b
; Pyott and Rosenmund, 2002
), implies that the pool has a
fixed size and is not instead in some steady-state equilibrium with a
larger reserve pool (the reverse reaction would formally be a
negligible component of
). An additional rate-limiting element in
the synaptic vesicle exocytic/endocytic cycle plays a role during more
extensive use (Stevens and Wesseling, 1999b
).
Equation 1 provides enough constraints to calculate the replenishment
rate constant (
) from the data plotted in Figure
2A, as outlined in the Appendix. The fraction of the
total response generated by transmitter that became available for
release after stimulation was initiated is plotted as a dashed
line in Figure 2A. The simultaneous solution of
two independent equations derived from Equation 1 (Eqs. 1A and 3A)
yields an average value for
of 0.24/sec for the experiments
summarized in Figure 2A (n = 14 slices). Although it is possible to devise alternative models that
generate slightly different estimates, the actual refreshment rate
could not be much faster, because this estimate is close to the upper bound (0.28/sec) derived without the constraints of a specific model.
It thus typically takes several seconds for fresh packets of
neurotransmitter to replace the expended readily releasable supply
during episodes of intense synaptic use.
Estimates of fusion efficiency
Equation 1 also provides information about the efficiency with
which action potentials trigger exocytosis that can be used as a
consistency check for the logic presented so far. Although the present
analysis does not provide meaningful absolute units for N
because neither the number of synapses activated simultaneously nor the
quantal response sizes are known, the fraction of the RRP that was
triggered to undergo exocytosis by the first action potential in each
20 Hz train can be calculated by dividing the size of the first
response by N. This fraction is termed the initial fusion
efficiency because it represents the efficiency with which isolated action potentials trigger the release of available vesicles at
resting synapses (Stevens and Wesseling, 1999a
). The common solution
for Equations 1A and 3A yields a value for this parameter of 0.044, for
the experiments summarized in Figure 2. (The individual solutions for
the two equations for the data plotted in Fig. 2A are
plotted in Fig. 2C.) This value fits within the published range of 0.03-0.07 for these synapses, giving us confidence that our
approach measures the same kinetic elements that have been studied
previously (Dobrunz and Stevens, 1997
; Schikorski and Stevens, 1997
).
Although we did observe a significant amount of heterogeneity between
preparations in both the rate of RRP replenishment [range, 0.13-0.36;
coefficient of variation (CV) = 0.33; see also Stevens and
Wesseling (1998)
] and the initial fusion efficiency (range
0.022-0.13; CV = 0.52), Figure 2D shows that
the variation was not correlated between the two parameters
(r = 0.01).
Slowly dissipating, activity-dependent acceleration of the
replenishment process
Is neurotransmitter prepared for exocytosis much more quickly at
active nerve terminals than at quiescent ones? The average replenishment rate constant of 0.24/sec that we have determined for the
RRPs of active Schaffer collateral synapses is not much faster, if at
all, than the resting refreshment rate measured at similar types of
synapses grown in cell culture [which range from 0.09/sec to 0.4/sec
(Stevens and Wesseling, 1998
)]. To compare the replenishment rate
during high-frequency stimulation with the rate during rest intervals
at the same Schaffer collateral synapses, we measured the complete time
course over which the RRP refills after being depleted.
The experimental strategy used is conceptually similar to previously
published methods (Stevens and Tsujimoto, 1995
; Stevens and Wesseling,
1999b
). Experiments were conducted during which the pool was emptied
two times in succession, with an experimentally varied rest interval as
diagrammed at the top of Figure 3. Trains of action potentials (80 at 20 Hz) were used instead of osmotic shocks
to elicit exocytosis from the synaptic terminals. An estimate of pool
refilling during the rest interval was derived by dividing the sum of
the first 60 responses during the second stimulus train by the
corresponding sum of responses evoked by the first one. To account for
the steady-state amount of release that persists after the RRP has
already been exhausted, the sums were first adjusted by subtracting the
equivalent measure derived from experiments when no time was allowed
for recovery between the two stimulus trains.

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Figure 3.
The RRP replenishment time course during periods
of rest is predicted by the refreshment rate when synapses are active.
The RRP was emptied with 80 action potentials (20 Hz), and subsequent
recovery was monitored after an experimentally varied delay with an
identical burst of stimulation (diagrammed at top). The
sums of the responses to the second stimulus train were normalized as
described in Results and plotted against the recovery interval.
The curve is the predicted RRP refilling time course calculated with
Equation 2 from the replenishment rate measured when the synapses were
active (0.30/sec for these synapses; mean ± SEM; 9 cells, at
least 10 trials for each point). Inset, Average synaptic
strengths of the responses elicited during the first and second
stimulus trains for the 2 sec recovery interval are plotted versus time
during the trial (filled circles represent the
responses that were used to estimate the RRP recovery after 2 sec of
rest, i.e., the first 60 responses of each stimulus train).
|
|
As anticipated from Stevens and Wesseling (1998)
, the replenishment
rate at Schaffer collateral synapses during long recovery periods is
somewhat slower than the value for
estimated when the
synapses are active. If the replenishment process remained constant
after stimulation ceased, Equation 1 would predict a single exponential
time course of refilling with a time constant of 3.3 sec (i.e., 1/
,
= 0.30/sec for this particular set of synapses). Instead,
however, the recovery time course was more closely approximated by a
somewhat slower, 5 sec exponential (recovery data are plotted in Fig.
3; the single exponential is not shown). This difference was expected
because the residual calcium that accumulates in presynaptic terminals
during high-frequency use has been shown to accelerate the
replenishment process several-fold (Stevens and Wesseling, 1998
).
During subsequent periods of rest, the rate diminishes gradually as
residual calcium is pumped out of the terminals. Equation 1 can be
modified to account for the decaying effect of residual calcium during
rest intervals, yielding:
|
(2)
|
where
(t) is no longer a constant but decays to
baseline along a single exponential with a time constant of 10 sec
during periods of rest (Stevens and Wesseling, 1998
). If
(t) starts at 0.30/sec at the beginning of the recovery
period and then slows down threefold, Equation 2 yields the
dashed line in Figure 3, which provides a good approximation
for the recovery time course.
The estimate of the RRP replenishment rate at active synapses is thus
consistent with the measured time course of pool refilling during
subsequent periods of rest. The slowly decaying, residual calcium-dependent acceleration appears to be the only significant kinetic element that increases the rate at which neurotransmitter becomes available for release during periods of heavy use.
Pool capacity does not depend on the measurement methodology
Although the conclusion that it takes several seconds for fresh
vesicles laden with neurotransmitter to be prepared for exocytosis at
active synapses does not depend on the particular formal theory used to
calculate the RRP refreshment rate, it is based on the classic concept
that a functionally definable subset of the synaptic vesicles is
available for action potential-triggered exocytosis. To test this
generally accepted assumption more thoroughly, we investigated the
effects of changing either the efficiency with which individual action
potentials trigger the exocytosis of readily releasable vesicles, or
the rate of stimulation, on our measure of pool capacity.
Calcium
Raising the extracellular concentration of calcium enhances the
strength of resting synapses by increasing the efficiency with which
action potentials trigger exocytosis of release-ready vesicles, whereas
magnesium has the opposite effect [Stevens and Wesseling (1999a)
and
references therein]. Changing the ratio of the two divalent ions
should not affect measurements of RRP capacity if the RRP is a pool of
fixed size.
The capacity of the pool was measured from the responses to 80 stimuli
(20 Hz), with either 4.5 mM Ca/0.5 mM Mg or 2.5 Ca/2.5 Mg in the bath; the normalized response sizes are plotted in
Figure 4Ai. The total
divalent ion concentration was kept constant because axonal
excitability can be influenced by this parameter (Frakenhaeuser and
Hodgkin, 1957
). At the higher calcium concentration, the average size
of the first synaptic response during stimulation was approximately twice the size of the corresponding one measured with the lower calcium
concentration in the bath. The synaptic strength depressed so much more
quickly in higher calcium, however, that the sums of all 80 responses
were statistically indistinguishable between the two conditions.

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Figure 4.
The capacity of the RRP does not depend on the
measurement protocol. A, Short-term depression was
induced with 80 stimuli (20 Hz) with either 2.5 mM Ca/2.5
mM Mg (squares) in the bath or 4.5 Ca/0.5 Mg
(circles) at the same synapses. i,
Responses were normalized by the average size of the first response
recorded at the lower calcium concentration and plotted versus stimulus
number (3 slices, 7 trials for each). ii, The RRP
replenishment rate constant and the initial fusion efficiency were
calculated by simultaneously solving Equations 1A and 3A, as in Figure
2C. The gray lines represent the analysis
of responses evoked under the high calcium condition; the black
lines are for the lower calcium experiments. The dashed
lines represent the solutions for Equation 1A; the solid
lines represent Equation 3A. Points of intersection represent
the common solutions. Note that, as predicted, the fusion efficiency in
high calcium is greater than the fusion efficiency in low calcium by a
factor similar to the amount of enhancement in synaptic strength
observed after switching into the higher calcium-containing solution.
B, Depression was induced with 81 stimuli at 20 and 40 Hz for the same synapses. i, The response sizes were
normalized by the average size of the first responses in the stimulus
trains and plotted versus stimulus number for both sets of trials (3 slices, 11 trials for each). ii, Simultaneous solution
of Equations 1A (dashed lines) and 3A (solid
lines). The gray lines represent the analysis of
the 40 Hz responses; black lines represent the analysis
of 20 Hz responses.
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|
Neither the RRP capacity nor the replenishment rate calculated as
outlined in the Appendix differed significantly between conditions. The
measured capacity was slightly larger under the high calcium condition
(9%), and the replenishment rate was slightly lower (0.26 vs
0.31/sec), both differences reflecting a nonsignificantly lower (5%)
average steady-state response to the final 20 stimuli under the high
calcium condition. As expected, the increase in the initial fusion
efficiency calculated from the simultaneous solutions of Equations 1A
and 3A for both sets of data (Fig. 4Aii) closely
matched the increase in synaptic strength that occurred when the
calcium to magnesium ratio was increased.
Stimulation frequency
The measurement of RRP capacity should also be independent of the
particular stimulation protocol used to empty it. To test this, pool
capacity was measured from 80 responses generated at either 20 or 40 Hz
(Fig. 4B). Although the sum of the responses evoked
by the first 60 stimuli at 20 Hz was 28% greater than the corresponding sum of responses to 60 action potentials recorded at 40 Hz, this difference was expected because there was twice as much time
for replacement transmitter to become available for release during the
slower stimulus trains. When this factor is taken into account as
outlined in the Appendix, the resting capacity estimated from the
responses evoked by the 20 Hz stimulation was within 5% of the value
derived from the 40 Hz trials. The solutions of Equations 1A and 3A are
plotted in Figure 4Bii. As expected, the RRP
replenishment rate constants were similar for the two data sets
(0.29/sec for the 40 Hz stimulation protocol and 0.26/sec for the 20 Hz protocol).
Together, these results indicate that the capacity of the RRP does not
depend on the particular protocol used to measure it. They provide
support for the general concept that the neurotransmitter used for
synaptic signaling is drawn from a nonarbitrary RRP (Birks and
MacIntosh, 1961
; Elmqvist and Quastel, 1965
) and for our particular model of RRP replenishment (Eq. 1).
A test of Equation 1 in particular
Further analysis of the experiments already summarized in Figure
1A provides another, independent test of our specific
model. In addition to predicting the average fullness of the RRP under near-empty steady-state conditions, Equation 1 provides enough constraints to predict quantitatively the time course of transition over which a new steady state is achieved when the frequency of stimulation is suddenly doubled, as it was in those experiments. The
predicted time course follows a single exponential with a time constant
of 94 msec (as derived in the Appendix). Figure
5 shows that this prediction corresponds
well with the observed time course of decay in synaptic strength.

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Figure 5.
The working model predicts the synaptic response
settling time course when the stimulation frequency is doubled after
the RRP has been emptied. The circles represent the
relative synaptic strength during the 40 Hz stimulation (also plotted
on a smaller scale as open circles in Fig.
1A). The dashed line is the
prediction generated by Equation 1 in the Appendix and depends on the
integral of the small transient increase in the overall rate of
exocytosis that occurs after switching frequencies from 20 to 40 Hz.
|
|
Controls indicating that postsynaptic responses linearly track
exocytic rates
As mentioned above, the analysis presented in this report relies
on the assumption that postsynaptic responses can be used as linear
detectors of the amount of transmitter release at these synapses during
20 and 40 Hz use. This would not be a valid assumption for some other
types of central synapses in which postsynaptic elements of short-term
plasticity have been observed. Following are a series of controls
designed to confirm the conclusions of earlier reports (Dobrunz and
Stevens, 1997
) indicating that postsynaptic receptors faithfully track
transmitter release at the Schaffer collateral synapses used in this study.
Receptor desensitization
At some types of synapses, postsynaptic receptor desensitization
contributes to short-term depression (Trussell et al., 1993
). To
confirm that receptor desensitization did not contribute to the rapid
decrease in synaptic strength that occurred during stimulation frequencies of 20 and 40 Hz, or when the stimulating frequency was
increased during stimulation, experiments similar to those documented
in Figures 1A and 4B were conducted
in the presence and absence of 100 µM CTZ, a
drug that blocks glutamate receptor desensitization (Patneau et al.,
1993
; Yamada and Tang, 1993
).
Figure 6A shows that
receptor desensitization does not play a role in the short-term
depression observed in these experiments. CTZ did cause a 12% increase
in the amplitudes of the synaptic responses, an effect that may be
attributable to alleviation of receptor desensitization that ordinarily
partially shapes individual postsynaptic responses or to some other
effect of CTZ on glutamate receptor kinetics (Yamada and Tang, 1993
).
However, the relative increase was the same for all responses elicited
by the stimulus trains, as reflected in the slope of 1.12 for the
straight line in Figure 6Aii. Postsynaptic
receptor desensitization thus played no apparent role in short-term
depression even at stimulation rates as high as 40 Hz.

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Figure 6.
CTZ and KYN do not affect short-term
depression. Ai, Forty Hertz stimulation. Schaffer
collaterals were stimulated 80 times at 40 Hz in the presence and
absence of 100 µM CTZ. Average responses to the stimulus
trains with (gray traces) and without
(black traces; scaled by 1.12) CTZ are plotted (data are
from 4 slices, 18 trials for each). The first six responses are plotted
in the top panel. Note that CTZ amplified the first
response slightly more than the rest, possibly because of presynaptic
side effects of the drug. The entire electrophysiological recordings
(the trace gathered in the absence of drug is scaled by 1.12), with the
stimulus artifacts blanked (2 msec windows), are plotted in the
bottom panel. Aii, Twenty Hertz and
frequency switching. Schaffer collaterals were stimulated 60 times at
20 Hz and then 21 more times at 40 Hz as in Figure
1A in the presence and absence of 100 µM CTZ. The size of the synaptic response to each
stimulus was normalized by the average size of the first control
response (no drug). The size of each response recorded in CTZ is
plotted against the size of the corresponding control response to the
same stimulus number (open circles represent responses
at 40 Hz; filled circles are 20 Hz responses). The
dashed gray line is straight, with a slope of 1.12 (3 slices, 10 trials each). Inset, The average current
traces representing the responses to the 20 stimuli preceding and after
the frequency switch for each condition are overlaid (the response
recorded in the absence of drug was scaled by 1.12; the larger of the
two sets of current deflections represents responses recorded at 20 Hz;
the baseline of the 40 Hz response average was calculated and
subtracted as for the inset of Fig.
1A). Note that the scaled responses with and
without drug are identical and that the average 40 Hz response size is
approximately half that recorded at 20 Hz. B, Schaffer
collaterals were stimulated at least 80 times at 40 Hz alternately in
the presence and absence of KYN (300 µM: 3 slices, 22 trials each; 1000 µM: 3 slices, 10 trials each). The
normalized sizes of the control responses are plotted against the
corresponding sizes of the responses gathered with KYN in the bath for
each stimulus (i, 300 µM KYN;
ii, 1000 µM KYN). The dashed
lines are straight with slopes of 0.34 (i) and 0.22 (ii).
|
|
Receptor saturation and voltage-clamp errors
The glutamate receptor antagonist KYN was used in an additional
control designed to test for other unanticipated nonlinearities in the
postsynaptic response to the release of neurotransmitter at 40 Hz. For
example, it has been suggested that the glutamate released from a
single vesicle may bind to between 70 and 90% of all receptor binding
sites, saturating the response at individual synapses (Jonas et
al., 1993
; Diamond and Jahr, 1997
) (but see Liu et al., 1999
;
McAllister and Stevens, 2000
). If multiple vesicles are released
simultaneously more often at individual synapses when the probability
of release is high, this phenomenon might have affected the linearity
of our postsynaptic measurements and caused us to underestimate the
true amount of depression in the release of transmitter from the
presynaptic terminals (for review, see Auger and Marty, 2000
). A large
space/voltage-clamp error in our patch-clamping technique could have
had a similarly misleading effect.
Synaptic responses to 80 stimuli (40 Hz) were recorded in the presence
and absence of 300 and 1000 µM KYN in separate sets of
experiments. KYN competitively blocks glutamate binding to the non-NMDA
ionotropic receptors used to track transmitter release in this study.
This drug dissociates rapidly enough on the time scale of transmitter
clearance from the synaptic cleft that it lowers the effective affinity
of the glutamate receptors for glutamate (Diamond and Jahr, 1997
). The
same quantitative models that predict glutamate receptor saturation
during normal synaptic transmission also predict that, in addition to
partially blocking the synaptic response,
300 µM KYN
should shift the dose-response relationship between transmitter
release and postsynaptic response size well into the linear range
(Diamond and Jahr, 1997
). Figure 6B shows that
neither treatment affected the accumulation of short-term depression, however, indicating that receptor saturation does not
introduce a nonlinear component into our postsynaptic measure of
transmitter release. Furthermore, KYN did reduce the overall synaptic
strength substantially (66% in 300 µM KYN,
78% in 1000 µM KYN), making it unlikely that
voltage-clamp errors contributed significant nonlinearities to our measurements.
Intersynaptic cross talk
Finally, we provide a positive control for our assumption that the
postsynaptic responses to Schaffer collateral stimulation can be used
as linear estimators of transmitter release. The CTZ and KYN
experiments argue against receptor desensitization or saturation as
significant contributions to short-term plasticity, but do not
necessarily address other potential postsynaptic mechanisms. A more
direct test has been provided by Dobrunz and Stevens (1997)
, who showed
that the quantal sizes of responses to transmitter released from single
synapses do not depress during repetitive use, when stimulus strengths
are so weak that only one afferent synapse is activated at once. We
typically evoked release from tens of synapses simultaneously for our
experiments, however. Although there is no indication that transmitter
released at the same time from multiple synapses interacts with the
AMPA type of glutamate receptors in a nonlinear way at Schaffer
collateral synapses (Asztely et al., 1997
), cross talk between
calyceal-type synapses has been reported to result in postsynaptic
forms of short-term depression (Trussell et al., 1993
; Neher and
Sakaba, 2001
). Such a phenomenon, if operative at Schaffer collateral synapses, might have led to an overestimate of the actual amount of
presynaptic depression in our experiments.
An experiment designed to test this possibility instead verified that
the amount of depression in synaptic strength measured at multiple,
simultaneously active synapses was matched by decreases in the
probability of release at individual synapses. Short-term depression
and RRP refilling were measured with pairs of stimulus trains
(80 stimuli at 20 Hz) separated by 2 sec rest intervals as
diagrammed at the top of Figure
7B. Weak stimuli were
interleaved with those of normal strength during experimental trials.
The weak stimulus intensities may have evoked action potentials in several axons, all with afferent synapses with low release
probabilities, or in single afferent synapses. Experimental trials were
alternated with control trials during which only weak stimuli were used
throughout. Cross talk between synapses would be measurable as a change
in the sizes of the successful responses to weak stimulation caused by
transmitter release elicited by the normal intensity stimuli.

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Figure 7.
Individual synapses behave like
simultaneously activated populations. Schaffer collaterals were
stimulated with pairs of 4-sec-long spike trains (20 Hz) separated by 2 sec intervals. For half of the trials, only a minimal number of
afferents were stimulated throughout. For the other half, stimuli of
normal intensity were interleaved with the weak stimuli.
A, Typical, sequential raw data example of a failure, a
large response, and a minimal response during interleaved stimulation.
B, C, The average sizes
(B) and probability (C) of
successful transmissions in response to the minimal stimuli were
averaged into 200 msec bins and plotted versus the time of the
experiment. The squares represent the interleaved
minimal responses; the circles summarize experiments in
which only minimal stimuli were used throughout.
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|
Figure 7 shows that neither the size of the successful minimal
responses (Fig. 7B) nor the probability of release (Fig.
7C) was affected by the transmitter release elicited by the
large, interleaved stimuli. This result argues strongly against a
contribution of intersynaptic cross talk to short-term depression.
The average amplitude of the successful minimal responses during both
types of trials may have declined a small amount during the first
second of stimulation (Fig. 7B). The effect is attributable to the infrequent, simultaneous exocytosis of multiple vesicles, as
expected of a stochastic release process when the overall probability of release is as high as it was at the beginning of the weak stimuli trains (Zucker, 1973
).
During 20 Hz use, the probability of release at the synapses activated
by the weak stimuli depressed just as extensively as the synaptic
currents did in the other experiments reported here. The RRP
refreshment rate constant calculated by the method outlined in the
Appendix for the data plotted in Figure 7C is 0.23/sec. This value is indistinguishable from the rate constant calculated from the
synaptic currents elicited by stronger stimulations. The RRPs refilled
~45% during the first 2 sec of rest, yielding an extrapolated replenishment rate constant of 0.30/sec, a value that is not
significantly different from the rate constant calculated for the
synapses when active. These results provide assurance that the synaptic
currents measured for this study were linearly related to the amount of release at multiple, simultaneously active synapses, and they confirm
that it takes several seconds for neurotransmitter to replenish the
RRP, even when synapses are active.
 |
DISCUSSION |
Here we show that a slowly dissipating, residual calcium-driven
acceleration mechanism is sufficient to account for the full range of
activity-dependent modulation of the rate at which neurotransmitter is
prepared for exocytosis at Schaffer collateral synapses. Fresh quanta
of neurotransmitter were found to replace spent ones in the RRP at an
average rate of 0.24/sec when synapses were active. During subsequent
periods of rest, the RRP refilled with an ~5 sec exponential time
course, as expected if the replenishment process were to gradually
decelerate during inactive periods as demonstrated previously (Stevens
and Wesseling, 1998
). With no deceleration during rest intervals, the
0.24/sec rate constant would predict an only slightly faster
exponential refilling time course with a 4.2 sec time constant. This
leaves little kinetic room for a rapidly dissipating component of
replenishment-rate enhancement that might have been missed by the
earlier study and indicates that the rate at which the RRP is
replenished can be accelerated only modestly, even during periods
of heavy synaptic use.
A kinetically simple model (Eq. 1) of the rate-limiting mechanisms that
control how long it takes for neurotransmitter to be prepared for
release provides a good account of the dynamics of short-term
plasticity analyzed here. In particular, Figure 5 shows that when the
RRP is in a near-empty steady state, our working model predicts
quantitatively the time course over which the synaptic strength settles
to a new steady state after perturbations in the stimulus frequency, a
behavior that is a hallmark of first-order kinetic reactions.
Although the cell biological process of vesicular maturation is
complex, involving endocytosis, vesicle genesis and loading, physical
translocation and docking to the release sites, and biochemical priming
(Sudhof, 1995
), the observation that first-order kinetics describe well
the process by which vesicles are readied for exocytosis is consistent
with the possibility that only a single first-order enzymatic step in
the exocytic/endocytic cycle is rate limiting during the first several
seconds of heavy synaptic use. The identity of the molecular machinery
that limits how quickly vesicles are prepared for exocytosis remains
obscure, although it seems to be enzymatic in nature (Stevens and
Wesseling, 1998
, 1999b
; Pyott and Rosenmund, 2002
) and may be related
to biochemical priming that takes place during or after physical
docking to the active zone (Kawasaki et al., 1998
). During extended
periods of synaptic activity, a second rate-limiting process also plays
a role in a longer-lasting form of synaptic depression that may be
related to depletion of the reserve pool of vesicles or to some other rate-limiting element in the exocytic/endocytic cycle (Stevens and
Wesseling, 1999b
).
Does the readily releasable pool have kinetic subdivisions?
Our working model makes no qualitative kinetic distinctions among
readily releasable vesicles. The data presented here are also
consistent with models in which some of the release-ready vesicles are
available for immediate exocytosis, and the rest are used to restock
quickly this smaller pool when required, as long as the rate of
transfer between the two pools is fast on the time scale of these
experiments (Neher and Zucker, 1993
; Voets et al., 1999
; Voets, 2000
).
On the other hand, the phenomena modeled by these more complicated
schemes can often be explained equally well if the efficiency with
which action potentials trigger the fusion of individual release-ready
vesicles is a heterogeneous property of the release sites themselves
(Beutner et al., 2001
; Sakaba and Neher, 2001
). At present, we favor
models in which all of the release-ready vesicles are prevented from
undergoing exocytosis by a single type of energy barrier, because when
the release process is enhanced by residual calcium, the propensity for
exocytosis of the whole pool is potentiated in parallel (Stevens and
Wesseling, 1999a
).
Relation to earlier studies
On the basis of electrophysiological data alone, the RRP
refreshment rate that we have measured may pertain either to the time
it takes for reserve vesicles to be prepared for release or to some
other mechanism of neurotransmitter mobilization such as direct
refilling of the depleted readily releasable vesicles themselves.
However, Pyle et al. (2000)
recently measured the time it takes for
fluorescently labeled reserve vesicles to replace spent readily
releasable ones during periods of rest after episodes of high-frequency
synaptic use at similar synapses in culture. They report a single
exponential recovery time course with a 7 sec time constant, derived
from optical measurements, that is similar to the 5 sec time constant
for RRP refilling measured here, suggesting that the RRP is replenished
primarily with waiting reserve vesicles and not by some other means.
Several studies have reported that the transmitter mobilization process
is much faster when synapses are active than it is during subsequent
rest intervals (Kusano and Landau, 1975
; Pyle et al., 2000
). In the
earliest study to report such a phenomenon, Kusano and Landau (1975)
used a model in which action potentials always release the same
fraction of the RRP, and they concluded that the amount of short-term
depression observed during high-frequency use is incompatible with a
slow replenishment process at the squid giant synapse. It is now known,
however, that the efficiency with which action potentials trigger
release is not stationary at the mammalian central synapses that we
study (Stevens and Wesseling, 1999a
). Although squid synapses may
behave differently from Schaffer collateral synapses in this respect,
it is also possible that the short-term depression in synaptic strength
measured by Kusano and Landau (1975)
did not correspond to the true
extent of RRP depletion, much as a similar analysis would lead to an
underestimate of pool depletion for the synapses in our preparation.
Such an underestimate may have led to an overestimate of the amount of activity-dependent acceleration in the replenishment process at the
squid giant synapse.
Pyle et al. (2000)
reported a faster time course for RRP refilling when
measured electrophysiologically, from which they have concluded that
individual readily releasable vesicles can be reused rapidly several
times before being replaced at a slower rate by vesicles from the
reserve pool. The basis of our quantitatively differing
electrophysiological results is uncertain. One possibility is that the
stimulation protocol used by Pyle et al. (2000)
to elicit exocytosis in
the electrophysiological portion of their study did not completely
empty the available pool. This might have resulted in a recovery time
course that partially reflected short-term enhancement in that a larger
fraction of the available pool would have been released by trains
initiated after shorter rest intervals than by those initiated after
longer periods of rest [for a more extensive discussion of this issue,
see Stevens and Wesseling (1999a)
].
What is the role of the RRP?
The release-ready supply of synaptic vesicles supports the ability
of synapses to communicate information encoded by the spike-firing rate. The hippocampal synapses that we have studied start with a
typical release probability of ~30-40% (Hessler et al., 1993
; Rosenmund et al., 1993
; Allen and Stevens, 1994
; Huang and Stevens, 1997
). Although they fail to release transmitter in response to most
individual action potentials, they can still reliably transmit information by using short bursts of action potentials that are sure to
trigger some exocytosis when the RRP is at least partially full.
However, this option is no longer available to synapses that have
expended all of their release ready vesicles. After the RRP has been
exhausted, the probability of release becomes inversely proportional to
the stimulus frequency (Eccles and Rall, 1951
; Curtis and Eccles, 1960
;
Elmqvist and Quastel, 1965
; Abbott et al., 1997
). Because transmitter
release is stochastic and rare when synapses are depleted of their
release-ready vesicles, increasing the frequency of presynaptic
activity would have minimal impact on the overall signal detected by
postsynaptic neurons.
Because of the kinetic constraints imposed by a slow RRP replenishment
rate, information would likely be transmitted more efficiently via
these synapses by a neural code that relies on sporadic bursts of
activity than on one that uses precise modulations in the frequency of
continuous activity. Consistent with this, excitatory neurons in the
hippocampus and other brain regions do tend to fire such bursts of
spikes in awake and behaving mammals (Ranck, 1973
; Scott et al., 1986
;
Newsome et al., 1989
; Knierim and van Essen, 1992
; Meister and Berry,
1999
). This raises the following question: is the slow
replenishment rate an unavoidable biochemical limitation that hampers
the design of efficient neural circuits, or does the nervous system
derive some computational benefit from such constraints on synaptic operation?
 |
FOOTNOTES |
Received July 24, 2002; revised Sept. 6, 2002; accepted Sept. 9, 2002.
Funding was provided by National Institutes of Health Grants NS10827
(J.F.W.) and NS32742 (D.C.L.) and the McKnight Endowment Fund (D.C.L.).
We thank Dr. Dana Cohen, Dr. Isabel Pérez-Otaño, Dr. Iman
Brivanlou, and Dr. Richard Aldrich for providing helpful suggestions.
Correspondence should be addressed to John F. Wesseling, Duke
University Medical Center 3209, Duke University Department of Neurobiology, Durham, NC 27710. E-mail:
wesseling{at}neuro.duke.edu.
 |
APPENDIX |
Derivation of the RRP refreshment rate from Equation 1
According to Equation 1, when the RRP starts off empty, and there
is no exocytosis (i.e.,
= 0), the pool replenishes as a function of
time by:
These conditions are approximated during the brief intervals
between stimuli when the RRP is in a near-empty steady state, as it is
after the 60th action potential in a high-frequency train. While the
pool is maintained in a steady state, the amount of refilling between
stimuli must be equivalent to the amount of exocytosis,
r(
), elicited by each action potential. If
is the frequency of stimulation (20 Hz or 40 Hz for this study):
because 1/
is the time between stimuli. The solution for
depends on the pool capacity, N, which turns out to be an
unwieldy parameter. A more convenient parameter is the initial fusion
efficiency, fe, defined as the fraction