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The Journal of Neuroscience, October 1, 1998, 18(19):7709-7716
Glial Contribution to Glutamate Uptake at Schaffer
Collateral-Commissural Synapses in the Hippocampus
Dwight E.
Bergles and
Craig E.
Jahr
Vollum Institute, Oregon Health Sciences University, Portland,
Oregon 97201
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ABSTRACT |
Astrocytes in the hippocampus express high-affinity glutamate
transporters that are important for lowering the concentration of
extracellular glutamate after release at excitatory synapses. These
transporters exhibit a permeability to chaotropic anions that is
associated with transport, allowing their activity to be monitored in
cell-fee patches when highly permeant anions are present. Astrocyte
glutamate transporters are highly temperature sensitive, because
L-glutamate-activated, anion-potentiated transporter currents in outside-out patches from these cells exhibited larger amplitudes and faster kinetics at 36°C than at 24°C. The cycling rate of these transporters was estimated by using paired applications of either L-glutamate or D-aspartate to measure
the time necessary for the peak of the transporter current to recover
from the steady-state level. Transporter currents in patches recovered
with a time constant of 11.6 msec at 36°C, suggesting that either the
turnover rate of native transporters is much faster than previously
reported for expressed EAAT2 transporters or the efficiency of these
transporters is very low. Synaptically activated transporter currents
persisted in astrocytes at physiological temperatures, although no
evidence of these currents was found in CA1 pyramidal neurons in
response to afferent stimulation. L-glutamate-gated
transporter currents were also not detected in outside-out patches from
pyramidal neurons. These results are consistent with the hypothesis
that astrocyte transporters are responsible for taking up the majority
of glutamate released at Schaffer collateral-commissural synapses in
the hippocampus.
Key words:
glutamate transporter; astrocyte; GLT-1; GLAST; EAAC1; hippocampus; CA1
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INTRODUCTION |
Removal of glutamate from the
extracellular space is achieved via the activity of high-affinity
Na+-dependent transporters. This clearance of
extracellular glutamate is necessary to maintain low ambient levels,
reducing the tonic activation of receptors so that excitotoxic neuronal
degeneration does not occur (Rothstein et al., 1996 ; Tanaka et al.,
1997 ). Members of the glutamate transporter family exhibit cell
type-specific expression, with GLT-1 and GLAST expressed in
glial cells (primarily astrocytes and Bergmann glial cells) and EAAC1
and EAAT4 expressed in neurons (Kanai et al., 1995 ; Yamada et
al., 1996 ; but see Conti et al., 1998 ). However, the relative
contribution of neuronal versus glial transport in the uptake of
synaptically released glutamate is not known. A dramatic demonstration
of the importance of the two glial transporters in glutamate
homeostasis has emerged from studies in which their expression has
either been reduced or blocked entirely. These animals have
elevated glutamate in the CSF, exhibit extensive neuronal
degeneration, suffer from spontaneous seizures, and ultimately die
prematurely (Rothstein et al., 1996 ; Tanaka et al., 1997 ; Watase et
al., 1997 ). The role of the neuronal EAAC1 transporter is less certain.
Animals lacking EAAC1 transporters develop essentially normally, do not
suffer seizures, and exhibit no neurodegeneration (Peghini et al.,
1997 ). Although this phenotype contrasts with animals treated with
antisense (Rothstein et al., 1996 ), the spontaneous seizures observed
in antisense-treated animals may result from dysfunction of GABA metabolism (Sepukty et al., 1997 ).
By recording the net charge movement that accompanies glutamate
transport, it has been possible to monitor the activity of these
transporters in glial cells after release of glutamate at excitatory
synapses, both in culture (Mennerick and Zorumski, 1994 ; Linden, 1997 )
and in acute slices of hippocampus (Bergles and Jahr, 1997 ) and
cerebellum (Bergles et al., 1997 ; Clark and Barbour, 1997 ). These
studies indicate that some of the glutamate released into the synaptic
cleft reaches glial membranes, despite evidence that glutamate
transporters are expressed by the postsynaptic neurons (Rothstein et
al., 1994 ). At climbing fiber synapses in the cerebellum, less than
one-quarter of the glutamate released from a vesicle is recovered
postsynaptically (Otis et al., 1997 ), providing further evidence that
glial cells are primarily responsible for the uptake of synaptically
released glutamate. However, these studies were performed at room
temperature. Given the reportedly high-temperature dependence of
glutamate flux (Wadiche et al., 1995a ) and the apparent rapid turnover
rate of endogenous transporters (Bergles and Jahr, 1997 ), it is
possible that at physiological temperatures neuronal transporters may
be more effective in restricting the diffusion of glutamate from the
cleft (Tong and Jahr, 1994 ; Asztely et al., 1997 ).
To investigate the temperature dependence of glial glutamate transport
in the hippocampus, we recorded synaptically evoked transporter
currents from astrocytes located in stratum radiatum of area CA1. The
persistence of these currents at physiological temperatures and the
lack of detectable transporter currents in pyramidal neurons suggest
that astrocyte transporters are primarily responsible for the uptake of
glutamate released from the terminals of Schaffer
collateral-commissural fibers in the hippocampus.
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MATERIALS AND METHODS |
Hippocampal slices were prepared from 12- to 15-d-old male
Sprague Dawley rats in accordance with a protocol approved by the Department of Animal Care at Oregon Health Sciences University. Rats
were anesthetized with halothane and decapitated, and the hippocampi
were removed and placed in ice-cold artificial CSF (ACSF) consisting of
(in mM): 119 NaCl, 2.5 KCl, 2.5 CaCl2,
1.3 MgCl2, 1 NaH2PO4,
26.2 NaHCO3, and 11 glucose, saturated with 95%
O2-5% CO2. Hippocampi were mounted in an agar
block, and 400-µm-thick slices were made by cutting the tissue
transversely using a Vibratome (TPI Instruments). Slices were allowed
to recover on a gauze net submerged in ACSF for 30 min at 34°C and at
room temperature thereafter.
Individual slices that had recovered for at least 1 hr were transferred
to a Lucite chamber with a coverslip bottom, where they were held
stationary with a "harp" made from 0.5 mm silver wire and single
nylon threads. Whole-cell recordings were made from astrocytes located
in the stratum radiatum region of area CA1, which were visualized using
an upright microscope (Axioskop; Zeiss) equipped with
infrared-Nomarski optics. Astrocytes were identified as described
previously (Bergles and Jahr, 1997 ), by their small size, high-resting
potentials, and low-input resistances. The internal solution for
whole-cell recordings of transporter currents contained (in
mM): 130 K-methanesulfonate, 20 HEPES, 10 EGTA, and 1 MgCl2, pH 7.2. To increase the likelihood of
detecting transporter currents in pyramidal neurons, K-thiocyanate
(KSCN) (130 mM) was substituted for
K-methanesulfonate in some recordings. SCN was not
used as the permeant anion in whole-cell recordings from astrocytes,
because it induced a holding current and caused them to visibly shrink
over time, affecting the stability of the recordings. Whole-cell
recordings of EPSCs were made from CA1 pyramidal neurons using an
internal solution composed of (in mM): 100 Cs-methanesulfonate, 20 TEA-Cl, 20 HEPES, 10 EGTA, 1 MgCl2, 4 ATP-Mg, and 0.3 GTP-Na, pH 7.2. Holding
potentials have been corrected for the different junction
potentials.
Evoked responses were elicited with a constant-current stimulator
(Winston Electronics) using bipolar stainless steel electrodes (tip
separation, 200 µm) placed in stratum radiatum >100 µm from the
cell. Stimulus parameters were 40-100 µA, 100 µsec for all experiments, except those testing for transporter currents in pyramidal
neurons in which the parameters were 100-200 µA, 200 µsec.
Whole-cell currents were amplified using an Axopatch 200A (Axon
Instruments), filtered at 1-5 kHz and sampled at 10-20 kHz. Series resistance was <10 M , and 80-90% compensation was used. Field electrodes had resistances of 1-3 M when filled with 3 M NaCl and were placed in stratum radiatum of area CA1.
Field EPSPs (fEPSPs) were recorded with an Axoclamp-2A (Axon
Instruments). Slope measurements were made from the initial rise
of the fEPSP using linear regression. To avoid contamination of the
rising phase of the fEPSP with the fiber volley at 36°C,
1,2,3,4-tetrahydro-6-nitro-2,3-dioxo-benzo[f]quinoxalie-7-sulfonamide (NBQX) (10 µM) and
3-(2-carboxypiperazin-4-yl)-propyl-l-phosphonic acid (CPP) (5 µM) were applied at the end of the experiment to allow
the stimulus artifact and fiber volley to be subtracted from the
synaptic response. A cut was made at the CA3-CA2 border when
picrotoxin and SR-95531 were included in the ACSF to reduce the
propagation of seizure discharges to area CA1. Stimulus artifacts have
been truncated for clarity.
Outside-out patches were removed from astrocytes and pyramidal neurons
located in area CA1. Rapid applications of solutions to these patches
were performed as described previously, using a four-barrel flow pipe
attached to a piezoelectric bimorph (Tong and Jahr, 1994 ). The junction
potential between the control and test solutions was used to monitor
the speed and duration of the solution application. The rise and decay
of these "open tip" responses occurred in <200 µsec (20-80%).
Nucleated patches were obtained by maintaining slight negative pressure
when pulling the electrode away from the cell. Patch recordings were
made with an internal solution containing (in mM): 130 KSCN, 20 HEPES, 10 EGTA, and 1 MgCl2, pH 7.2. Patch
currents were filtered at 5 kHz and sampled at 50 kHz.
The bath temperature was raised by allowing heated water to circulate
through a jacket surrounding a 5 inch length of the inflow tubing. The
temperature of the solutions applied to patches was maintained at the
bath temperature by raising the meniscus formed by the objective so
that the tips of the flow pipes were submerged by >5 mm. Temperature
changes were measured with a miniature thermistor probe
(TeleThermometer; YSI) placed in the center of the chamber
or in front of the flow pipes.
Half-decay measurements were made relative to steady state. For
measurements of peak amplitudes during paired-pulse experiments, a 30 msec control response was subtracted from the first three (L-glutamate) or all (D-aspartate) of the
paired responses before measuring the amplitude of the second response.
This adjusted for currents arising on the decay of the control
response.
Data are expressed as mean ± SD, and all comparisons
between 24°C and 36°C were significant at p < 0.01 (Student's paired t test), unless otherwise noted. When
percentages are listed, the mean values for the two temperatures are
also listed in parenthesis.
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RESULTS |
Temperature-dependent changes of transporter currents
in patches
In addition to the stoichiometrically defined movement of
Na+, K+, and
H+ that are coupled to glutamate translocation
(Zerangue and Kavanaugh, 1996 ), glutamate transporters exhibit a
permeability to anions that is uncoupled from glutamate flux (Fairman
et al., 1995 ). By including chaotropic anions, such as
SCN , in the patch pipette that are highly
permeable through these transporters (Kavanaugh et al., 1997 ), the
activity of the transporters can be monitored by recording the
glutamate-gated movement of SCN. These anion-potentiated transporter
currents are ~10-fold larger than currents mediated solely by the net
movement cations that accompanies transport (Bergles and Jahr, 1997 ),
allowing kinetic measurements of transporter activity to be made. To
measure the change in the intrinsic kinetics of astrocyte transporters, outside-out patches were removed from the somata of CA1 astrocytes, and
transporter currents activated in response to a saturating dose (10 mM) of L-glutamate were recorded first at room
temperature (22-24°C) and then at 36°C. Raising the temperature of
the solutions to 36°C caused marked changes in the transporter
current (Fig. 1A),
increasing the peak amplitude by 28.7 ± 19.7% (24°C, 39.5 pA; 36°C, 50.2 pA), decreasing the rise time (20-80%) by
21.5 ± 20.9% (24°C, 121.9 µsec; 36°C, 95.0 µsec), and
decreasing the decay from the peak (half-decay) by 50.6 ± 11.0%
(24°C, 1.04 msec; 36°C, 0.51 msec) (n = 30). The
change in rise time is likely to be an underestimate, limited by the
speed of solution exchange. A small increase in the steady-state
current was sometimes visible in these patches (8 of 30 patches);
however, the steady-state transporter current was small under these
conditions ( 6.5 ± 5.2 pA) (n = 30), which
decreased the precision of this measurement.

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Figure 1.
Temperature-dependent changes in astrocyte
transporter currents. A, Outside-out patch removed from
an astrocyte located in stratum radiatum of area CA1. Solid
lines in A and B are the control
responses recorded at room temperature, and dotted lines
are the responses of the same patch recorded at 36°C.
Inset, Response at 36°C has been scaled to that in
control and shown at a faster time base to illustrate the time course
of the two responses. B, Response of a different patch
to D-aspartate (10 mM). Traces
are illustrated as in A. Traces are
averages of 8-12 consecutive responses recorded at 90 mV. KSCN-based
internal solution. The open tip response above each
trace indicates the duration of the agonist
application.
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To gain a better estimate of this increase in steady-state current,
temperature-dependent changes in the response of patches to saturating
D-aspartate were also recorded. D-aspartate
elicits currents with a larger steady-state component (Fig.
1B) (Bergles and Jahr, 1997 ), consistent with the
greater steady-state anion flux per transport cycle observed for
D-aspartate than for L-glutamate (Wadiche et
al., 1995b ) and the higher affinity of D-aspartate for
EAAT1 and EAAT2 transporters (Arriza et al., 1994 ). The amplitude of
the steady-state current measured at the end of a 30 msec pulse of 10 mM D-aspartate increased by 11.1 ± 7.9%
(n = 9); however, this was not statistically
significant. Given the previously reported temperature dependence of
glutamate flux (Wadiche et al., 1995a ), an increase in temperature
should increase the steady-state current produced by the flux of
cations that are stoichiometrically coupled to transport because of the
increased cycling of the transporters. In these recordings, however,
~90% of the current is mediated by the uncoupled movement of anions
through the transporters (Bergles and Jahr, 1997 ). The lack of change
in the steady-state anion current suggests that the proportion of time
that transporters spend in the conducting state per transport cycle is
unchanged at 36°C.
The steady state/peak ratio for D-aspartate decreased from
0.42 ± 0.11 to 0.36 ± 0.10 (n = 9)
at 36°C, as a result of the larger increase in peak amplitude
(30.0 ± 11.9%; n = 9; 24°C, 23.9 pA; 36°C,
31.1 pA). A decrease in steady state/peak ratio was also observed for
L-glutamate (24°C, 0.16 ± 0.06; 36°C, 0.085 ± 0.03) (n = 30). The rise time, half-decay
time, and deactivation time (decay of the current from the end of the
glutamate pulse) also decreased with the jump in temperature for
responses elicited by D-aspartate (rise time, 24.5 ± 23.4%; 24°C, 133.3 µsec; 36°C, 91.1 µsec; half-decay time,
45.2 ± 5.7%; 24°C, 0.90 msec; 36°C, 0.50 msec; deactivation
time, 54.5 ± 10.7%; 24°C, 24.4 msec; 36°C, 11.03 msec)
(n = 9) (Fig. 1B).
The cycling rate of the glutamate transporter EAAT2 (GLT-1) has been
reported to exhibit a Q10 of 2.5-3 (Wadiche et
al., 1995a ). The turnover rate of astrocyte transporters in patches was
estimated by measuring the time necessary for the peak amplitude of the transporter current to recover from the steady-state level, by applying
paired applications of L-glutamate separated by different intervals. At room temperature, transporter currents recovered with a
time constant of 23.7 ± 1.0 msec (n = 4; single
exponential fit) (Fig.
2A,C).
This time constant of recovery decreased at 36°C to 11.6 ± 0.3 msec (n = 11) (Fig.
2B,C), a Q10
of >2, suggesting that the turnover rate of these native glial
transporters approaches ~100 sec 1, which is two
to three times faster than turnover rates estimated for EAAT2
transporters expressed in oocytes (Wadiche et al., 1995a ). The recovery
of transporter currents in patches in response to D-aspartate was slower than for L-glutamate
(Fig.
3A,C),
as expected from the lower equilibrium Imax
measured for D-aspartate in EAAT1- and EAAT2-expressing
oocytes (Arriza et al., 1994 ). Increasing the temperature decreased the
time constant of recovery from 35.0 ± 1.8 (n = 4)
to 16.5 ± 0.6 msec (n = 10) (Fig.
3B,C), similar to the approximately
twofold decrease observed for L-glutamate.

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Figure 2.
Recovery time course of
L-glutamate-evoked transporter currents. A,
B, L-glutamate (10 mM) was
applied for 30 msec to an outside-out patch from an astrocyte and then
reapplied for 20 msec after a variable delay, at both 24°C
(top traces) and 36°C (bottom traces).
Traces are averages of six consecutive responses
recorded at 90 mV. KSCN-based internal solution. C,
Summary plot of the ratio of the peak amplitude of the second pulse
(P2) over the peak amplitude of the control response
(P1) for recordings made at both 24°C
(n = 4) and 36°C (n = 11).
The four patches used to measure the recovery at 24°C were also used
to measure the recovery at 36°C.
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Figure 3.
Recovery time course of
D-aspartate-evoked transporter currents. A,
B, D-aspartate (10 mM) was
applied to an outside-out patch from astrocytes for 30 msec and then
reapplied for 20 msec after a variable delay, at both 24°C
(top traces) and 36°C (bottom traces).
Traces are averages of five consecutive responses
recorded at 90 mV. KSCN-based internal solution. C,
Summary plot of the ratio of the peak amplitude of the second pulse
(P2) over the peak amplitude of the control response
(P1) for recordings made at both 24°C
(n = 4) and 36°C (n = 10).
The four patches used to measure the recovery at 24°C were also used
to measure the recovery at 36°C.
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Temperature-dependent changes in synaptic transporter currents
To test whether glutamate transporters were activated in
astrocyte membranes at physiological temperatures, transporter
currents elicited via single (100 µsec) stimuli to the Schaffer
collateral-commissural projections in stratum radiatum were recorded
from astrocytes at room temperature and at 36°C. Ionotropic glutamate
receptors were blocked in these experiments with 10 µM
NBQX and 5 µM D,L-CPP. At room
temperature, transporter currents recorded under these conditions had a
rise time of 4.4 ± 0.8 msec and a half-decay time of 17.7 ± 1.8 msec (n = 14) (Fig.
4A). Raising the bath
temperature to 36°C decreased the latency of the response and
decreased the rise time (2.2 ± 0.4 msec) and half-decay time
(7.7 ± 0.8 msec) (n = 14) of the synaptic
transporter current (Fig. 4A). These results indicate
that at near physiological temperatures glutamate escapes from these
synaptic clefts and reaches transporters on glial membranes, suggesting
that the increased activity of neuronal transporters at this
temperature is not sufficient to sequester the released glutamate. The
rise and half-decay times of these currents decreased at the higher
temperature by 49.2 ± 8.3 and 56.5 ± 5.1%
(n = 14), respectively. The effect of raising the temperature on the peak amplitudes of these evoked currents was more
variable, but on average, they were increased by 35.9 ± 34.3% (24°C, 39.5 pA; 36°C, 53.8 pA) (n = 14). The
approximately twofold decrease in the rise and decay times of these
evoked transporter currents at 36°C is consistent with the faster
kinetics of the transporter currents observed in patches at this
temperature and suggests that the time course of the synaptic
transporter current cannot be accounted for by free diffusion of
glutamate to these sites, because free diffusion has a
Q10 of 1.2-1.3 (Hille, 1992 ). The total charge
transfer was less at 36°C, suggesting that less glutamate is
transported by the astrocyte. However, the slow tail of the response
also decreased (Fig. 4A), presumably reflecting an
increase in the rate of redistribution of extracellular potassium, making a quantitative comparison of the amount of glutamate transported under the two conditions problematic.

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Figure 4.
Temperature-dependent changes in evoked responses.
A, Synaptically activated transporter current
(STC) recorded from a stratum radiatum astrocyte.
Vm = 96 mV. K-methanesulfonate-based
internal solution. B, AMPA receptor-mediated EPSCs
recorded from a CA1 pyramidal neuron. Vm = 80 mV. Cs-methanesulfonate-based internal solution. C,
Field EPSPs (fEPSP) recorded in stratum radiatum
of area CA1. A-C, Solid lines are the
responses recorded at room temperature, and the dotted
lines are the responses recorded at 36°C.
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Increasing the bath temperature to 36°C produced similar changes in
AMPA receptor-mediated EPSCs in pyramidal neurons, decreasing the rise
time by 43.8 ± 12.2% (24°C, 1.54 msec; 36°C, 0.84 msec), decreasing the half-decay time by 45.9 ± 10.0% (24°C, 7.58 msec; 36°C, 4.03 msec), and increasing the peak by 55.27 ± 67.6% (24°C, 133.7 pA; 36°C, 194.4 pA) (n = 19). These temperature-dependent changes in EPSCs were reflected in the
73.3 ± 39.6% (24°C, 1.01 mV/msec; 36°C, 1.81 mV/msec)
(n = 16) increase in the slope of fEPSPs recorded in
stratum radiatum (Fig. 4C).
Transporter currents in CA1 pyramidal neurons
In situ hybridization and immunocytochemical studies
suggest that EAAC1 transporters are expressed in rat CA1 pyramidal
neurons during the second postnatal week (Shibata et al., 1996 ; Furuta et al., 1997 ). The human homolog of EAAC1, EAAT3 also exhibits a
permeability to anions (Wadiche et al., 1995b ), suggesting that glutamate-gated anion currents might be elicited in
SCN -loaded pyramidal neurons with synaptic
stimulation. However, when EPSCs elicited via Schaffer collateral
stimulation were blocked with antagonists of AMPA and NMDA receptors
(NBQX, GYKI-52466, and D,L-CPP), no remaining
evoked inward current was detected (n = 8) (Fig.
5). Because the turnover rates of
transporters are strongly dependent on temperature, single and paired
responses (50 msec interval) were also recorded at 36°C but similarly
failed to elicit transporter currents. It is possible that there were too few transporters activated with these synaptic stimuli to elicit a
detectable anion current, because the mean amplitude of the AMPA
receptor EPSCs recorded under these conditions was 274 pA
(Vm = 90 mV), much smaller than the
climbing fiber EPSCs associated with synaptic transporter currents in
Purkinje cells (Otis et al., 1997 ). However, large amplitude (>2 nA)
autaptic EPSCs elicited in microisland cultures of CA1 pyramidal
neurons also were not accompanied by detectable transporter currents
(J. S. Diamond and C. E. Jahr, unpublished
observations).

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Figure 5.
Transporter currents are not associated with EPSCs
in CA1 pyramidal neurons. The ionotropic glutamate receptor antagonists
NBQX (10 µM) and D,L-CPP (10 µM) completely blocked evoked responses, at both 24°C
and 36°C. The brief inward current observed in NBQX and CPP is
attributable to the increased amplitude and slower decay of the
stimulus artifact at 36°C. Vm = 90 mV.
ACSF contained picrotoxin (100 µM) and SR-95531 (5 µM). KSCN-based internal solution.
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Large outside-out patches from CA1 pyramidal cells were also used to
test for functional transporters in neuronal membranes. With
SCN (130 mM) in the pipette,
L-glutamate (10 mM) elicited large currents (Fig. 6A1),
which were blocked by the glutamate receptor antagonists NBQX,
GYKI-52466, and D,L-CPP (Fig.
6A2), demonstrating that they were mediated
by AMPA and NMDA receptors (n = 10). In the presence of
these antagonists, no inward current remained at either negative
(Vm = 90 mV) or positive
(Vm = 90 mV) potentials at room temperature
(Fig. 6A2) or at 36°C (n = 6), as would be expected if anion-permeable transporters were present.
Transporter currents were also not detected in six nucleated patches
from CA1 pyramidal cells that had L-glutamate-activated inward currents >1 nA (Vm = 60 mV) in the
absence of antagonists. It is unlikely that the lack of transporter
currents in these patches is caused by blockade by the glutamate
receptor antagonists, because these antagonists (at the same
concentrations) did not affect L-glutamate-gated
transporter currents in patches from astrocytes (n = 6)
(Fig. 6B1,B2), consistent with previously published results (Mennerick and Zorumski, 1994 ; Bergles and Jahr, 1997 ). These data also indicate that astrocytes in situ do not express ionotropic glutamate receptors in
their somatic membranes.

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Figure 6.
Transporter currents are not detected in pyramidal
cell patches. A, Outside-out patch from a CA1 pyramidal
neuron. L-glutamate (10 mM) activates inward
(Vm = 90 mV) and outward
(Vm = 90 mV) (A1)
currents that are completely blocked by NBQX (10 µM),
GYKI-52466 (25 µM), and D,L-CPP
(10 µM) (A2). B,
L-glutamate (10 mM) activates transporter
currents in outside-out patches from CA1 astrocytes
(B1), which were not affected by NBQX (10 µM), GYKI-52466 (25 µM), and
D,L-CPP (10 µM)
(B2). Responses were recorded at 90 mV and +90
mV, as in A. All solutions contained 20 µM
glycine. Traces are averages of 8-12 consecutive
responses. A KSCN-based internal solution was used for both
recordings.
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DISCUSSION |
Astrocytes in the mammalian CNS have highly branched processes
that come in close apposition to synaptic contacts (Spacek, 1985 ;
Kosaka and Hama, 1986 ), they express glutamate transporters at a high
density (Lehre et al., 1995 ; Furuta et al., 1997 ), and they have a high
capacity for glutamate uptake (Attwell et al., 1993 ). The two
transporters expressed in astrocytes, GLT-1 and GLAST, are critically
important for maintaining a low extracellular concentration of
glutamate (Rothstein et al., 1996 ; Tanaka et al., 1997 ). The current
generated by the electrogenic cycling of these transporters can be
detected in astrocytes after stimulation of Schaffer
collateral-commissural fibers in acute hippocampal slices (Bergles and
Jahr, 1997 ). We report here that at near physiological temperatures
these transporter currents persist, becoming faster and larger,
indicating that glutamate continues to diffuse out of these synaptic
clefts and reach glial membranes. Stimulation of Schaffer
collateral-commissural fibers did not elicit transporter currents in
CA1 pyramidal neurons, nor were they present in patches removed from
these cells, suggesting that glutamate transporters are expressed at a
very low density at this age in pyramidal neurons. Because there is no
direct evidence for the expression of glutamate transporters
presynaptically at these synapses (Rothstein et al., 1994 ; Furuta et
al., 1997 ; but see Taxt and Storm-Mathisen, 1984 ), these results
suggest that astroglial transporters are primarily responsible for the
uptake of glutamate released from Schaffer collateral-commissural
fibers.
Kinetics of astrocyte transporters at
physiological temperatures
Astrocyte transporter currents in patches had more rapid kinetics
at 36°C than at room temperature (22-24°C), activating, desynchronizing, and deactivating more rapidly, as would be expected for underlying conformational changes that require high-activation energies (Hille, 1992 ). The turnover or cycling rate of the
transporters was estimated by measuring the time necessary for the peak
of the anion current to recover from the steady-state level. The time
constant of this recovery was 23.7 ± 1.0 msec for
L-glutamate at room temperature and decreased to 11.6 ± 0.3 msec at 36°C. This rapid recovery suggests a physiological
turnover rate of 86 sec 1 for these endogenous
transporters, which is two to three times faster than that previously
measured for the cloned EAAT2 transporters expressed in oocytes (14.6 sec 1 at room temperature, with a reported
Q10 of 2.5-3) (Wadiche et al., 1995a ). The
estimate of turnover rate based on recovery of the anion conducting
state assumes that once glutamate binds the transporter it undergoes
translocation, with negligible unbinding occurring to the outside. An
alternative explanation for this rapid recovery is that some glutamate
unbinds before being transported, resulting in a lower transport
efficiency but a faster recovery of the anion conductance. Although
this efficiency may be temperature-dependent, it is unlikely to
entirely account for the faster recovery of the transporter current at
36°C, because transporters also cycle faster at higher temperatures
(Wadiche et al., 1995a ). The previous estimate of the turnover rate of
EAAT2 transporters was based on the steady-state accumulation of
radiolabeled L-glutamate (Wadiche et al., 1995a ), an assay
that does not provide information about the efficiency of transport.
Nevertheless, a model involving significant unbinding of glutamate to
the outside is consistent with a lower equilibrium flux rate and may
provide an explanation for the discrepancy between the two results.
Glutamate transporters in CA1 pyramidal neurons
Hippocampal pyramidal neurons in juvenile rats (postnatal days
14-16) express the EAAC1 glutamate transporter (Shibata et al., 1996 ;
Furuta et al., 1997 ). The human homolog of EAAC1, EAAT3 (Arriza et al.,
1994 ) exhibits a permeability to anions similar to other glutamate
transporters (Wadiche et al., 1995b ), and C6 glioma cells that express
only EAAC1 transporters (Palos et al., 1996 ) have anion permeable
glutamate transporters (M. P. Kavanaugh, personal
communication). The conductance of the EAAT3 transporter, relative to others in the family and based on the reversal potentials of the combined transport and anion current, suggests that the permeability of EAAT3 to anions is less than GLAST but greater than
GLT-1 (Wadiche et al., 1995b ). Although transporter currents were not
detected in pyramidal neurons after stimulation of Schaffer collateral-commissural fibers, the quantal content of these EPSCs was
small relative to those used to resolve transporter currents in
Purkinje neurons (Otis et al., 1997 ), raising the possibility that not
enough transporters were activated to be detected. Nevertheless, transporter currents also were not detected in pyramidal neurons in
microisland cultures after autaptic stimulation.
L-glutamate-gated transporter currents were also not
resolved in large outside-out patches from CA1 pyramidal neurons.
Anionic currents similar to those observed in astrocyte patches
(Bergles and Jahr, 1997 ) would be expected in pyramidal cell patches if neuronal transporters were (1) expressed at similar densities, (2) had
comparable anion permeabilities, and (3) were present in somatic
membranes. Because recent results indicate that EAAC1 is present in the
somatic membrane of pyramidal neurons at this developmental age (Furuta
et al., 1997 ), these results suggest that the combination of the lower
density and lower conductance of these transporters to anions accounts
for the inability to detect glutamate-activated transport currents in
CA1 pyramidal neurons. These results also suggest that GLT-1 (Mennerick
et al., 1998 ) or other as yet unidentified transporters that have an
associated anion permeability are not expressed at a high density in
CA1 pyramidal neurons at this age. Our results are consistent with the
phenotype of animals in which the expression of EAAC1 transporters has
been selectively reduced by transgenic means. Mice lacking EAAC1
transporters appear essentially normal, exhibiting no
neurodegeneration, no increased susceptibility to induced seizures, and
no increased mortality (Peghini et al., 1997 ). This phenotype contrasts
strongly with animals that lack GLT-1 expression. These transgenic
animals have spontaneous seizures, an increased susceptibility to
ischemic insults, and elevated glutamate levels in the extracellular
space (Tanaka et al., 1997 ), consistent with results obtained through treatment with antisense for GLT-1 (Rothstein et al., 1996 ). Although animals treated with antisense EAAC1 have a higher incidence of spontaneous seizures (Rothstein et al., 1996 ), this may be attributable to a breakdown in GABA metabolism rather than a consequence of reduced
uptake of glutamate by pyramidal neurons (Sepukty et al., 1997 ). These
results suggest that EAAC1 transporters are not critical for
maintaining a low ambient glutamate concentration.
Unlike the other glutamate transporters (GLT-1, GLAST, and EAAT4), the
expression of EAAC1 transporters is not restricted to the CNS (Pines et
al., 1992 ; Storck et al., 1992 ; Fairman et al., 1995 ), with substantial
EAAC1 found in peripheral tissues, including the heart, muscle, kidney,
and intestine (Kanai and Hediger, 1992 ; Mukainaka et al., 1995 ). This
wide distribution of EAAC1 transporters suggests that they may perform
more of a metabolic function, providing additional glutamate necessary
for the detoxification of ammonia and synthesis of proteins. This hypothesis is supported by the lack of colocalization of EAAC1 and
other synaptic markers (Coco et al., 1997 ).
Implications for synapse specificity in the hippocampus
Glutamate released at excitatory synapses in the CA1 region of the
hippocampus is not restricted to the synaptic space after release but
diffuses rapidly out the cleft and reaches nearby glial membranes
within a millisecond (Bergles and Jahr, 1997 ). The slow time course of
the transporter current recorded from astrocytes suggests that
glutamate may remain elevated for many milliseconds after release in
the extrasynaptic space, diffusing to transporters distant from the
cleft (Chaudhry et al., 1995 ). Neighboring synapses in this region of
the hippocampus are on average <0.5 µm apart (Rusakov and Kullmann,
1998 ), suggesting that high-affinity ionotropic NMDA and metabotropic
receptors may be activated and AMPA receptors desensitized by this
spillover of glutamate. Although a direct demonstration of glutamate
spillover in the hippocampus has been elusive, this phenomenon has been proposed to explain why NMDA receptors sense a larger number of quanta
than AMPA receptors, based on the lower amplitude variability of NMDA
receptor-mediated responses at these synapses (Asztely et al., 1997 ).
Diffusion of glutamate to adjacent sites could also explain why NMDA
receptor-only EPSCs are sometimes visible at low stimulus strengths
(for review, see Kullman and Asztely, 1998 ). If glutamate transporters
expressed by astrocytes are primarily responsible for the uptake of
glutamate released at these synapses, they may be an important
determinant in maintaining synapse specificity by restricting the
diffusion of glutamate to neighboring synapses, although barriers
to diffusion and additional binding sites may also play an important
role (Barbour and Hausser, 1997 ). The pivotal role of glial
transporters is suggested by a recent study showing that the
GLT-1-selective transporter antagonist dihydrokainate can increase
the incidence of spillover at Schaffer collateral-commissural synapses
at physiological temperatures; this conclusion was based on the ability
of dihydrokainate to increase the difference in the variance between
AMPA and NMDA receptor-mediated components of EPSCs in CA1 pyramidal
neurons (Asztely et al., 1997 ). The results presented here showing that
glutamate reaches astrocyte transporters at physiological temperatures,
but does not elicit detectable transporter currents in pyramidal cells,
suggests that astrocytes are primarily responsible for the uptake of
glutamate released from Schaffer collateral-commissural synapses.
 |
FOOTNOTES |
Received June 4, 1998; revised July 13, 1998; accepted July 21, 1998.
This work was supported by a grant from National Institutes of
Health.
Correspondence should be addressed to Dwight E. Bergles, Vollum
Institute, L474, Oregon Health Sciences University, Portland, Oregon
97201.
 |
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