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The Journal of Neuroscience, November 1, 2001, 21(21):8362-8369
Paired-Pulse Plasticity at the Single Release Site Level: An
Experimental and Computational Study
Eric
Hanse and
Bengt
Gustafsson
Institute of Physiology and Pharmacology, Göteborg
University, SE-405 30 Göteborg, Sweden
 |
ABSTRACT |
CA3-CA1 glutamatergic synapses in the hippocampus exhibit a large
heterogeneity in release probability (p)
and paired-pulse (PP) plasticity, established already in the early
neonatal period when the CA3-CA1 connections consist of only a single
release site. At such a site two factors decide initial release
probability: the number of immediately releasable vesicles (preprimed
pool) and the vesicle release probability
(Pves1). Depletion and replenishment of this pool, an alteration in Pves,
and desensitization of postsynaptic receptors may contribute to PP
plasticity. A model based on data from single neonatal CA3-CA1
synapses has been used to address the relative importance of these
factors for the heterogeneity in PP plasticity. At a 20 msec PP
interval, the PP ratio
(P2/P1) varied from 0.1 to 4.5 among the synapses. At this interval
desensitization and replenishment were of little importance. The
heterogeneity was explained mostly by the variation in
Pves1, whereas the preprimed pool
size was of minor importance. Pves altered
from the first to the second stimulus such that
Pves2 was rather uniform among the synapses.
Its variation thus contributed little to the heterogeneity in PP ratio.
The model also shows that the relationship between alterations in
release probability and PP ratio is complex. Thus, an increase in
release probability can be associated with an increase, a decrease, or
no change at all in PP ratio, depending on the original values of
Pves1 and the preprimed pool and on which
one of these factors is altered to produce the increase in release probability.
Key words:
paired pulse; release probability; hippocampus; CA1; synaptic plasticity; development
 |
INTRODUCTION |
A ubiquitous feature of synapses is
that synaptic activity modifies synaptic action. In its simplest form
this plasticity can be seen as paired-pulse (PP) facilitation
(PPF)/paired-pulse depression (PPD), in which the second
afferent stimulation produces more/less synaptic action than the first
one (Katz and Miledi, 1968
; Zucker, 1989
; Thomson, 2000
). Mechanisms,
both on the presynaptic and postsynaptic side, may contribute to
paired-pulse plasticity. These include changes in the number of
release-ready vesicles, in the release probability of the individual
vesicles, and in the responsiveness of the postsynaptic receptors.
Paired-pulse plasticity is of functional interest because it decides
the short-term computational properties of the synapse. Moreover, it is
also used as a tool for evaluation of possible presynaptic changes after other kind of manipulations of the synapse. For example, manipulations thought to influence presynaptic release are generally assumed to alter paired-pulse plasticity in a predictable manner.
To properly understand what underlies variations in paired-pulse
plasticity among synapses, as well as to use it as a tool, one would
have to know what factors determine release probability and how these
factors may be altered after a first stimulus. For the Schaffer
collateral synapses on CA1 pyramidal cells, release probability
to the first (initial) stimulus and paired-pulse plasticity vary
considerably among the synapses in a correlated manner (Dobrunz and
Stevens, 1997
). It has been suggested that the initial release probability is primarily decided by the number of readily releasable vesicles (Dobrunz and Stevens, 1997
), but how this latter factor could
give rise to the correlated variation in paired-pulse behavior is
unclear. Recently, examination of release from these synapses in the
neonatal rat has indicated that initial release probability also
depends to a considerable extent on a variation in vesicle release
probability (Pves) (Hanse and
Gustafsson, 2001a
,b
). Moreover, the release-ready pool was found to be
very small (on average only one vesicle) and variable among the
synapses. Such information would then allow for an evaluation of the
manner in which vesicle release probability and the size of the
release-ready pool could create a variation in the paired-pulse
behavior among these synapses.
In the present article, we have modeled the paired-pulse behavior of
single release sites exhibiting the above features. The aim has not
been to give a full account of all aspects of paired-pulse behavior.
Rather, by explaining a specific instance of paired-pulse behavior our
aim is that some general insights into how paired-pulse plasticity is
molded and how it can be used as a tool may emerge.
 |
MATERIALS AND METHODS |
Hippocampal slice preparation. The experimental data
used in the present study were obtained as described in detail
previously (Hanse and Gustafsson, 2001a
,b
). Hippocampal slices were
prepared from 1- to 7-d-old Wistar rats. The rats were killed by
decapitation in accordance with the guidelines of the local ethical
committee for animal research. Whole-cell patch-clamp recordings were
performed from visually identified CA1 pyramidal cells using a pipette
solution containing (in mM): 95 Cs-gluconate, 20 TEA-Cl, 10 NaCl, 5 QX-314, 4 Mg-ATP, 0.4 Na-GTP, 0.2 EGTA, and 10 HEPES, pH 7.3, adjusted with CsOH. Recordings were performed at
30-32°C and the extracellular solution contained (in
mM): 124 NaCl, 3.0 KCl, 4 CaCl2, 4 MgCl2, 1.25 NaH2PO4, 26 NaHCO3, 10 glucose, and 0.02 bicuculline
methiodide or 0.1 picrotoxin.
Afferents in the stratum radiatum were activated with 10 impulse, 50 Hz
trains at 0.2 Hz using minimal extracellular stimulation. Several
findings suggested that this minimal stimulation consistently resulted
in the activation of a single axon contributing a single synapse to the
cell recorded from this synapse containing a single release site (Hanse
and Gustafsson, 2001a
). They also suggested that this release site
releases one vesicle per stimulus at most (Triller and Korn, 1982
;
Stevens and Wang, 1995
; Dobrunz and Stevens, 1997
; Liu et al., 1999
;
Matveev and Wang, 2000
). Most importantly, the average EPSC
amplitude, excluding failures, was found to be independent of release
probability during the burst (Hanse and Gustafsson, 2001a
). This result
strongly argues against a release of more than one vesicle per action
potential, because that would have resulted in larger EPSC amplitudes
at positions of higher release probability during the burst.
Determination of vesicle release probability and size/variation
of preprimed pool. The release probability
(p) of a single release site is thought to be
determined by the number of release-ready, or primed, vesicles
(npool) and by the
Pves, such that
|
(1)
|
Pves varies among the release
sites but is considered to be the same within a release site (Hanse and
Gustafsson, 2001b
). We refer to the pool of vesicles primed at the
arrival of the first stimulus of the 10 impulse train as the preprimed
pool. The analysis to determine Pves1
(Pves at the first stimulus position of the train) and the size of the preprimed pool for individual synapses have been described previously (Hanse and Gustafsson, 2001b
).
Briefly, all of the 10 impulse trials, ~100 per synapse, were also
considered as 9 impulse trials (disregarding the last response), and so
on, down to 2 impulse trials. Then, for each of these
n-impulse trials, two groups of trials were selected. One
group contained trials in which only a single release event occurred
during the n stimuli. The other one contained trials in
which two release events occurred during the n stimuli, with the condition that one of the events occurred at the last
(nth) stimulus position for the given length. For each trial
length the probability that a release event occurred at the first
stimulus position was then compared between the one release and two
release event groups. When the release probabilities in the first
stimulus position in the train were the same for the two groups, the
release event at the nth position in the train could not
have originated from a vesicle that was primed at the onset of train
stimulation. However, when the release probability was higher for the
two release event group, this second vesicle must have belonged to the
preprimed pool. This analysis then defined, for each synapse, the
stimulus position at which release no longer originates from preprimed vesicles but rather originates from vesicles recruited to a primed state during the train (refilling point). The average preprimed pool for each synapse was then estimated as the cumulative release occurring before the refilling point was reached.
This analysis also allows for an estimation of
Pves1, because the trials in which the
preprimed pool consisted of only one vesicle are the trials in which
only one release event occurred before the refilling point. Thus,
Pves1 was determined as the release
probability in the first stimulus position for those single release
trials. This method for determining
Pves1 is thus based on a subset of the
trials (~100) to which each synapse was subjected. To estimate the
sampling error in the estimation of
Pves1 we performed a Monte Carlo
simulation of release from a preprimed pool according to Equation 1 and
a binomial distribution of the pool size (see Fig.
2B). These simulations, each with 100 trials, gave an
estimated Pves1 that on average was
equal to the predefined one with a SD of ~0.06. This can be compared
with the SD of 0.28 for the variation between synapses (Hanse and
Gustafsson, 2001b
). Because there was an intersimulation variation in
the release probability at position 1 (P1) (SD = 0.04) that correlated
with that of the estimated Pves1
(r
0.7), the error with respect to the calculated
P1 (for a given simulation or
experiment) will thus only be approximately one-half the above
estimated error in Pves1. The
Pves value at the second stimulus
position (Pves2) was calculated as
follows:
|
(2)
|
where P2 is the release
probability at position 2 (using all trials) and
npool is the average size of the
preprimed pool.
If release events occurring up to the refilling point were considered,
any given synapse displayed a substantial trial-to-trial variation in
the number of such events. This variation was used to estimate the size
distribution of the preprimed pool across all trials (see Fig. 2).
Although a fixed refilling point provides for an accurate estimation of
the average preprimed pool (Hanse and Gustafsson, 2001b
), it may
introduce some bias in the estimation of the size distribution. First,
a vesicle that is recruited during the train may be released before the
refilling point and, if so, bias the distribution toward larger pool
contents. Second, if there are more than two preprimed vesicles (the
refilling point analysis is based on a preprimed pool of two vesicles),
a preprimed vesicle may be released after that position and, if so,
bias the distribution toward smaller pool contents. These putative
biasing effects are partially opposing each other and their influence should be small as long as the preprimed pool is small. A small (0.5-2
vesicles) average preprimed pool was also found among these synapses
(Hanse and Gustafsson, 2001b
). Nevertheless, because of these
considerations, the distributions of the trial-to-trial variation of
the preprimed vesicle pool should be considered provisional.
Model computations. Based on the range of the experimentally
estimated values of Pves1 and
Pves2 and the size and variation of
the preprimed pool, release probabilities in response to a first
(P1) and a second
(P2) stimulus were calculated using
Equation 1. Pves1 was varied between
0.1 and 1.0 and the (average) preprimed pool was varied between 0.6 and
1.8. Pves2 was set to a fixed value of
0.35. The trial-to-trial variation in the preprimed pool size was
simulated by a binomial distribution. The paired-pulse ratio was
calculated as
P2/P1.
The analysis and the calculations were performed using custom software
written in Igor Pro (Wavemetrics, Lake Oswego, OR).
Unless otherwise indicated, data are presented as mean ± SEM.
Student's t test was used to determine statistical significance.
 |
RESULTS |
Figure 1A
illustrates unitary quantal release from a single terminal of a
Schaffer collateral axon onto a CA1 pyramidal cell in response to train
activation (20 msec interval). Such activation of synapses in 1- to
7-d-old rats resulted in release that varied considerably among the
synapses with respect to initial release probability
(P1), and facilitation/depression
behavior (Hanse and Gustafsson, 2001b
). The
P1 values varied from almost 0 up to
almost 1.0, whereas release probability to the second stimulus (P2) had a somewhat more narrow
distribution, mostly between 0.1 and 0.4 (Fig. 1B).
No correlation was observed between the
P1 and the
P2 values (Fig. 1B).
The paired-pulse ratio
(P2/P1)
varied widely among the synapses, with most synapses demonstrating
PPD (Fig. 1C). Synapses with low
P1 produced PPF, and the larger
the P1 the more the PPD. However, the
scatter was considerable, indicating a rather poor predictive ability
of P1 with respect to paired-pulse plasticity. The
P2/P1
ratio did not correlate with the age of the animal during the first
postnatal week (r = 0.03; p > 0.05).

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Figure 1.
Release probabilities and paired-pulse (20 msec)
ratio among synapses. A, Ten consecutive sweeps (0.2 Hz)
from one synapse in response to paired stimuli. EPSCs are indicated by
asterisks. B, Relationship between
P1 and P2 among
synapses (n = 42). The solid line is
a linear regression line (r = 0.14;
p > 0.05), and the dashed line
indicates equality between P1 and
P2. Nine synapses with no
first-release probability (low-frequency mute synapses) are not
included in the graph. C, Relationship between the
paired-pulse ratio
(P2/P1)
and P1 among the synapses
(n = 42). The dashed line indicates
equality between P1 and
P2. D, Relationship between
paired-pulse ratios measured using release probabilities and EPSC
areas. The solid line is a linear regression line
(r = 0.96; p < 0.001).
|
|
Paired-pulse plasticity was also evaluated as
EPSC2/EPSC1, where
EPSC1 and EPSC2 are the
average EPSC magnitudes (including failures). Discrepancies between
this ratio and that of
P2/P1 would indicate the influence of changes in quantal size on paired-pulse plasticity. On average, both the magnitude and probability ratio were
0.84 ± 0.12 (n = 43), and the two ratios
correlated well (slope = 0.98) throughout the range of
paired-pulse plasticity (Fig. 1D). That is,
postsynaptic factors such as desensitization do not participate in
paired-pulse plasticity under these conditions.
To analyze what may explain the above paired-pulse behavior,
P1 and
P2 were calculated using Equation 1 as
described in Materials and Methods.
Binomial trial-to-trial distribution of preprimed vesicles
As described in Materials and Methods, the size of the preprimed
pool at a given release site varies from trial to trial. To account in
the model for this variation, the nature of this variation was
examined. For each synapse the number of preprimed vesicles at each
stimulus trial was determined (see Materials and Methods), and a
distribution of these values was obtained. Synapses were then
subdivided arbitrarily into four groups with respect to their average
pool size, and the distributions within each of these groups were
pooled together (Fig. 2, left
column). In the group with the lowest average size of preprimed
pool (Fig. 2, left, uppermost graph), the
pool was zero in more than one-half of the trials, and trials with two
preprimed vesicles were rare. However, in the group with the largest
average pool (Fig. 2, left, lowermost
graph) preprimed vesicles were absent in <10% of the trials, and
up to four preprimed vesicles could occur.

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Figure 2.
Distribution of the trial-to-trial variation in
the preprimed pool size. The left column shows the
trial-to-trial variability in the number of preprimed vesicles. Results
from different synapses were pooled together in four groups according
to the average size of their preprimed pool. The average pool size
within each group is indicated in the graphs together with the number
of synapses included. The right column shows binomial
distributions using two, three, four, and five sites, respectively;
each site had an occupancy probability of 0.3.
|
|
The fact that on some trials preprimed vesicles were absent suggests
that priming is reversible. Otherwise, it seems difficult to understand
why during some of the 5 sec intertrial intervals two to three vesicles
have entered a primed state whereas during many other such intervals no
vesicle has entered such a state. It may then be conceived that docked
vesicles are in equilibrium between a primed and a nonprimed state. The
simplest model is to assume that each synapse has a number of
docking/priming sites equal to the largest number of preprimed vesicles
observed for that synapse. We thus computed the binomial distribution
of site occupancy by varying the number of sites from two to five and keeping the probability of site occupancy (at each site) constant. The
right column of Figure 2 shows that for matching average
preprimed pool sizes, a p value of 0.3 gave distributions
closely resembling the experimental ones.
Such a value can then used to model the trial-to-trial variability of
the preprimed pool.
Computed paired-pulse ratio: Pves1 and
preprimed pool
The experimentally determined values of
Pves for the first stimulus
(Pves1) vary among the synapses from
close to 0 up to almost 1 (Fig. 3) (Hanse
and Gustafsson, 2001b
). For the calculations, Pves1 was thus allowed to vary from
0.1 to 1.0 in steps of 0.1. Experimentally,
Pves for the second stimulus
(Pves2) was found to vary mostly
between 0.2 and 0.5, independently of
Pves1 (Fig. 3). In the model we
therefore chose to use a fixed value of 0.35 for
Pves2. The average size of the
preprimed pool was varied between 0.6 and 1.8 in steps of 0.3, with
each average size represented by a binomial distribution of
npool sizes (compare Fig. 2,
right column). The calculated values of
P1 and
P2 are plotted against each other in
Figure 4A. In agreement
with the experimental values (Fig. 1B), the modeled
P1 values vary from close to 0 up to
0.9, and the P2 values are more
narrowly distributed, mostly within 0.1-0.4. It can be noted that when
P1 increases because of an increase in Pves1 (for a given pool
size) P2 decreases, but this decrease
is relatively less the larger the pool size. However, when
P1 increases because of an increase in
pool size (for a given Pves1) then
P2 increases, relatively more the
larger the Pves1. These two
contrasting effects indicate an overall lack of a relationship between
P1 and
P2, as also observed experimentally
(Fig. 1B).

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Figure 3.
Experimentally obtained relationship between
Pves2 and Pves1
among the synapses (n = 42). The dashed
line is the regression line for these data
(r = 0.09; p > 0.05).
Pves2 was calculated using Equation 2, where
P2 is the release probability at stimulus
position 2, npool is the average size of the
preprimed pool, and P1 is the release
probability at stimulus position 1.
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Figure 4.
Calculated relationships between
P1,
P2, and the PP ratio at different
magnitudes of Pves1 and the preprimed pool.
The release probabilities in response to the first
(P1) and second
(P2) stimulus were calculated using
Equation 1 as described in Materials and Methods.
Pves1 was varied between 0.1 and 1 in steps
of 0.1. The average preprimed pool was varied between 0.6 and 1.8 vesicles in steps of 0.3. Pves2 was set to a
fixed value of 0.35. A, Relationship between
P1 and P2. The
dashed line indicates equality between
P1 and P2.
B, Relationship between the paired-pulse ratio
(P2/P1)
and P1. The dashed line
indicates a PP ratio of 1. C, Same as in
B, but each PP-Pves1 curve
is normalized with respect to the paired-pulse ratio value obtained at
a pool of 1.2.
|
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Figure 4A shows that most calculated values fall
below the "P1 = P2 line" (dashed line),
indicating a predominance of PPD over PPF. When the
P2/P1
ratio is plotted against P1 (Fig.
4B), there is an overall but broad relationship
between the paired-pulse ratio and P1,
in agreement with the experimentally observed relationship (Fig.
1C). The broadness is again related to the contrasting
actions of Pves and preprimed pool
variations, respectively. When P1
increases because of an increase in
Pves1, the paired-pulse ratio
decreases, in line with the common notion that an increase in release
probability should be associated with a substantial decrease in
paired-pulse ratio. However, the horizontal nature of the lines drawn
through the iso-Pves values in Figure
4B shows that when
P1 increases because of an increase in
the pool size, the paired-pulse ratio changes little or, for large
Pves1 values, actually increases. To
better illustrate the relative change in the paired-pulse ratio introduced by preprimed pool variations, the same values have been
replotted in Figure 4C after normalization to the PP ratio calculated for the median (average) preprimed pool (1.2). It can be
noted that for Pves1 values of >0.5,
an increase in the preprimed pool causes an increase in
P1 associated with a substantial
relative increase in the paired-pulse ratio.
Nevertheless, the above calculations suggest that the variation in
paired-pulse ratio is dominated by the variation in
Pves1. This effect of
Pves1 depends on two factors. The
first factor is that a change in Pves1
alters the
Pves2/Pves1
ratio, thereby changing the
P2/P1
ratio. The second factor is that a larger
Pves1 will lead to a larger depletion
after the first stimulus. In Figure 5A, the calculated values of
P2/P1
(solid lines) are plotted against the
Pves1 value for the five different
pool sizes. It can be noted that when
Pves1 is small (0.1-0.2), there is a
large PPF of 100-200%. When Pves1 is
large (>0.7) there is a large PPD, with the second response being only
some 10-30% of the first one. To separate the above two effects of
Pves1, the depletion factor was
annulled by using the same pool size for the calculation of
P2 as for
P1. These
P2/P1
ratios are shown in the same graph (Fig. 5A, dashed lines). Comparison between the two sets of
P2/P1
calculations indicates that most of the variation in paired-pulse ratio
depends on changes in the
Pves2/Pves1
ratio. That is, depletion does not cause large changes in the absolute
values of the paired-pulse ratio. Nevertheless, depletion appears to
cause considerable changes in the normalized paired-pulse ratio, in
particular for larger values of Pves1.
To illustrate that effect more directly, the calculated values (Fig.
5A, solid lines) were, for each size of (average)
preprimed pool, normalized with respect to those calculated using the
same pool size for P2 as for
P1 (Fig. 5A, dashed
lines). This procedure demonstrates (Fig. 5B) that
depletion causes a decrease in the normalized paired-pulse ratio that
depends strongly on the value of Pves1
as well as on the preprimed pool size.

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Figure 5.
Paired-pulse ratio
(P2/P1)
against Pves1: effects of
Pves2 variations and of depletion. These
calculations were performed as described in the legend to Figure
4. A, Relationship between
Pves1 and the paired-pulse ratio.
Solid lines represent the relationship for five
different pool sizes (0.6, 0.9, 1.2, 1.5, and 1.8, respectively). The
dashed line represents calculations using the same five
pool sizes, but in this case the pool size was the same for the first
and second stimulus (i.e., there was no depletion of vesicles).
B, Relative effect of vesicle depletion for paired-pulse
ratio for different pool sizes (0.6-1.8) and for different
Pves1 values. The plot is derived from
A such that for each pool size, the ratio between the
curves with (solid line in A) and without
(dashed line in A) depletion was
constructed. C, Effect of different
Pves2 values on the relationship between the
paired-pulse ratio and first-release probability. The white
area, corresponding to a Pves2 value
of 0.35, is the same as the plot shown in Figure
4B. The gray and
black areas correspond to
Pves2 values of 0.25 and 0.45, respectively.
These Pves2 values correspond approximately
to the mean ± SD of the experimentally obtained
Pves2 (0.33 ± 0.11).
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|
Computed paired-pulse ratio: Pves2
Figure 3 shows that the experimentally estimated values of
Pves2 varied from ~0.2-0.5
independently of Pves1. The variation in Pves2 will then not be expected to
affect the paired-pulse ratio in a manner that is correlated with
initial release probability but rather to introduce scatter in the
PPF/PPD-P1 relationship. The
influence of Pves1 (and of preprimed
pool) variations on paired-pulse ratio was thus examined using a fixed
Pves2 value of 0.35. However, to
indicate the effect of Pves2 on the
paired-pulse ratio, the calculations of
P2 and
P1 illustrated in Figure
4B were also performed using
Pves2 values of 0.25 and 0.45. Figure
5C shows that this variation of
Pves2 introduces some shift of the
relationship between paired-pulse ratio and initial release probability
without altering its overall shape.
Paired-pulse ratio versus Pves1 and
preprimed pool size
Heterogeneity in P1 among the
synapses is explained about equally by variations in
Pves1 and in preprimed pool size
(Hanse and Gustafsson, 2001b
). The above calculations suggest that it is mostly P1 differences attributed to
variation in Pves1 that should cause
differences in the paired-pulse ratio. Figure
6 shows the experimentally observed
paired-pulse ratios plotted against Pves1 (Fig. 6A) and
the preprimed pool size (Fig. 6B) estimated for these
synapses. As can be noted from the individual values (Fig. 6,
filled circles) as well as from the binned averages (Fig. 6A, filled squares) and the regression
line (Fig. 6B, dashed line), these
paired-pulse ratio values covaried with
Pves1 and not with pool size.
Calculated relationships are also included in these graphs (as
solid lines).

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Figure 6.
Pves1, but not
the preprimed pool, determines the paired-pulse ratio.
A, Relationship between
P2/P1 and
Pves1. Filled circles are
experimental data obtained from 42 synapses. Filled
squares represent binned averages (bin size is 0.2 Pves units) of the experimental data. Error
bars are ±SEM and are only seen outside the
symbol for the lowest Pves1
value. Lines are connecting calculated values using the
parameter values given in the legend to Figure 4.
B, Relationship between
P2/P1 and
the preprimed pool. Filled circles are experimental data
obtained from 42 synapses. The dashed line is the
regression line for these data (r = 0.14;
p > 0.05). Solid lines are
connecting calculated values using the parameter values given in
the legend to Figure 4.
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 |
DISCUSSION |
The present experimental results and calculations suggest that
heterogeneity in paired-pulse plasticity among the Schaffer collateral
synapses in the neonatal rat is primarily explained by a variation in
Pves1. Variations in
Pves2 and in the size of the
release-ready vesicle pool were found to be of secondary importance, and desensitization was of no importance. The present model also suggests that an increase in initial release probability is not necessarily associated with a decrease in paired-pulse ratio but can
also be associated with no significant alteration or even with a
substantial increase.
Paired-pulse plasticity: Pves changes,
pool changes, and desensitization
Paired-pulse plasticity is commonly seen as resulting from the
interaction of three factors: two presynaptic ones and a postsynaptic one. Facilitation results from an increase in
Pves, based for example on
"residual" calcium from the first stimulus. Depression can result
from a decrease in Pves, a decrease in
vesicle pool size (depletion), and desensitization of postsynaptic
receptors. In the present calculations, desensitization was not taken
into account because, at least with the paired-pulse intervals used (20 msec), paired-pulse plasticity was found experimentally to be the same
regardless of whether it was evaluated by EPSC magnitude or by release
probability. That is, postsynaptic factors such as desensitization do
not play any role (Hjelmstad et al., 1999
).
The importance of vesicle depletion was evaluated using model
calculations. Depletion was found to have an effect on paired-pulse plasticity that was strongly dependent on
Pves1 and on the preprimed pool. For
lower Pves1 values, depletion gave
~20% lower values of paired-pulse plasticity that were independent
of preprimed pool size. For large
Pves1 values, corresponding values
were 40-80%, with the effect being more accentuated for the smaller
preprimed pool sizes. Vesicle depletion can thus be a significant
factor in the generation of PPD under certain conditions. These
calculations did not take into account possible recruitment of newly
primed vesicles. Approximately one-sixth of the hippocampal neonatal synapses lack initial release but display a low release probability (0-0.1) to the second stimulus ("low-frequency mute" synapses) (Hanse and Gustafsson, 2001b
). This behavior was explained by a lack of
a preprimed pool and by a fast onset of recruitment. We have no
evidence that such a fast recruitment occurs in synapses exhibiting a
preprimed pool. However, if so, such recruitment should act to diminish
the depletion effect.
Our model calculations suggest that the variation in
Pves1 among the synapses creates the
large heterogeneity in paired-pulse plasticity. This effect of
Pves1 depends on two factors. The
first is that a change in Pves1 alters
the
Pves2/Pves1
ratio, thereby changing the
P2/P1
ratio. The second is that a larger
Pves1 will lead to a larger depletion
effect. A key model factor is that Pves2 is kept constant at an
intermediate value (0.35). At synapses with higher/lower
Pves1 values,
Pves is thus supposed to
decrease/increase during the paired activation and lead to PPD/PPF (see
also Matveev and Wang, 2000
). A decrease in
Pves with paired activation does not
conform to the residual calcium hypothesis. However, such a reduction
in Pves has been described in other
synapses (Bellingham and Walmsley, 1999
; Thomson and Bannister, 1999
;
Wu and Borst, 1999
; Waldeck et al., 2000
). Thus, in agreement with
these other recent studies (Bellingham and Walmsley, 1999
; Thomson and
Bannister, 1999
; Wu and Borst, 1999
; Matveev and Wang, 2000
; Waldeck et
al., 2000
), our results suggest that depression is not explained solely by vesicle depletion. In the presently analyzed synapses,
Pves2 was not found to be constant,
but its variation was considerably less than that of
Pves1, and was independent of
Pves1. The model calculations
indicated that this Pves2 variation
created some broadening of the relationship between paired-pulse ratio
and P1.
Temporal aspects of paired-pulse plasticity
Experimental data have been limited to a single paired-pulse
interval (20 msec). This is an interval at which the initial release-dependent release inhibition should have vanished (Stevens and
Wang, 1995
; Dobrunz et al., 1997
; Hjelmstad et al., 1997
) and at which
possible recruitment of newly primed vesicles is likely kept at a
minimum. An understanding of paired-pulse plasticity along the time
axis would then in addition require knowledge of the
Pves2 dynamics, both from a value
higher than Pves1 as from a lower one,
as well as of vesicle recruitment dynamics.
Dissociation between initial release probability and
paired-pulse plasticity
It is commonly assumed that an increase in initial release
probability is associated with a decrease in paired-pulse ratio. However, the calculations show that when
P1 increases because of an increase in
preprimed pool size there is either little change, or, for larger
values of Pves1, a substantial
increase in the paired-pulse ratio. Because of the small size of the
preprimed pool, its average size had a large effect on release
probability. For example, a doubling of pool size could cause an
~50% increase in P1 associated with
anything from no change to a 100% increase in paired-pulse ratio. In
the model, a pool-size change can be achieved by an increase either in
the probability for a docked vesicle to be in a primed state or in the
number of docking/priming sites. The observation of a phorbol
ester-induced change in release probability unaccompanied by changes in
paired-pulse ratio (Honda et al., 2000
) may then be explained in this
manner. Conversely, the finding of a change in paired-pulse ratio
unaccompanied by any change in release probability after BDNF treatment
(Sherwood and Lo, 1999
) in NT-3-deficient mice (Kokaia et al., 1998
)
and in Rab3A-deficient mice (Geppert et al., 1997
) can be explained either by a selective change in Pves2
or by a reciprocal change in Pves1 and
the size of the preprimed pool.
Preprimed pool distribution
The experimental analysis suggested that the preprimed pool of
vesicles fluctuated in size from trial to trial. A binomial model for
this fluctuation was constructed for usage in the paired-pulse calculations. This binomial model was based on the assumption that the
final release-ready stage is reversible, with docked vesicles being in
equilibrium between a nonprimed and a primed state. Such reversibility
in the final release-ready stage appears compatible with current
molecular models of the release process (Murthy and Stevens, 1999
;
Matveev and Wang, 2000
; Voets, 2000
; Zenisek et al., 2000
). To vary the
average preprimed pool in the model, the number of docking sites was
varied (two to five) and the probability of a vesicle to be in the
primed state was kept constant at 0.3. Experimentally estimated
distributions of preprimed pool fluctuations from synapses with
different average preprimed pool sizes were quite similar to the
simulated ones, which lends support to this kind of binomial model.
Moreover, the number of docking/priming sites used (two to five) is in
good agreement with the number of such sites contained within a region
destined to be a release site (Zhai et al., 2001
). However, the
experimental data would also be compatible with other parameters of
such a model. Nevertheless, this binomial description may be helpful for calculations of release probabilities and may serve as an analytical tool for the evaluation of release under experimental circumstances.
Dependence on age
The experimentally observed paired-pulse ratio did not correlate
with the age of the animal (within the first postnatal week), indicating that its variability among the synapses was not a
developmental feature. The presently found relationship between
paired-pulse ratio and initial release probability also agrees in its
overall variability and shape with that obtained from putative single release sites of the same hippocampal connections from older animals (Dobrunz and Stevens, 1997
). However, the present relationship is
substantially shifted toward more PPD/less PPF compared with that
previous study. This shift may be related to differences in
experimental conditions that may affect release conditions, such as
temperature and divalent ion concentrations. However, examination of
paired-pulse plasticity using population EPSP recordings has indicated
that under the same experimental conditions, a substantial shift occurs
in a facilitating direction at approximately days 8-12 (P. Wasling, E. Hanse, B. Gustafsson., unpublished observations). Although not
excluding other possibilities, these data point to age difference as a
major explanation. It will be of interest to find out in future studies
which of the factors that decides paired-pulse plasticity undergoes
such developmental change that explains such a shift in paired-pulse ratio.
Paired-pulse plasticity within a synapse
Can the present calculations also explain what happens to the
paired-pulse ratio when Pves1 and the
preprimed pool change within a given synapse? With respect to changes
in pool size, there seems no reason to believe otherwise. However, with
respect to Pves1, the situation is
more complicated. Recent studies, albeit in neocortical axons (Koester
and Sakmann, 2000
) and hippocampal cultures (Prakriya and Mennerick,
2000
), have indicated, directly or indirectly, a wide variation in
action potential-induced calcium influx among synaptic boutons. The
variations in Pves1 among synapses may
then be explained by a variation in calcium influx. Because manipulation of release probability often concerns a modulation of the
amount of presynaptic calcium influx, one may also conjecture that in
this situation Pves1 may vary whereas
Pves2 does not change much at
all. However, there is at present no experimental support for
such a notion. Moreover, Pves may be
altered in a manner unrelated to calcium influx. Thus, to increase the
usefulness of the present specific model to understand induced
paired-pulse plasticity variations, an extension to incorporate changes
in Pves2 may be needed.
 |
FOOTNOTES |
Received April 6, 2001; revised Aug. 10, 2001; accepted Aug. 21, 2001.
This study was supported by grants from the Swedish Medical Research
Council (project numbers 12600 and 05180), the Swedish Society of
Medicine, and Harald Jeanson's Foundation. We thank F. Asztely, J. Eilers, L. Groc, and P. Wasling for critically reading this manuscript.
Correspondence should be addressed to Eric Hanse, Institute of
Physiology and Pharmacology, Göteborg University, Box 432, SE-405
30 Göteborg, Sweden. E-mail: eric.hanse{at}physiol.gu.se.
 |
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