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The Journal of Neuroscience, March 15, 2000, 20(6):2073-2085
Heterogeneous Conductance Levels of Native AMPA Receptors
T. Caitlin
Smith1,
Lu-Yang
Wang2, and
James R.
Howe1, 2
1 Interdepartmental Neuroscience Program and
2 Department of Pharmacology, Yale University School of
Medicine, New Haven, Connecticut 06520-8066
 |
ABSTRACT |
The single-channel properties of AMPA receptors can affect
information processing in neurons by influencing the amplitude and
kinetics of synaptic currents, yet little is known about the unitary
properties of native AMPA receptors in situ. Using
whole-cell and outside-out patch-clamp recordings from granule cells in
acute cerebellar slices, we found that migrating granule cells begin to
express AMPA receptors before they arrive in the internal granule cell
layer and receive synaptic input. At saturating agonist concentrations, the open probability of channels in outside-out patches from migrating cells was very high, allowing us to identify patches that contained only one or two active channels. Analysis of the single-channel activity in these patches showed that individual AMPA receptors exhibit
as many as four distinguishable conductance levels. The conductance
levels observed varied substantially for different channels, although
on average the values fell within the range of unitary conductances
estimated previously for synaptic AMPA receptors. In contrast to
patches from migrating granule cells, we rarely observed directly
resolvable single-channel currents in patches excised from the somata
of granule cells in the internal granular layer, even though these
cells gave large AMPA receptor whole-cell currents. We did, however,
detect AMPA receptors with apparent unitary conductances of <1 pS in
patches from both migrating and mature granule cells. Our results
suggest that granule cells express a heterogeneous population of AMPA
receptors, a subset of which are segregated to postsynaptic sites after synaptogenesis.
Key words:
granule cell; cerebellum; AMPA receptor; glutamate; single channel; synaptic; extrasynaptic; development
 |
INTRODUCTION |
Although AMPA receptors mediate
EPSCs in most CNS neurons, the single-channel properties
of these receptors have not been directly studied in neurons in
situ. AMPA receptors are multimeric assemblies of the glutamate
receptor (GluR) subunits GluR1-4, and their subunit composition and
stoichiometry, as well as RNA editing and alternative splicing,
influence several important channel properties (Hollmann and Heinemann,
1994
; Bettler and Mulle, 1995
; Dingledine et al., 1999
). Because of the
extensive array of potential AMPA receptor assemblies and
neuron-to-neuron differences in subunit expression, it is not
surprising that previous studies have found considerable variability in
AMPA receptor phenotype (McBain and Dingledine, 1993
; Yamada and Tang,
1993
; Geiger et al., 1995
; Fleck et al., 1996
; Tóth and
McBain, 1998
).
Studies of recombinant AMPA receptors have shown that homomeric, as
well as heteromeric, channels display multiple conductance levels whose
amplitudes depend on subunit composition (Swanson et al., 1997
;
Rosenmund et al., 1998
; Derkach et al., 1999
). Multiple open levels in
AMPA receptors were first observed in studies of cultured CNS neurons
(Cull-Candy and Usowicz, 1987
; Jahr and Stevens, 1987
; Ascher and
Nowak, 1988
; Cull-Candy et al., 1988
). However, previous single-channel
studies of native AMPA receptors in cultured neurons have been
performed at low agonist concentrations, and the consequently low open
probability (popen) of the
channels made the number of channels contributing to the record
indeterminate. Therefore, it was uncertain to what extent the different
open levels reflected conductance substates or the presence of
different channel types.
Localization of synaptic AMPA receptors in situ at
postsynaptic densities presents further barriers to studying channel
properties directly. Thus information about the conductance of synaptic
channels is limited to estimates obtained from nonstationary
fluctuation analysis of synaptic currents. Recently, investigations of
recombinant AMPA receptors demonstrated that the prevalence of sojourns
in conductance substates varies with agonist concentration (Rosenmund et al., 1998
). If native AMPA receptors show similar
concentration-dependent behavior, this would further complicate
comparisons of synaptic data with single-channel results obtained at
low agonist concentrations in vitro, because the transient
rise in glutamate concentration after transmitter release peaks at
saturating levels (Clements et al., 1992
; Clements, 1996
; Diamond and
Jahr, 1997
).
In the present study, we have recorded currents through single AMPA
receptors at saturating agonist concentrations, under conditions at
which the high popen of the channels
enabled us to identify patches containing at most two active channels.
We have taken advantage of the postnatal development of the cerebellum to record AMPA receptor currents at two developmental stages: (1)
during migration through the molecular layer (ML) before the neurons
receive synaptic input and (2) after synaptogenesis in the internal
granular layer (IGL). We found that AMPA receptors expressed by
migrating cerebellar granule cells exhibit as many as four conductance
levels, which showed extensive heterogeneity from channel to channel.
On average, larger-conductance channels in outside-out patches had
conductances similar to those estimated for synaptic AMPA receptors at
the mossy fiber-granule cell synapse (Traynelis et al., 1993
; Silver
et al., 1996b
).
 |
MATERIALS AND METHODS |
Slice preparation and patch-clamp recordings. Mice of
ages postnatal day 6 (P6)-P47 (C57-black-6; Charles River
Laboratories, Wilmington, MA) were anesthetized with Metofane
(Pitman-Moore) and decapitated, and the brains were removed in ice-cold
oxygenated artificial CSF (ACSF). Parasagittal slices (150-200
µm thick) of cerebellum were cut with a vibratome. Slices were then
incubated in ACSF at 37°C for 30-60 min and at room temperature
(20-22°C) thereafter. ACSF contained (in mM): 125 NaCl,
2.5 KCl, 2 CaCl2, 1 MgCl2,
10 glucose, 1.25 NaH2PO4H2O,
26 NaHCO3, 2 Na-pyruvate, 3 myo-inositol, and 0.5 ascorbic acid, pH 7.4, when oxygenated.
In the recording chamber, the slices were continuously perfused
(~1-2 ml min
1) with ACSF that
contained the potassium channel blockers tetraethylammonium chloride
(10 mM) and 4-aminopyridine (0.1 mM) and the
GABAA receptor antagonist bicuculline
methylchloride (20 µM). Currents through NMDA receptors
were blocked by addition of either 100 µM
D-2-amino-5-phosphonovaleric acid (D-APV) or 20 µM D-APV and 20 µM
7-chlorokynurenic acid. All recordings were performed at room
temperature. The pipette solution contained (in mM): 97.5 Cs-gluconate, 32.5 CsCl, 5 EGTA, 10 HEPES, 1 MgCl2, and 2 lidocaine n-ethyl bromide
(QX314; to block currents through sodium channels), pH 7.2. To replace
the diffusional loss of intracellular polyamines, 100 µM spermine was included in the pipette
solution. Patch pipettes (7-12 M
) were made from
borosilicate glass, coated with Sylgard (Dow Corning), and
fire-polished. Granule cells were identified by their location, appearance, and small capacitance (1-4 pF). The developmental stages
of granule cells were determined visually on the basis of their
positions within the slices.
In outside-out patch recordings, cyclothiazide (100 µM)
was added to the external solutions from a dimethylsulfoxide (DMSO) stock solution (final DMSO, 0.5%) to reduce AMPA receptor
desensitization (Partin et al., 1993
). In these experiments, patches
were first equilibrated with ACSF containing cyclothiazide before
switching to ACSF containing cyclothiazide and agonist. When activated
in this manner, ensemble or single-channel currents typically reached steady-state levels within 3 sec of the start of the application. Cyclothiazide was not included when measuring whole-cell AMPA-type currents evoked by kainate.
Data acquisition and analysis. Whole-cell and single-channel
currents were recorded using an EPC-9 patch-clamp amplifier. Data from whole-cell recordings were acquired and stored as described previously (Howe, 1996
). To minimize distortion by
resistance-capacitance (RC) filtering, whole-cell recordings were
discontinued if the membrane time constant,
= RC, exceeded 200 µsec. In most whole-cell recordings,
was <100 µsec. For
channels mediating whole-cell currents, estimates of maximal
popen were obtained from whole-cell currents by analyzing mean current versus variance plots as described in Smith et al. (1999)
.
Outside-out patch recordings were low-pass filtered at 10 kHz (
3 dB;
four-pole Bessel type) and stored on videotape. The replayed signals
were redigitized at 94 kHz and were additionally low-pass filtered with
a digital Gaussian filter. For spectral density analysis of
steady-state agonist-evoked ensemble currents in outside-out patches,
the data were digitally low-pass filtered at 2 kHz (
3 dB) and
compressed to a sampling rate of 9.4 kHz. Spectral density analysis was
performed as described previously (Howe, 1996
). Single-channel
recordings were digitally low-pass filtered at 2 kHz (
3 dB) and
compressed to final sampling rates of 31.3 or 47 kHz for inspection and
display. All the digitized records were carefully inspected for
artifacts and baseline drift before any quantitative analysis was
performed. In most records, the baseline did not drift appreciably. In
one patch, minor adjustments to the baseline were made as required.
Single-channel analysis was only performed on outside-out patch
recordings that were stable and quiet. The seal resistance of the
patches (determined from the holding current at
100 mV) ranged from
70 to 770 G
(mean, 160 G
). The mean rms noise at
100 mV was
132 ± 3 fA (121-144 fA; 31.3 kHz sampling; 2 kHz low-pass
filtering; eight patches).
As described below, two independent methods of single-channel
analysis were used to measure the amplitudes of single-channel currents. Both methods also gave estimates of the proportion of time
spent at the various open levels. We measured a mean reversal potential
of 0.85 ± 2.0 mV (n = 9 cells) in whole-cell
recordings of AMPA-type currents, so we used a reversal potential of 0 mV to calculate single-channel conductances.
Mean low-variance analysis. To measure the amplitudes of
completely resolved single-channel openings, we used the mean
low-variance method of Patlak (1988)
using routines written with
IgorPro software (WaveMetrics, Lake Oswego, OR) as described previously
(Smith et al., 1999
). The data were low-pass filtered at 2 kHz (
3 dB) and sampled at 31.3 kHz. The mean amplitude and variance of the closed-channel points (baseline) were calculated from a portion of
record just before agonist application. The baseline was set to zero by
subtracting the mean closed-channel current from all points, and the
variance was calculated for a sliding window of 11 points corresponding
to a duration of 350 µsec (2 filter rise times = 330 µsec
at 2 kHz filtering). Open points were identified according to the
criteria that the mean amplitude of the points in the window was >2
SDs of the baseline current and the variance of the points in the
window was less than one-quarter of the baseline variance. These
criteria reliably found events at least two filter rise times in
duration. The low-variance open points were appended to the current
trace, and the entire record was visually inspected. Open points that
appeared to correspond to artifacts were deleted. The computer routine
found low-variance points on either side of the baseline, and at
100
mV, outward low-variance points (which could not be AMPA receptor
currents and were excluded from further analysis) always comprised
<0.1% of the total low-variance open points found in the record.
Histograms of the low-variance open points were typically constructed
using 75-100 bins, which were fitted with the sum of multiple Gaussian
components using TAC software (Bruxton Corporation, Seattle, WA)
to obtain mean currents for the multiple open levels in the records.
Histograms of open points from longer portions of the record did not
always show clear peaks; in such cases, we used the apparent open
levels found during inspection of the data as initial values for the
fit. All histograms were fitted with the minimum number of components
required to give a good fit, with the restriction that the SD of each
Gaussian component was no greater than twice the SD of the
closed-channel current.
Hidden Markov analysis. To confirm our mean low-variance
results, we also estimated open levels by hidden Markov analysis (Chung
et al., 1990
, 1991
) using the Yale hidden Markov modeling (HMM)
module of TAC software. Hidden Markov analysis models the behavior of
ion channels by analyzing single-channel data with backward-forward
and Baum-Welch algorithms to obtain a maximum likelihood estimate of
the parameters of a discrete-time Markov model (Venkataramanan et al.,
1999a
,b
, 2000
). These parameters, whose initial values are set
by the investigator, include the number of states, the current level of
each state, the rate constants between states, and the initial state
probabilities. We fitted 2-3 sec segments of steady-state high
popen channel activity with three
classes of single-channel models: (1) models in which the open
states were connected to each other in series (class A), (2) models in
which each open state was connected to every other open state (class
B), and (3) models in which direct transitions between open states were
not allowed (class C). The models with four open states
(indicated by O) are shown below. The corresponding versions of Model A with three and five open states were also tested.
In some cases, versions of Model B with three and four open states were
compared.
Model A is approximately based on the results of Rosenmund et al.
(1998)
, who concluded that the different open levels observed in their
single-channel recordings corresponded to differently liganded open
states. These authors modeled the AMPA receptor as a tetramer that
opened to increasingly larger conductance levels when two, three, or
four agonist molecules were bound. Agonist-binding steps were not
explicitly included in any of the models used here. However, within the
context of the observations made by Rosenmund et al. (1998)
and the
high agonist concentrations used in this study (in which unliganded or
singly-liganded species would be rare), the sequential open and closed
states in Model A would correspond to differently liganded channel
states, in which the binding and unbinding of agonist molecules could
occur to and from both closed and open states. Within this same
context, Model C only allows binding and unbinding to and from closed
states, and Model B strictly implies that a channel can adopt different conductance levels with the same number of agonist molecules bound (which must be possible on thermodynamic grounds). Although these considerations guided our choice of models to evaluate, the results reported here are insufficient to decide whether the above
interpretations are physically realistic.
The initial values for rate constants between connected states were set
to 1000 sec
1. The initial values for the
amplitudes of open levels were either those estimated from the fits to
the mean low-variance open points (from the same data) or those
estimated from inspection of the records. Open levels were assigned
amplitudes in increasing order as indicated by the numbers in the
models above. Hidden Markov analysis was performed at three different
sampling rates (47, 23.5, and 11.75 kHz), and the data were low-pass
filtered at 40% of the sampling rate (18.8, 9.4, and 4.7 kHz,
respectively) by the sharp-cutoff inverse filter function of TAC
(Venkataramanan et al., 2000
). For our records, we found that different
sampling and filtering rates did not appreciably affect the number or
amplitude of the open levels. Different models were compared at the
same sampling rate and low-pass filtering. When evaluating fits
obtained with different models, the fit was deemed significantly
improved if the log likelihood of the model with more parameters
improved by 10 n log units, where n was the
number of additional nonzero parameters. Rate constants initially set
to zero could not be altered by the fitting procedure, but parameters
assigned initial nonzero values were unconstrained. If the fit
converged and any of the rate constants were very small (i.e.,
approaching zero), the states were considered disconnected; likewise,
current levels were considered superfluous if they differed from the
baseline, or another open level, by <2 SDs of the closed-channel
current (at 2 kHz filtering). Similarly, states with mean open times
close to the sampling interval were considered unnecessary.
Determining whether one or more channels were active in an
outside-out patch. To test whether our presumed single-channel records indeed represented the activity of only one AMPA receptor, we
compared the observed current levels in the record with those predicted
from the binomial distribution if the observed channel activity were
caused by several smaller channels instead of one channel with multiple
open levels. An all-points histogram of the observed steady-state
channel activity in an outside-out patch was plotted and fitted with
one Gaussian component for the closed points and one Gaussian component
for each of the open levels. From the multiple Gaussian fit to the
results, the relative area of the Gaussian component corresponding to
the closed points was used to calculate the open probability of an
individual channel if the record arose from N identical
channels (where N corresponds to the number of observed open
levels). The popen was defined as:
This estimate of the popen of
the hypothetical individual channels was used to calculate the
probability P of finding j channels simultaneously open at a given time using the binomial
relationship:
Results are given as the mean ± SEM.
 |
RESULTS |
We observed previously that cerebellar granule cells begin to
express functional AMPA receptors at approximately the time they leave
the external germinal layer (EGL) in approximately the first postnatal
week (Smith et al., 1999
). After proliferating in the EGL, granule
cells migrate inward through the ML and Purkinje cell layer,
toward their final destination in the IGL. After they reach the IGL,
granule cells receive glutamatergic synaptic input from mossy fibers
(Altman, 1972a
,b
). By the end of the second postnatal week, most
granule cells have arrived in the IGL (Altman, 1972b
). Although granule
cells can receive synaptic input soon after entering the IGL, mossy
fiber synapses do not mature until approximately P40-P60 (Hámori
and Somogyi, 1983
; Mason and Gregory, 1984
; Wall and Usowicz, 1999
). To
investigate the expression and single-channel properties of native AMPA
receptors, we used patch-clamp techniques to record agonist-evoked
whole-cell and single-channel currents through AMPA receptors in
granule cells in situ at different stages of postnatal development.
Granule cells express functional AMPA receptors
before synaptogenesis
Whole-cell currents from granule cells in the EGL, ML, and IGL
were evoked by bath application of kainate, an agonist that produces
sustained currents through AMPA-type channels because of incomplete
receptor desensitization [Patneau et al. (1993)
and references
therein]. The slow solution exchange ensured that the whole-cell
currents were not contaminated by currents through kainate-type
glutamate receptors, which quickly enter and slowly recover from
desensitization when activated by kainate (Huettner, 1990
; Herb et al.,
1992
; Lerma et al., 1993
). Concentration-response data obtained under
these conditions gave a mean EC50 value for kainate of 78 ± 10 µM (n = 5 cells,
with at least 4 concentrations each). The mean
EC50 value obtained here, similar to previous values obtained for kainate activation of AMPA receptors (Huettner, 1990
; Patneau and Mayer, 1990
; Traynelis and Cull-Candy, 1991
), is
~10-fold larger than the corresponding value obtained for
kainate-type channels expressed by granule cells in situ
[EC50 for kainate, 8 µM
(Smith et al., 1999
)]. Applications of 10 µM
kainate, a concentration that elicits substantial kainate-type currents
in granule cells if kainate receptor desensitization is reduced
(Pemberton et al., 1998
; Smith et al., 1999
), did not evoke significant
whole-cell currents in this study. Taken together, these results
support the conclusion that the kainate-evoked currents recorded here are through AMPA-type channels.
In agreement with our previous results (Smith et al., 1999
), we found
that proliferating granule cells in the outer layers of the EGL do not
express significant AMPA-type whole-cell currents in response to
saturating concentrations of kainate (Fig.
1; 300-600 µM). However,
kainate did elicit currents through AMPA receptors from granule cells
in the ML and the IGL. As shown in Figure 1, the average amplitude of
the steady-state whole-cell currents increased with the developmental
stage of the neuron, indicating that the expression of functional AMPA
receptors increases as granule cells migrate toward the IGL. In
addition, the average amplitude of whole-cell AMPA-type currents
continued to increase even after granule cells arrived in the IGL, as
evidenced by the larger amplitudes of whole-cell currents evoked from
mature IGL cells (>P40) compared with those evoked from immature IGL
cells (P6-P22). In mature IGL cells, even currents evoked by a
submaximal concentration of kainate (100 µM) were larger
than those evoked by saturating concentrations of kainate in immature
IGL cells.

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Figure 1.
Whole-cell currents through AMPA receptors
increase as cerebellar granule cells mature. The first four
bars (left to right)
denote mean currents evoked by saturating concentrations of kainate
(300-600 µM) in EGL, ML, immature IGL, and mature IGL
cells, respectively; the last bar on the
right is the mean current evoked in mature IGL cells by
100 µM kainate. Inspection of all the data indicated that
the steady-state current amplitudes were log-normally distributed. The
logarithms of the individual current amplitudes were used to calculate
the mean and SEM for each sample population. The figure shows the
antilogs of the values (mean ± SEM) obtained from the log-normal
distributions: EGL, 2.3 pA (n = 9 cells); ML, 27.5 pA (n = 5 cells); immature IGL (<P40), 57.5 pA
(n = 9 cells); mature IGL (>P40), 178 pA
(n = 3 cells); and mature IGL (100 µM
kainate), 135 pA (n = 5 cells). There were no
significant differences in whole-cell capacitance between the granule
cells in the different groups.
|
|
Detectable AMPA receptor single-channel activity in
outside-out patches from migrating granule cells
To study the properties of the channels underlying the AMPA-type
whole-cell currents, we pulled outside-out patches from granule cells
migrating through the ML and bath-applied saturating concentrations of
kainate (1 mM) or glutamate (2 mM). Both
agonists were applied in the presence of 100 µM
cyclothiazide to reduce AMPA receptor desensitization (Partin et al.,
1993
). We observed currents through AMPA receptors evoked by glutamate
in 28 of 31 outside-out patches from granule cells in the ML. Some
patches appeared to contain many channels, giving ensemble currents of
up to 40 pA, but it was not uncommon for patches to show only one or
two active channels.
Although our whole-cell recordings indicated that kainate-type currents
were minimal or absent under these experimental conditions (see above),
the whole-cell results do not exclude the possibility that kainate
receptors could have contributed to the observed single-channel
activity during occasional escapes from desensitization. We believe,
however, that our single-channel records were not contaminated with
kainate receptor activity. First, although single-channel currents
through kainate-type channels can be observed in patches from EGL
granule cells, the very small conductances of the kainate receptors
expressed in granule cells make detection of discrete single-channel
currents unlikely at the developmental stages studied here (Smith et
al., 1999
). Second, the characteristics of kainate receptor
single-channel activity observed in patches from granule cells are
quite different from the single-channel activity described here
(T. C. Smith and J. R. Howe, unpublished observations) (Smith et al., 1999
). For example, in the present study, saturating
concentrations of both kainate and glutamate evoked single-channel
activity with a very high popen,
whereas kainate receptors expressed by EGL granule cells show a much
lower popen, even when high agonist concentrations are applied after reducing desensitization with concanavalin A. Finally, the concentration dependence of the channel activity we observed in the present work was entirely consistent with
our concentration-response data for AMPA-type whole-cell currents.
There were several characteristics common to the single-channel
activity of the AMPA receptors that we studied in ML patches. At high
agonist concentrations, all the channels displayed periods of high
popen activity that lasted hundreds of
milliseconds or even seconds (Fig.
2A). These high
popen periods are reminiscent of the
high popen activity seen with
NMDA-type glutamate receptors (Jahr and Stevens, 1987
; Howe et al.,
1988
, 1991
). For NMDA receptors, however, this high
popen activity is also observed at low
agonist concentrations (Gibb and Colquhoun, 1992
), whereas that was not the case for the AMPA-type channels studied here. In this regard, the
high popen periods displayed by AMPA
receptors are more similar to the activity of nicotinic acetylcholine
receptors, which, at high agonist concentrations, display high
popen periods thought to reflect
escapes from desensitized states (Sakmann et al., 1980
; Colquhoun and
Ogden, 1988
). High popen AMPA receptor
activity was interrupted by silent periods, which themselves could be
hundreds of milliseconds long (Fig. 2A) and which
likely resulted from entry into desensitized states. (Although 100 µM cyclothiazide was present, it slows, rather
than removes, desensitization.) In support of this view, preliminary
results suggest that the duration of the long closed periods increases
in the absence of cyclothiazide, although high
popen periods evoked by kainate
remain.

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Figure 2.
Single-channel activity of an AMPA receptor
expressed by a migrating granule cell. Holding potential, 100 mV.
A, Steady-state activity of an AMPA receptor in an
outside-out patch from a granule cell in the ML. Glutamate (2 mM) and cyclothiazide (100 µM) were present
throughout the recording. The zero current level is indicated by the
solid horizontal
lines. Data were sampled at 31.3 kHz and low-pass
filtered at 2 kHz ( 3 dB). B, Portions of the
single-channel recording shown in the top
trace of A on a faster time scale.
|
|
The high popen behavior of the
channels allowed us to identify patches that appeared to contain only
one or two active channels. Almost all the channels (11 of 13) in these
patches visited more than one conductance level, the only exceptions
being channels with very small single-channel currents. Examples of
transitions to conductance sublevels are shown in Figure
2B. Although almost all the data presented in this
study were obtained at saturating agonist concentrations, we also
recorded single-channel currents over a range of concentrations.
Channels showing multiple open levels spent more of their open time in
larger sublevels as the agonist concentration was increased, as
reported previously for recombinant AMPA receptors (Rosenmund et al.,
1998
). Although this was an obvious feature of all our recordings, to
quantify the results at low agonist concentrations in patches
containing two channels is difficult because the low
popen made the assignment of openings
to a particular channel uncertain. However, we did obtain results in
three one-channel patches over a wide range of glutamate
concentrations. On average, the proportion of open time spent at the
largest open level increased from 6 ± 3% at 20 µM glutamate to 28 ± 7% at 100-200
µM glutamate and 82 ± 7% at 2 mM glutamate.
Native AMPA receptors show up to four conductance sublevels
We limited our single-channel analysis to patches that appeared to
contain only one or two active channels, as determined from analysis of
the high popen behavior at 2 mM glutamate (with 100 µM
cyclothiazide). In patches that appeared to contain two channels, there
were often portions of the record in which only one channel was active,
due to entry into long-lived closed or desensitized states. Several
consistent characteristics of the records indicate that the multiple
current levels that we observed are in fact conductance substates of
single AMPA receptors, rather than currents through several smaller
channels. First, there were apparently direct transitions between
nonadjacent open levels. Second, for some channels, the open levels
observed were clearly not multiples of each other, as would be expected
if different open levels corresponded to the simultaneous opening of
more than one channel. Third, the high
popen periods contained many brief closings that appeared to be direct transitions from and to the largest
open level. Finally, as noted above, the high
popen periods were interrupted by shut
periods that lasted up to hundreds of milliseconds. Given the long
duration and relative infrequence of these shut periods, it is highly
unlikely that two or more independently gating channels would give rise
to these shut periods by opening and closing simultaneously. Therefore,
if multiple channels contributed to the record, one would expect these
long-lived closed periods to be bordered by periods in which only
smaller current levels were observed. This was clearly not the case
(see Fig. 2).
Although most of the larger-conductance channels that we studied
displayed open levels that were not multiples of each other, the
closely spaced open levels observed for smaller-conductance channels
often appeared to be. To evaluate further the likelihood that the
channel activity observed arose from multiple channels, we compared the
observed proportion of time spent at each open level with the
proportions predicted from the binomial distribution if the activity
arose from multiple channels gating independently. For example, how
likely was it that a patch appearing to contain only one active AMPA
receptor with open levels of 3, 5, and 7 pS actually contained three
identical channels of 2-3 pS? In Figure 3A, the filled
bars illustrate the relative time one such channel spent at
each open level at 2 mM glutamate; the
open bars represent the predicted probabilities
of observing one, two, or three independent channels open
simultaneously (calculated as described in Materials and Methods).
Clearly the results deviate from those predicted from the binomial
distribution. A similar analysis was performed for eight different
channels, and in each case the predicted proportion of time spent at
each current level differed substantially from the proportions observed
experimentally. We also calculated how much the area under the
closed-points component (see Materials and Methods) would have to
differ from its fitted area to give hypothetical
popen values consistent with the
observed results if the activity arose from multiple channels. In each
case this difference exceeded 80% of the measured area of the
closed-points component, which far exceeded the uncertainty of the
measurements.

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Figure 3.
The observed current levels in outside-out patch
recordings are inconsistent with the activity of multiple channels.
A, Analysis of data from a putative one-channel
recording. The filled bars indicate the
proportion of time at each open level
(PN) observed during steady-state
activity evoked by 2 mM glutamate (with
cyclothiazide). The open bars indicate
the proportion of time at each current level predicted from the
binomial distribution (described in Materials and Methods) if the
currents in the record arose from the activity of three independently
gating channels. B, Mean ratios (± SEM) of the observed
PN to the
PN predicted from the binomial
distribution (if the activity arose from multiple independently gating
channels). The results are from eight records in which two
(circles), three (squares), or four
(triangles) open levels were evident
(n = 2, 3, and 3 individual channels,
respectively). Note that the y-axis is discontinuous.
For points off the scale, the mean ratios are given in
parentheses.
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|
The mean results from this analysis of eight individual AMPA receptors
are summarized in Figure 3B, which shows the average ratio
of the observed proportion of time the record spent at a particular
current level to the proportion predicted if the current levels arose
from multiple channels. Because the predictions differ quite strikingly
from the observed data, we believe that our presumed single-channel
records are indeed likely to contain only one active channel, even when
the larger open levels appear to be multiples of the smallest.
Granule cells express AMPA receptors with heterogeneous
conductance levels
Although almost all the AMPA receptors that we studied in patches
showed multiple open levels at saturating concentrations of agonist,
there was considerable channel-to-channel variability in the amplitudes
of the conductance sublevels, as well as in the number of levels
detected. The single-channel currents through 13 channels were measured
during activity evoked by 2 mM glutamate. Single-channel
currents evoked by 1 mM kainate were also measured for 3 channels. Interestingly, although agonist-dependent differences in the
apparent unitary conductance of AMPA-type channels have been found
using fluctuation analysis (for example, see Jonas and Sakmann, 1992
;
Wyllie et al., 1993
; Swanson et al., 1997
), the conductance levels
observed with kainate and glutamate did not differ significantly for
any of the channels studied here.
Figure 4 illustrates examples of data
from a smaller AMPA receptor (Fig.
4A,B) and a larger AMPA receptor
(Fig. 4C, D) in outside-out patches from two
different ML cells. Three small, closely spaced, open levels were
detected for the AMPA receptor shown in Figure 4A. In
Figure 4A the dotted lines show
the currents for each open level superposed on examples of the activity
of this channel. The three peaks in the histogram of low-variance open
points (from a selected portion of the record) correspond to
conductances of 3, 6, and 9 pS (Fig. 4B). The
larger-conductance AMPA receptor in Figure 4C visited four
detectable open levels. At 2 mM glutamate the
channel spent most of its time at the largest conductance level (22 pS), but examples of long-lived sojourns at the two smallest levels (7 and 14 pS) were also evident. In addition, the record contained
openings to a level with a mean conductance of 18 pS, most of which
were short-lived. A histogram of low-variance open points obtained from
this channel is shown in Figure 4D, with the four
Gaussian fit to the results superposed.

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Figure 4.
AMPA receptors expressed by migrating
granule cells show heterogeneity in the number and amplitudes of their
conductance sublevels. The zero current levels are indicated by
solid lines. Open levels are indicated by
dotted lines. Channel currents were
activated by 2 mM glutamate in the presence of 100 µM cyclothiazide. A, Outside-out patch
recording from a granule cell in the ML. Holding potential, 150 mV.
The second and fourth
traces from the top are expanded portions
of the first and third
traces, respectively, the beginning of which are
indicated by asterisks. Data were sampled at 47 kHz and
low-pass filtered at 2 kHz ( 3 dB). B, Histogram of
mean low-variance open points from the channel recording shown in
A. The histogram was fitted with the sum of three
Gaussian components, giving mean conductance levels of 3, 6, and 9 pS
(thin lines, individual Gaussian
components; thick line, sum of individual
components). C, Outside-out patch recording from a
granule cell in the ML. Holding potential, 100 mV. Data were sampled
at 31.3 kHz and low-pass filtered at 2 kHz ( 3 dB). D,
Histogram of mean low-variance open points from the channel
recording shown in C. The histogram was fitted with the
sum of four Gaussian components, giving mean conductance levels of 7, 14, 18, and 22 pS (thin lines, individual
Gaussian components; thick line, sum of
individual components).
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|
Some of the patch-to-patch variability in conductance levels may
reflect differences in the repertoire of AMPA receptors expressed by
different granule cells. It was clear, however, that individual cells
expressed multiple types of AMPA receptors. In each patch that
contained two active channels, the two channels showed distinguishably different conductance levels. An example of results from a patch that
contained two channels is illustrated in Figure
5. At the beginning of the trace, only
the relatively smaller channel is active. In the middle of the trace,
both channels are active. Near the end of the trace in Figure 5A, the
smaller channel is silent, leaving only the activity of the larger
channel. Figure 5, B and C (traces taken
from the beginning and end of the trace in Fig. 5A),
illustrates that the channel in Figure 5Ba has a smaller
single-channel conductance than does the one in Figure 5Bb.
This is also evident when histograms of low-variance open points are
overlaid (Fig. 5D; histograms were constructed from portions
of the trace where only one channel was active).

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Figure 5.
Two AMPA receptors with different
single-channel conductances in the same outside-out patch. Holding
potential, 100 mV. Data were sampled at 31.3 kHz and low-pass
filtered at 2 kHz ( 3 dB). A, Outside-out patch
recording from a granule cell in the ML. Note that two channels are
active simultaneously in the middle of the recording.
Ba, Portion from the beginning of the recording in
A on a faster time scale, where only the smaller channel
is active. b, Portion near the end of the recording in
A on a faster time scale, where only the larger channel
is active. Ca,b, Portions of records in
B on a faster time scale to show the difference in the
largest conductance levels (dotted
horizontal lines). D,
Overlaid histograms of low-variance open points from each channel. The
shaded histogram is derived from the activity of the
smaller channel in Ba. The unshaded
histogram is derived from the activity of the larger channel in
Bb.
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|
We used two independent methods of single-channel analysis to estimate
the open levels of 13 individual AMPA receptors in eight outside-out
patches. Consideration of all the records indicated that 2-3 pS was
the minimum separation from baseline, and between levels, that we could
resolve (see Materials and Methods). At holding potentials of
100 to
150 mV, this corresponded to approximately twice the SD of the
closed-channel current. We measured the open levels of most channels
using mean low-variance analysis. For three channels, however, the
rapid kinetics of the channel behavior made detection of open levels
with mean low-variance analysis unreliable (for example, compare the
kinetic characteristics of the channels shown in Figs. 4C
and 5). The three channels exhibiting rapid kinetics were those with
the largest conductance levels; although it is possible that there is a
correlation between channel conductance and gating kinetics, this
apparent difference may reflect the better signal-to-noise ratio for
the larger-conductance channels. To estimate the open levels of
channels with rapid kinetics, we used HMM techniques as described in
Materials and Methods.
We first used HMM to verify the amplitudes of open levels that we
measured by mean low-variance analysis. The open levels estimated with
HMM at three different filter settings (18.8, 9.4, and 4.7 kHz) were
similar, and they agreed well with the values obtained from fits to the
mean low-variance open points (data low-pass filtered at 2 kHz). The
levels obtained with HMM and mean low-variance analysis were usually
identical and, on average, agreed within 1 pS. The observation that the
amplitudes of the open levels were relatively insensitive to low-pass
filtering implies that the open levels detected are unlikely to reflect incompletely resolved transitions between different channel states. We
then used HMM to estimate the open levels of channels not amenable to
mean low-variance analysis because of their rapid kinetics. Although
HMM is in principle able to detect very small signals, only levels
above our resolution at 2 kHz filtering are depicted in Figure
6.

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Figure 6.
Heterogeneous open levels of AMPA
receptors expressed by granule cells in situ. Amplitudes
of the open levels (in picosiemens) of 13 individual AMPA receptors
observed in outside-out patch recordings (circles,
squares, triangles, and
diamonds show levels in order of decreasing amplitude).
Current levels were measured at 100 mV (or 150 mV for channel 6)
using mean low-variance analysis and/or hidden Markov analysis and
converted to conductances using a reversal potential of 0 mV. Channels
11-13 showed rapid kinetics and were analyzed exclusively with hidden
Markov modeling. Channels are plotted in order of increasing amplitude
of the largest open level. For each channel where four open levels were
detected (channels 9-13, brackets), HMM fits with four
open states were significantly better than fits with three open
states.
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|
Figure 6 summarizes the number and amplitudes of open levels we
observed from the single-channel activity of 13 individual AMPA
receptors. These channels exhibited from one to four detectable open
levels that ranged in conductance from 3 to 44 pS. Interestingly, there
is a correlation between the number of open levels detected and their
amplitudes. It is possible that the smaller-conductance channels have
additional open levels that are too small or too brief to detect.
Alternatively, AMPA receptors may truly differ in the number of their
open states.
In addition to providing another method to measure channel open levels,
HMM allowed a quantitative assessment of the number and connectivity of
open levels that best described the data. For the five largest
conductance channels (Fig. 6, bracketed channels 9-13), HMM
analysis showed that Model A with four open states (in order of
increasing conductance) gave significantly better fits to the
single-channel records than did analogous models having three open
states. In addition, versions with five open states did not
significantly improve the fit to the data. For three of five channels,
models that allowed direct transitions between all open levels (Model
B) gave better fits to the data than did Model A. For each channel, the
worst fits were obtained using Model C, which disallowed direct
transitions between open states. The results of the above comparisons
are summarized in Table 1.
The HMM analysis also confirmed our impression that different channels
showed different kinetic behavior. Figure
7 shows the rate constants and mean open
times obtained from fitting the four-open-state version of Model A to
the activity of two different AMPA receptors (sampled at 23.5 kHz;
filtered at 9.4 kHz). The mean open times for the channel with the
relatively faster kinetics (Fig. 7B) are much briefer than
the window duration used for mean low-variance analysis (330 µsec),
and at 2 kHz low-pass filtering the record consisted primarily of
incompletely resolved events. Although Model B usually gave better fits
than Model A, the open times obtained with the two types of models were
very similar for each channel analyzed. Thus although the connectivity
of the states is somewhat unresolved, we believe that the mean open
times estimated with HMM are good approximations of channel dwell
times.

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Figure 7.
Rate constants obtained from hidden Markov
modeling for two channels in different ML patches. The mean dwell times
(in milliseconds) are shown for the four open states (states
5-8) in bold type. Rate
constants >1000 sec 1 were rounded to three
significant figures. A, The channel that gave these
results is the channel illustrated in Figure 4C. This
channel displayed relatively long-lived sojourns in the various open
levels. Both HMM and mean low-variance analysis gave conductance levels
of 7, 14, 18, and 22 pS (states 5-8, respectively).
B, The channel that gave these results is illustrated in
Figure 5, Ba and Ca. The rapid kinetics
of this channel made estimates of the open levels from mean
low-variance analysis unreliable. The conductances obtained from HMM
analysis were 6, 15, 22, and 34 pS (states 5-8,
respectively). The mean open times estimated for this channel were all
<100 µsec.
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Rectification behavior of AMPA receptors in granule cells
in situ
One possible explanation for the heterogeneity we observed in
single-channel conductances is that the channels in ML patches differ
in subunit composition. Inclusion of the edited GluR2 subunit in
coexpression experiments reduces the single-channel conductance of
GluR4 channels (Swanson et al., 1997
). In addition, the relative abundance of GluR2 has been demonstrated to affect sensitivity to block
by internal polyamines (Washburn et al., 1997
). Therefore, because of
the observed variability in conductances, we asked whether native AMPA
receptors in granule cells might also exhibit heterogeneity in their
rectification properties.
We first asked whether granule cells show significant cell-to-cell
variability in the average rectification behavior of AMPA receptors, as
has been shown for granule cells in culture (Kamboj et al., 1995
). In
contrast to previous in vitro results, we found that
AMPA-type whole-cell currents evoked by glutamate or kainate consistently showed linear or outwardly rectifying I-V
relations in both ML and IGL cells (Fig.
8A,B;
ML, n = 4 cells; IGL, n = 5 cells).

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Figure 8.
Whole-cell currents through AMPA receptors in
granule cells show linear or outwardly rectifying current-voltage
relations, as do some ensemble patch currents. A, B,
Whole-cell I-V curves from a granule cell in the ML
(A) and the IGL (B).
C, I-V curve (a)
and ensemble currents (b) from an outside-out
patch excised from a granule cell in the ML. Several channels were
active in this patch. Holding potentials (in millivolts) are indicated
to the left of the traces in
b. Data were sampled at 31.3 kHz and low-pass filtered
at 2 kHz ( 3 dB).
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In contrast to the whole-cell results, agonist-evoked ensemble currents
in outside-out patches from migrating granule cells showed both inward
and outward rectification, suggesting that these patches contained
different subsets of AMPA receptors. In four patches, we observed
linear or outwardly rectifying I-V relations (Fig.
8C), whereas three other patches showed inward
rectification. These results suggest that the linear
I-V relations of whole-cell currents may reflect
the average behavior of a heterogeneous population of AMPA receptors,
rather than reflecting the rectification behavior of a single type of
AMPA receptor.
The heterogeneous rectification behavior of AMPA receptors was also
evident in single-channel recordings. Some channels exhibited rectification behavior similar to that in the multichannel patch shown
in Figure 8C, which passed outward currents at positive potentials, whereas others showed some flickery channel block, as if
the channels might be weakly blocked by internal polyamines. Still
other channels, such as the one illustrated in Figure
9, appeared to be more strongly blocked
by internal polyamines, exhibiting a marked decrease in
popen at positive potentials. This
channel showed long silent periods at positive potentials that were
occasionally interrupted by shorter periods of activity in which little
or no flickery channel block was evident (Fig. 9A,
top two traces). Interestingly, the
single-channel I-V curve exhibited only slight inward
rectification (Fig. 9B, filled
circles), whereas the mean current measured for
representative portions of the record at each potential showed strong
inward rectification (open circles). Comparison
of the two I-V curves in Figure 9B demonstrates
that the rectification behavior of this channel is manifest primarily as a dramatic reduction in popen at
positive potentials. Taken together, these data indicate that migrating
granule cells express AMPA receptors that show substantial
heterogeneity in both their single-channel conductances and
rectification.

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Figure 9.
Inwardly rectifying AMPA receptor expressed by a
migrating granule cell. A, Outside-out patch recording
from a granule cell in the ML. Holding potentials (in millivolts) are
indicated to the left of the traces.
Glutamate (2 mM) and cyclothiazide (100 µM)
were present throughout the recording. Data were sampled at 31.3 kHz
and low-pass filtered at 2 kHz ( 3 dB). B,
I-V relations for the channel shown in
A. The filled circles
indicate the single-channel current (largest detectable open level) at
each potential, whereas the open circles
denote the average current passing through the channel per unit time at
each potential (from 4.5 sec of continuous data at each
potential).
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Granule cells express femtosiemens-conductance AMPA receptors
Consistent with the size of the single-channel currents described
above, most multichannel patches from ML cells showed large increases
in current noise after application of agonist (Fig. 10A). In contrast,
IGL patches that gave agonist-evoked currents had much smaller
increases in current noise (Fig. 10B), and directly resolvable single-channel currents were noticeably absent in IGL patches with one exception. In addition, the frequency with which agonist-evoked currents were observed was lower in IGL patches (5 of
10) than in ML patches (28 of 31).

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Figure 10.
Granule cells express AMPA receptors
with femtoseiman conductances. A, Top,
Outside-out patch from a granule cell in the ML. Data were sampled at
9.4 kHz and low-pass filtered at 2 kHz ( 3 dB). Bottom,
Power spectrum of the steady-state ensemble patch current shown in
A, top; noise = 3.7 pS (not corrected for
popen). B,
Top, Outside-out patch from a mature IGL cell (P47).
Note the much smaller agonist-induced current noise compared with the
recording in A. Data were sampled at 9.4 kHz and
low-pass filtered at 2 kHz ( 3 dB). Bottom, Power
spectrum of the steady-state ensemble patch current shown in
A, top; noise = 0.43 pS (not corrected for popen).
C, Outside-out patch recording from a granule cell in
the ML. Note the small sustained inward current, in addition to the
single-channel activity (shown on an expanded time scale in the
bottom trace). Data were sampled at 31.3 kHz and low-pass filtered at 1 kHz ( 3 dB). The different kinetics of
the ensemble patch currents in B and C
reflect differences in the rates of solution exchange in the two
experiments. cyclo, Cyclothiazide.
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Our results suggest that large-conductance AMPA receptors are primarily
absent from the cell bodies of IGL granule cells, although
smaller-conductance channels are still somatically localized. In each
of the five IGL patches that responded to agonist, we observed small
inward currents that developed and recovered gradually (Fig.
10B). Similar currents were observed in two ML
patches. We believe that these low-noise responses are mediated by AMPA
rather than by kainate receptors, because currents evoked by kainate (in the absence of concanavalin A) are blocked by the AMPA receptor antagonist GYKI 53655 (Smith et al., 1999
). In the low-noise
response from the ML patch shown in Figure 10C,
small-conductance single-channel activity is superposed on a
steady-state, low-noise current. The one IGL patch that showed
detectable single-channel activity gave a very similar response.
Repeated agonist application to each of the seven low-noise patches
(two ML and five IGL patches) reproducibly evoked inward currents that
appeared to result from the activity of numerous AMPA receptors with
very small conductances. Four patches showed agonist-evoked noise
increases that, although small, were sufficient to estimate the
apparent unitary conductance of the channels underlying the small
inward currents with spectral density analysis. The mean (± SEM)
noise value from these four patches was
355 ± 139 fS.
Taken together, our results suggest that granule cells in
situ express at least two populations of AMPA receptors on their cell bodies during development: larger-conductance AMPA receptors expressed by migrating cells that become relatively inaccessible to a
patch pipette after reaching the IGL and femtosiemens-conductance AMPA
receptors that are somatically expressed by granule cells in the ML and IGL.
 |
DISCUSSION |
One of our main findings is that granule cells in situ
express AMPA receptors with markedly different conductances. The
femtosiemens-conductance channels we detected in some patches are
similar to channels in cultured granule cells (Cull-Candy et al., 1988
;
Wyllie et al., 1993
). Patches from migrating granule cells contained
larger-conductance channels, most of which exhibited multiple open levels.
AMPA receptors expressed in cerebellar granule cells
in situ
Our results suggest that different populations of AMPA receptors
may have different subcellular distributions in mature granule cells.
The observation that the larger-conductance AMPA receptors (largest
open level > 2 pS) became inaccessible to a patch pipette soon
after granule cells arrive in the IGL suggests that these channels
cluster at synapses. In contrast, the presence of
femtosiemens-conductance channels in patches excised from IGL cell
bodies indicates that they are located extrasynaptically, although we
cannot exclude the possibility that they are also expressed at
synapses. Our finding that the density of larger-conductance AMPA
receptors is low on IGL cell bodies is consistent with the results of
Silver et al. (1996a)
, who did not detect single-channel currents in patches excised from IGL cell bodies. Our use of cyclothiazide to slow
desensitization probably explains why we detected
femtosiemens-conductance channels in somatic patches from IGL cells
whereas Silver et al. (1996a)
did not. The femtosiemens-conductance
channels were observed more frequently in patches from mature IGL,
rather than migrating, granule cells. Analysis of whole-cell current
noise also gave smaller
noise values for IGL
than ML cells (ML, 4.21 ± 1.29 pS and n = 5 cells; IGL, 2.22 ± 0.30 pS and n = 11 cells;
values corrected for popen), although
the difference was not statistically significant (P = 0.06, Student's t test). Together the results suggest that
the relative expression of femtosiemens-conductance channels increases
as granule cells mature.
The conductance of the femtosiemens channels agrees well with the
estimated conductance of GluR2 homomers and is smaller than that of
receptors comprised of significant amounts of GluR1, GluR3, or GluR4
(Swanson et al., 1997
; Rosenmund et al., 1998
; Derkach et al., 1999
).
Thus, although recent work has demonstrated that interactions between
GluR2 and proteins such as GRIP (Dong et al., 1997
) and
NSF (Nishimune et al., 1998
; Osten et al., 1998
; Song et al.,
1998
) are involved in synaptic targeting of AMPA receptors, our results
suggest that the extrasynaptic receptors we have detected in innervated
granule cells contain substantial amounts of GluR2.
Although we do not know whether expression of the larger-conductance
channels present in ML cells continues in IGL cells, synaptic clustering seems plausible, because the apparent
lack of somatic expression in IGL cells coincides with synaptogenesis. The whole-cell
noise values for ML and IGL
cells suggest coexpression of the larger-conductance and
femtosiemens-conductance AMPA receptors at both developmental stages.
Furthermore, on average the larger-conductance channels in
ML patches have conductances similar to the average conductances
estimated for synaptic AMPA receptors at mossy fiber synapses (12-20
pS) (Traynelis et al., 1993
; Silver et al., 1996b
). Previous work has
shown that AMPA (Craig et al., 1993
; Mammen et al., 1997
; O'Brien et
al., 1997
), acetylcholine (Anderson and Cohen, 1977
; Frank and
Fischbach, 1979
), GABAA (Killisch et al., 1991
),
and glycine (Kirsch et al., 1993
; Bechade et al., 1996
) receptors
cluster at synapses during synaptogenesis in cultured cells. It is
possible that granule cell AMPA receptors cluster at synaptic sites in
response to a signal resulting from mossy fiber activity. In support of
this, recent findings indicate that the immediate-early gene product
Narp, a protein expressed by presynaptic and postsynaptic terminals,
clusters AMPA receptors at synapses in an activity-dependent manner
(Tsui et al., 1996
; O'Brien et al., 1999
).
Heterogeneity of AMPA receptor single-channel properties
Another main finding of this work is that the larger-conductance
AMPA receptors expressed by migrating granule cells exhibit considerable heterogeneity in their conductances, probably reflecting differences in subunit composition and perhaps differences in the
relative contribution of alternative splice variants. Granule cells
express mainly GluR2, GluR4, GluR4c, and to a lesser extent GluR1
(Monyer et al., 1991
; Pellegrini-Giampetro et al., 1991
; Gallo et al.,
1992
; Sato et al., 1993
; Day et al., 1995
; Hack et al., 1995
; Ripellino
et al., 1998
). Swanson et al. (1997)
found that recombinant GluR4
homomers activated by glutamate showed three open levels (8, 15, and 24 pS), whereas heteromeric GluR2/4 channels had only two smaller open
levels (4 and 10 pS), and GluR2 homomers gave an estimated
noise of <1 pS. Although the relationship between GluR2 abundance and single-channel conductance has not been
rigorously examined, the relative abundance of GluR2 has been
demonstrated to affect other channel properties. Previous work suggests
that AMPA receptors are not assembled with the fixed, or severely
limited, stoichiometry of other ligand-gated ion channels (Cooper et
al., 1991
; Gu et al., 1991
; Kuhse et al., 1993
; Geiger et al., 1995
;
Kellenberger et al., 1997
; Tretter et al., 1997
; Washburn et al.,
1997
). Although our results do not exclude the possibility that certain
subunit assemblies may be preferred or that post-translational
modifications contribute to channel-to-channel variability, the
heterogeneity that we observe in conductances supports the hypothesis
that AMPA receptor assembly is, at least in part, combinatorial. Thus
differences in subunit composition are likely to be a source of
heterogeneity in the number and amplitudes of open levels.
Several channels that we studied showed four distinguishable open
levels. Invariably, channels showing fewer conductance levels were
those where the detection of conductance sublevels would have been
limited by the small size of the single-channel currents. Thus the
smaller channels may have had additional sublevels that were below our
resolution. Rosenmund et al. (1998)
recently proposed a tetrameric
model for recombinant AMPA receptors that included a singly-liganded
nonconducting state. In agreement with the results of Rosenmund et al.
(1998)
, we observed that the prevalence of sojourns in the different
open levels depended on agonist concentration, with openings to the
largest level becoming increasingly frequent as agonist concentration
increased. If the different open levels that we observed correspond to
differently liganded channel states, then the presence of four
conductance levels admits two explanations. Either all AMPA receptors
are tetramers, with some channels able to conduct in the
singly-liganded state; or the singly-liganded state is always
nonconducting, and some AMPA receptors are pentamers. The latter
explanation might reconcile previous work supporting both tetrameric
and pentameric assemblies (Mano and Teichberg, 1998
; Rosenmund et al.,
1998
; Rubio et al., 1998
).
Functional implications of heterogeneous AMPA
receptor properties
Whether the AMPA receptors expressed by migrating granule cells
serve a developmental function is unknown. A direct role in migration
seems unlikely because of the observation that the AMPA receptor
antagonist CNQX had no effect on granule cell migration (Komuro and
Rakic, 1993
). However, in vitro results have suggested a
role for AMPA receptors in neuritic development (Cox et al., 1990
;
Mount et al., 1993
; Pizzi et al., 1994
).
It is also possible that the appearance of AMPA receptors in
noninnervated granule cells simply reflects the preparation for impending synaptogenesis. If the channels in migrating cells are destined for synapses, this raises the possibility that the synaptic population of AMPA receptors is heterogeneous. Synaptic currents at the
mossy fiber-granule cell synapse show approximately linear I-V relations (Silver et al., 1996b
). One
explanation for this result is that all synaptic channels in granule
cells contain substantial amounts of GluR2. However, we consistently
found linear or outwardly rectifying I-V relations for
whole-cell currents in both ML and IGL cells, although single-channel
and ensemble currents in ML patches indicate that the rectification
behavior of individual AMPA receptors varied substantially. Thus it is possible that individual synaptic channels exhibit marked variation in
permeation properties, yet together give an approximately linear I-V relationship. Indeed, nonstationary noise analysis of
mossy fiber-evoked EPSCs has yielded average unitary conductance
estimates that appear too large to arise from a homogenous population
of GluR2-containing channels (Traynelis et al., 1993
; Silver et al., 1996b
; Swanson et al., 1997
).
Although individual neurons can selectively target subsets of AMPA
receptors to different synapses (Rubio and Wenthold, 1997
; Tóth and McBain, 1998
), there are also indications that
subsets of AMPA receptors present at a given synapse can vary.
Estimates of the mean conductance of receptors at the mossy
fiber-granule cell synapse range from 12 to 20 pS (Traynelis et al.,
1993