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The Journal of Neuroscience, February 15, 1998, 18(4):1305-1317
The Synaptic Basis of GABAA,slow
Matthew I.
Banks1,
Tong-Bin
Li2, and
Robert A.
Pearce1, 2, 3
Departments of 1 Anesthesiology and
2 Anatomy, and 3 Neuroscience Training Program,
University of Wisconsin, Madison, Wisconsin 53706
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ABSTRACT |
Although two kinetically distinct evoked GABAA
responses (GABAA,fast and GABAA,slow)
have been observed in CA1 pyramidal neurons, studies of spontaneous
IPSCs (sIPSCs) in these neurons have reported only a single population
of events that resemble GABAA,fast in their rise and decay
kinetics. The absence of slow sIPSCs calls into question the synaptic
basis of GABAA,slow. We present evidence here that both
evoked responses are synaptic in origin, because two classes of
minimally evoked, spontaneous and miniature IPSCs exist that correspond
to GABAA,fast and GABAA,slow. Slow sIPSCs occur
infrequently, suggesting that the cells underlying these events have a
low spontaneous firing rate, unlike the cells giving rise to fast
sIPSCs. Like evoked GABAA,fast and
GABAA,slow, fast and slow sIPSCs are modulated
differentially by furosemide, a subtype-specific GABAA
antagonist. Furosemide blocks fast IPSCs by acting directly on the
postsynaptic receptors, because it reduces the amplitude of both
miniature IPSCs and the responses of excised patches to applied GABA.
Thus, in the hippocampus, parallel inhibitory circuits are composed of
separate populations of interneurons that contact anatomically
segregated and pharmacologically distinct postsynaptic receptors.
Key words:
hippocampus; GABAA receptors; furosemide; IPSC; voltage clamp; pyramidal cell
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INTRODUCTION |
Multiple kinetic classes of
inhibitory synaptic currents are observed in hippocampal neurons
(Pearce, 1993 ; Hajos and Mody, 1997 ; Ouardouz and Lacaille, 1997 ). In
CA1 pyramidal cells, spontaneous IPSCs (sIPSCs) and currents evoked by
stimulation of stratum pyramidale (GABAA,fast) have
rapid rising and decay kinetics. In contrast, GABAA
currents evoked by stimulating in distal dendritic layers (GABAA,slow) are slow to rise and decay (Pearce,
1993 ) and have time courses unlike any described sIPSCs in these cells
(Ropert et al., 1990 ; Mody et al., 1991 ). The time courses of these two IPSCs have important functional consequences (Kapur et al., 1997 ), but
the mechanisms underlying their different kinetics have not been
elucidated.
We have suggested that the kinetics of these evoked currents differ
because they are produced by receptors with different kinetic and
pharmacological properties. The most compelling evidence that the
receptors underlying GABAA,fast and GABAA,slow
are distinct is their differential sensitivity to furosemide (Pearce,
1993 ) and other agents (Banks and Pearce, 1996 ; Pearce, 1996 ) that
block GABAA,fast but have little effect on the amplitude of
GABAA,slow. It is unclear, however, whether these drugs act
directly on the postsynaptic receptors or by a presynaptic mechanism.
For example, although furosemide is a subtype-specific blocker of
GABAA receptors (Tia et al., 1996 ; Wafford et al., 1996 ),
it also blocks the
Na+/K+/Cl
cotransporter (Misgeld et al., 1986 ) and thereby could alter transmitter release. Demonstrating that the block of
GABAA,fast by furosemide is postsynaptic would be strong
evidence that the receptors underlying these currents are different,
although it would not exclude a contribution of transmitter time course
to the kinetics of the response.
An alternative to differences in receptor kinetics that might account
for the prolonged time course of GABAA,slow is an extended presence of neurotransmitter (Lambert et al., 1996 ). This situation could arise by several mechanisms. Synchronous release in response to
electrical stimulation could overwhelm the mechanisms for clearing GABA
from the cleft, leading to prolonged activation of synaptic receptors.
This mechanism is consistent with the absence of slow sIPSCs and
implies that GABAA,slow is not physiologically relevant. It
is also possible that synaptic specializations limit diffusion of
transmitter even in response to physiological stimuli, as occurs at
some glutamatergic synapses (Otis et al., 1996 ), or that
GABAA,slow arises because of slow diffusion of transmitter
to extrasynaptic receptors (Lambert et al., 1996 ).
To investigate these issues, we recorded minimally evoked, spontaneous
and miniature GABAA IPSCs (mIPSCs), as well as the responses of excised receptors, in CA1 neurons and tested their sensitivity to furosemide. We observed two populations of sIPSCs with
kinetics similar to those of evoked GABAA,fast and
GABAA,slow. Slow sIPSCs constitute <0.1% of events,
suggesting that they arise from interneurons with low intrinsic firing
rates. Fast sIPSCs, mIPSCs, and excised GABAA receptors are
blocked by furosemide, whereas the amplitudes of slow sIPSCs are
unaffected. Thus, we conclude that in hippocampus at least two
inhibitory circuits exist in which different interneuron populations
communicate with pyramidal cells via pharmacologically distinct
receptors.
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MATERIALS AND METHODS |
Slice preparation. Young rats (14-42 d old) were
decapitated under ether anesthesia, and the heads immediately were
immersed in cold (4°C) artificial CSF (ACSF) [composition (in
mM): NaCl 127, KH2PO4 1.21, KCl
1.87, NaHCO3 26, CaCl2 2.17, MgSO4
1.44, and glucose 10] saturated with 95% O2/5%
CO2. A block of tissue containing both hippocampi was
dissected out with the brain immersed in ACSF, and the tissue was glued
to a vibratome tray with cyanoacrylate glue. Slices (400 µm) were cut
in a plane ~15° off the frontal plane to allow for optimal
visualization of the cortical laminae. Slices were held submerged at
35°C for 1 hr before transfer to the recording chamber, which was
perfused at 3 ml/min with ACSF saturated with 95%
02/5%CO2.
Patch-clamp electrophysiology. Cells in stratum pyramidale
of CA1 were visualized with a video camera (Hamamatsu C2400, Hamamatsu City, Japan) connected to an upright microscope (Zeiss Axioskop, Oberkochen, Germany) equipped with an infrared bandpass filter (Chroma
D775/220), a long working-distance water-immersion objective (Zeiss
Achroplan 40×, 0.75 numerical aperture), and differential interference
contrast optics (Nomarski). Whole-cell recordings were obtained either
at 35°C or at room temperature (24°C), as indicated, using an
Axopatch 1D (Axon Instruments, Foster City, CA) patch-clamp amplifier.
All data were obtained by pClamp software (Axon Instruments). Data were
filtered at 5 kHz, sampled at 10-20 kHz (Digidata 1200), and stored on
a Pentium-based PC. Patch pipettes were fabricated from borosilicate
glass (Garner KG-33, 1.7 mm outer diameter, 1.1 mm inner diameter) with
a Flaming/Brown two-stage puller (model P-87), fire-polished, and
coated with SYLGARD to reduce electrode capacitance. Tight-seal
whole-cell recordings were obtained by standard techniques (Hamill et
al., 1981 ; Edwards et al., 1989 ). Patch pipettes had open tip
resistances of 2-4 M when filled with the recording solution
[composition (in mM): CsCl 140, NaCl 10, HEPES 10, EGTA 5, CaCl2 0.5, MgATP 2, and QX-314 5, pH 7.3]. Access
resistances were typically 10-20 M and then were compensated
60-80%. Cells were held at 60 mV. Evoked GABAA IPSCS,
sIPSCs, and mIPSCs were isolated by bath application of 20 µM CNQX and 40 µM D,L-APV to
block AMPA and NMDA-mediated currents and by the inclusion of CsCl and
QX-314 in the patch pipette to block GABAB-mediated
currents. Stimuli were applied to stratum pyramidale (SP) to evoke
GABAA,fast and stratum radiatum (SR) or stratum
lacunosum-moleculare (SL-M) to evoke GABAA,slow.
Bicuculline (10 mM) was applied focally under visual
control with a Picospritzer (General Valve, Fairfield, NJ) or was
bath-applied (10 µM).
Rapid agonist application. Excised outside-out patches were
obtained from the somata of CA1 pyramidal cells and exposed to brief
(2.6 ± 0.2 msec; see below) applications of GABA by using a
modified "liquid filament" technique (Franke et al., 1987 ;
Maconochie and Knight, 1989 ). Application pipettes were fabricated from
double-barreled "theta" glass tubing with a thin septum (Thin
Theta, Sutter Instruments, Novato, CA), pulled to a small diameter with
a Flaming/Brown two-stage puller (model P-87), and broken to a tip
diameter of 200-400 µm. Application pipettes were mounted to a
piezoelectric stacked translator (Physik Instrumente model P-245.50),
driven by a high-voltage proportional amplifier (Physik Instrumente
model P-270). Solution exchange rates (10-90% in <100 µsec) were
estimated by measuring open tip junction currents with dilute perfusion
solution at the conclusion of each experiment (Clements and Westbrook,
1991 ; Raman and Trussell, 1995 ). The duration of the agonist pulse was
defined by measuring the time between the points at 10% of the peak
amplitude of the junction potential.
Data analysis. Data were analyzed on a Pentium-based PC,
using ClampFit (Axon Instruments), Origin (MicroCal), and StatMost (DataMost). Spontaneous IPSC data were filtered off-line at 2 kHz.
Spontaneous events were analyzed by an automated event detection algorithm that measured IPSC amplitude, 10-90% rise times
(trise), and the time to 63% decay
(tdecay). Amplitude threshold was set as
3· noise, where noise was
measured during periods of no visually detectable events and was
typically <3 pA. This algorithm successfully detected >98% of
fast-rising sIPSCs and mIPSCs, but it consistently missed 20-40% of
the slow events. Thus, the data were also scanned manually, and any
missed slow events were analyzed and added to the event list. It is
possible that small slow events were overlooked consistently, and this
may contribute to the observed difference in mean amplitude between
fast and slow sIPSCs (see Fig. 7).
To characterize the decay kinetics of fast IPSCs and rise and decay
kinetics of slow IPSCs, we selected a subset of events for exponential
curve fitting as well ( rise and
decay). The decays of fast IPSCs typically were
described best by two exponential components. In those cases in which
we were unsure whether the fit was improved by adding a second
exponential component, the F test was used to compare the
variance of the residual currents after subtracting the mono- or
biexponential fit. A significance level of p < 0.01 was used. In some cases the multiexponential decay was characterized by
the weighted time constant dec,Wt = (A1 1 + A2 2)/(A1 + A2), where Ai is the
amplitude of the ith component. One possible source of bias
in analyzing the decay kinetics of slow sIPSCs should be noted. Only
those spontaneous events for which the tails did not contain subsequent
contaminating events of substantial amplitude [i.e., (amplitude of
contaminating event) < 0.2 · (amplitude of analyzed event)] were
selected for exponential fitting. Slow sIPSCs and mIPSCs were affected
much more by this restriction because of their extended tails, and thus
primarily the largest slow sIPSCs and mIPSCs were used for exponential
fitting. It is unclear, however, whether this could cause the
consistent kinetic differences observed between evoked and spontaneous
events (Table 1). Statistical comparisons were made
with paired t tests. All data are presented as mean ± SE.
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RESULTS |
Evoked responses
The original description of fast and slow evoked GABAA
currents in CA1 pyramidal neurons was made by using sharp
microelectrodes and discontinuous voltage clamp in brain slices
obtained from adult rats (Pearce, 1993 ). For this study we chose to use
whole-cell recording techniques in slices from juvenile rats, because
these recordings offered superior noise characteristics and stability and allowed us to record minimally evoked and mIPSCs. Monosynaptic GABAergic IPSCs were elicited with bipolar glass electrodes (made from
theta glass) placed in SP and either SR or SL-M (Fig.
1). Evoked GABAA,fast and
GABAA,slow IPSCs had time courses at 35°C and 60 mV,
comparable to those recorded from adult animals by using sharp
microelectrodes (Table 1) (Pearce, 1993 ). We found that by using these
glass stimulating electrodes under direct visual control, we more
reliably could evoke currents that were "pure"
GABAA,slow or GABAA,fast than was possible with
tungsten electrodes used in previous studies. In particular, we were
able to discern that in most cells (25 of 33) the decay of evoked
GABAA,fast was composed of two decay phases of ~3.5 and
14 msec (Fig. 2, Table 1).
GABAA,slow was best fit by the sum of single rising and
falling exponential components (Table 1).

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Figure 1.
Selective stimuli elicit GABAA,fast
and GABAA,slow. Photomicrograph (right
column) of a CA1 pyramidal cell in a 400 µm slice taken from
a 29-d-old rat and the monosynaptic GABAA IPSCs recorded in
this cell at 35°C that were evoked by stimuli in stratum pyramidale and stratum radiatum (left column). Five superimposed
traces are shown for each stimulus location. The recording electrode
can be seen entering the field of view from the top right and
contacting the cell body. The apical dendrite of this cell is marked by
the arrowheads. A stimulating electrode placed in
stratum pyramidale just apical to the cell body evoked
GABAA,fast (left column, top traces), which
had kinetics and amplitude similar to spontaneous events recorded in
this cell. A second stimulating electrode placed next to the dendrite
in stratum radiatum evoked GABAA,slow (bottom left), the kinetics of which were clearly distinct from the
overlying spontaneous IPSCs. Stimulus artifacts were removed off-line
for clarity. Scale bar, 20 µm.
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Figure 2.
Fast IPSCs decay with biexponential kinetics.
Shown are average SP-evoked (A) and spontaneous
(B) IPSCs recorded in the same cell at 35°C.
Both monoexponential (dashed lines) and biexponential fits (solid lines) are superimposed on the data.
Insets show the data on an expanded time scale. Fit
parameters are included. SP-evoked IPSC: biexponential fit,
dec1,2 = 3.6 msec (63%) and 11.3 msec; monoexponential
fit, dec = 6.5 msec. Fast sIPSC: biexponential fit,
dec1,2 = 4.5 msec (71%) and 13.6 msec; monoexponential
fit, decay = 7.5 msec. In both cases the second decay
component significantly improved the fit (p < 0.01, using the F test).
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We also investigated the temperature dependence of the kinetics of
GABAA,fast and GABAA,slow, both because
recordings at room temperature are more stable than those obtained at
elevated temperature and because we wanted to facilitate comparison
with several previous studies of IPSC kinetics that also were done at
room temperature (Collingridge et al., 1984 ; Edwards et al., 1990 ;
Ropert et al., 1990 ; Otis and Mody, 1992 ; De Koninck and Mody, 1994 ).
At 24°C, evoked GABAA,fast had rise times that were
~1.8-fold slower and decay times that were approximately threefold
slower than at 35°C (Table 1). The kinetics of GABAA,slow
exhibited less temperature sensitivity than those of
GABAA,fast, with the rise time prolonged by
<1.5-fold at 24°C and the decay time by approximately twofold (Table
1). The rise time of GABAA,slow is difficult to interpret, because it may be distorted by dendritic filtering. The slow decay phase of GABAA,slow is not distorted substantially by
dendritic filtering (Pearce, 1993 ), and its temperature sensitivity
argues against the decay being determined by diffusion of transmitter away from the receptors (Hille, 1992 ).
Minimal stimulus-evoked responses
Because both fast and slow evoked responses could be observed in
low-noise patch recordings by using small glass stimulating pipettes,
we used these techniques to test for responses to stimulation of single
presynaptic fibers, using minimal stimuli. For these experiments,
recordings were obtained under direct vision from pyramidal neurons,
the dendrites of which could be visualized extending into stratum
radiatum. Patch stimulating electrodes were placed either at the level
of the cell body or of the dendrite and were repositioned as necessary
to obtain a selective fast or slow response, with as low a stimulus
intensity as possible. Stimulus intensity was raised slowly, and
multiple responses were obtained at each level. Both fast
(n = 7 cells) and slow (n = 5 cells)
all-or-none evoked responses could be obtained by this method (Fig.
3). The kinetics of these IPSCs were not
significantly different from nonminimally evoked IPSCs observed in
these cells (see Fig. 3 legend), and the two groups are pooled in Table
1. These data suggest that both GABAA,fast and
GABAA,slow can arise from neurotransmitter release
triggered by activity in individual presynaptic fibers.

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Figure 3.
Minimally evoked GABAA,fast and
GABAA,slow IPSCs. Shown are GABAA IPSCs
recorded at 35°C in the same cell in response to stimuli in stratum
pyramidale (A, a) and stratum
lacunosum-moleculare (B, a). In both cases, small
increases in stimulus intensity elicited all-or-none responses
(A, b; B, b). Note the difference in
amplitude scale in A, a versus B, a. The
kinetic parameters for exponential fits to the average minimally evoked
IPSCs in this cell were SP, dec1,2 = 2.72 msec (25%) and 11.7 msec; SL-M eIPSC,
rise = 5.50 msec and decay = 43.0 msec.
For SP minimally evoked IPSCs, the average fit
parameters in seven cells were dec1,2 = 3.37 ± 0.53 msec (38 ± 7%) and 13.0 ± 0.9 msec. For
SL-M, average parameters in five cells were
rise = 5.15 ± 0.26 msec and decay = 53.8 ± 8.4 msec.
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Two populations of spontaneous IPSCs in pyramidal cells
If GABAA,fast and GABAA,slow are synaptic
currents that result from transmitter release at two different sets of
synapses, then one would expect to see two populations of sIPSCs and
mIPSCs in pyramidal cells corresponding to the two evoked currents. In contrast to previous descriptions of a homogeneous population of
rapidly rising and decaying sIPSCs and mIPSCs, we occasionally observed
slowly rising and decaying events (Fig.
4). These slow events represent a
population of IPSCs with kinetic properties distinct from the more
commonly observed fast events. Figure
5A shows a scatterplot of
decay versus rise time for sIPSCs recorded 30 sec before and 30 sec
after one of the slow events shown in Figure 4A
(trace b; this was the only slow sIPSC observed in this cell). This slow event appears as a lone outlier point in this graph,
clearly separated from the other 320 rapidly rising and decaying
sIPSCs. Even more striking is the similarity in time course of the
average fast sIPSCs and the evoked GABAA,fast and of this
slow sIPSC and the evoked GABAA,slow (Fig. 5A,
open squares; 5B).

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Figure 4.
Kinetic heterogeneity of spontaneous and miniature
IPSCs. Shown are sIPSCs (A) and mIPSCs
(B) recorded at 35°C in five different cells.
sIPSCs with slow kinetics are marked by asterisks.
Calibration: 100 msec, 200 pA.
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Figure 5.
Evoked and spontaneous IPSCs have similar
kinetics. A, Scatterplot of
tdecay versus
trise for 321 sIPSCs (open
circles) recorded in a cell at 35°C. The single slow sIPSC is
the same event that is shown in Figure 4A
(second trace). The other 320 sIPSCs were recorded 30 sec before and 30 sec after this event. Also shown are the kinetic
parameters for the IPSCs evoked by SP and SL-M stimulation (open
squares) shown in B. B, Averaged
and normalized fast sIPSC, SP-evoked IPSC, slow sIPSC, and SL-M-evoked
IPSC recorded in the same cell as in A. Fit parameters
include the following: fast sIPSC, trise = 0.4 msec and dec1,2 = 3.5 msec (56%) and 13.7 msec;
SP-evoked IPSC, trise = 0.8 msec and
dec1,2 = 3.9 msec (62%) and 18.5 msec; slow sIPSC,
rise = 7.2 msec and decay = 52.2 msec;
SL-M-evoked IPSC, rise = 6.0 msec and
decay = 53.9 msec.
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Because slow sIPSCs and mIPSCs occurred relatively infrequently, it was
necessary to combine data from several cells to determine whether fast
and slow sIPSCs are truly distinct populations of events or merely the
two extremes of a kinetic continuum. Figure 6 shows the rise and fall kinetics for
>5000 sIPSCs pooled across six different cells studied at 35°C,
which were chosen for their high rates of slow sIPSCs. The histograms
of trise and tdecay show
that, when each kinetic parameter is considered independently, it is
not possible to separate out two populations of sIPSCs. However, two
populations do emerge in scatterplots of tdecay
versus trise. The vast majority of the sIPSCs
(>98%) falls in the area of the graph defined by
trise < 2.5 msec and
tdecay < 20 msec, but a second group of more
slowly rising and falling events (n 100) is also
apparent in the top right corner of the graph. In four additional cells
studied in detail at 24°C, the two populations of sIPSCs separated at
trise ~6 msec and
tdecay ~40 msec (data not shown).

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Figure 6.
Two kinetic classes of sIPSCs. A scatterplot of
tdecay versus
trise is shown for >5000 sIPSCs recorded at
35°C in six different cells with high rates of slow sIPSCs. Most of
the sIPSCs had rapid rise and fall kinetics and are clustered in the
lower left quadrant of the plot (see histograms at
left and bottom left). Approximately 2%
of the events had tdecay > 20 msec and
trise > 2.5 msec. Within these two groups
there was little correlation between tdecay
and trise (fast,
r2 = 0.0265; slow,
r2 = 0.137). Scale bars:
tdecay histogram, 100 counts;
trise histogram, 250 counts.
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Fast and slow mIPSCs and sIPSCs had kinetics similar to those of the
evoked GABAA,fast and GABAA,slow, and
this was true both at 35°C and at 24°C (Table 1). On average, fast
mIPSCs and sIPSCs were faster to rise than the evoked fast IPSC,
possibly because of a shorter transmitter transient during the mIPSC,
e.g., caused by asynchrony of release during the evoked response. It is
also apparent that the slow sIPSCs were slower to rise and faster to decay than the evoked GABAA,slow, especially at
24°C. It is possible that, when we stimulated in stratum
lacunosum-moleculare, we activated a subset of the synapses giving rise
to slow sIPSCs that has faster rising kinetics. It is still clear,
however, that fast and slow IPSCs have distinct kinetics.
Slow sIPSCs and mIPSCs frequently appeared larger in amplitude than the
majority of fast events (see Fig. 4). Quantifying this observation
required large numbers of fast and slow events. It was much easier to
categorize events on the basis of rise times alone, because the decay
phases of slow events often were contaminated with fast events and thus
were difficult to analyze. We recorded >30,000 events in six cells at
35°C and constructed amplitude histograms for the fastest rising
events (trise 1 msec) and the slowest rising
events (trise 4 msec; Fig.
7). We found that the slowest events were
significantly larger than the fastest events [69.5 ± 4.8 vs
57.4 ± 0.5 pA; p < 0.01, using the
Kolmogorov-Smirnov (K-S) test; n = 262 and 22888 events, respectively; both groups were significantly larger than the
population as a whole (53.1 ± 0.4 pA; p < 0.01, using the K-S test; n = 30,520 events)]. Part or all
of this difference may have been attributable to detection bias,
because it was more difficult to detect slowly rising, small-amplitude events.

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Figure 7.
Amplitude distributions of fast- and slow-rising
sIPSCs. Shown are cumulative amplitude distributions for the fastest
rising (trise 1 msec; dashed
line) and slowest rising (trise 4 msec; dotted line) sIPSCs of >30,000 sIPSCs recorded at
35°C in six cells. The distribution for the entire population of
sIPSCs (solid line) is plotted for reference. Also shown
are amplitude histograms for the fast-rising (top inset, open
bars) and slow-rising (bottom inset, filled
bars) sIPSCs. The histogram for the entire population appears
as a solid line in both insets.
Histograms were normalized so that their total area = 1.
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As mentioned above, slow sIPSCs and mIPSCs occurred much less
frequently than did fast sIPSCs and mIPSCs. We measured the rates of
action potential (AP)-dependent and AP-independent inhibitory events by
subtracting the event rate in TTX from that in control solution. We
found that both rates were four orders of magnitude higher for fast
events than for slow events (AP-dependent, 17.2 ± 7.2/sec vs
5.4 × 10 3 ± 2.2 × 10 3/sec; AP independent, 14.2 ± 2.1/sec vs
4.3 × 10 3 ± 2.5 × 10 3/sec; n = 7 cells; all
recordings at 35°C). The difference in AP-dependent spontaneous rates
is consistent with fast and slow sIPSCs arising from two different
groups of interneurons. Also, the occurrence of slow mIPSCs argues
against a role for presynaptic firing properties (e.g., bursting in
interneurons) in setting the time course of GABAA,slow.
Fast sIPSCs arise somatically
In a previous study it was shown that fast and slow evoked IPSCs
arise from synapses that are segregated anatomically (Pearce, 1993 ).
Using focal applications of bicuculline applied under direct visual
control, we tried to ascertain whether the two populations of sIPSCs
also arise from anatomically segregated synapses. Although the low rate
of occurrence of slow sIPSCs precluded our using this technique to
determine the location of synapses giving rise to this population of
sIPSCs, we found that the majority of fast sIPSCs arises from terminals
on or near the soma (Fig. 8). A short bicuculline puff (10 mM at 20 psi for 10 msec) at the cell
body transiently reduced the peak amplitude of the fast sIPSCs by 56% (control, 57.0 ± 1.6 pA; bicuculline, 25.1 ± 2.0 pA),
whereas the same puff at 55 µm from the cell body caused a 46%
reduction (30.7 ± 1.5 pA), at 110 µm caused a 28% reduction
(41.3 ± 2.5), and at 220 µm reduced the amplitude by <3%
(55.4 ± 3.3 pA) (Fig. 8B). Because of leakage
from the puffer pipette, the baseline sIPSC amplitude also was reduced
in a spatially restricted manner, similar to the effect on sIPSCs
immediately after the puff (Fig. 8B). Similar results
were obtained in four other cells. In all cases, maximal block of
sIPSCs occurred at the cell body, and at >200 µm the sIPSCs were
blocked by <5%.

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Figure 8.
Fast sIPSCs arise close to the soma.
A, Composite photomicrograph (left) of a
CA1 pyramidal cell showing the four positions at which bicuculline was
puffed onto the cell body or apical dendrite (marked by
arrowheads). The recording pipette can be seen entering the field of view from the right. Sample traces are
illustrated for each puffer pipette position (right
column). The time of the puff is indicated by the
arrowhead; recording was at 35°C. Calibration: 2 sec,
100 pA. B, Summary data for the cell illustrated in
A. Shown are sIPSC amplitudes without the puffer pipette
near the cell (Ctrl) and averaged 2 sec after the
bicuculline puff at four positions relative to the cell (black
bars). Because of leakage from the puffer pipette, the baseline
sIPSC amplitude was reduced in a spatially restricted manner
(striped bars) also, similar to the effect on sIPSCs
immediately after the puff.
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The lack of effect after dendritic application of bicuculline does not
necessarily indicate that no fast inhibitory synapses are located in
the dendrites because, compared with the soma, a relatively smaller
membrane area will be affected by a focal application. However, these
results do establish that the spatial resolution of the technique is at
least ~100 µm. The finding that the mean amplitude of sIPSCs was
reduced by 56% after somatic application of bicuculline thus
establishes a lower limit for the spatial restriction of fast synapses,
i.e., 44% of fast synapses are remote from the soma. If the
concentration of bicuculline achieved by puff application was
sufficient to block somatic IPSCs only partially, then the percentage
of remote synapses is <44%. These data are further evidence that fast
sIPSCs correspond to GABAA,fast and that the interneurons
giving rise to kinetically distinct IPSCs have distinct projection
patterns.
Furosemide selectively modulates fast and slow sIPSCs
The data presented above show that two classes of synapses give
rise to GABAA,fast and GABAA,slow and strongly
suggest that these synapses arise from distinct groups of interneurons.
We will now present evidence that the receptors at these two classes of
synapses have distinct pharmacological properties.
Furosemide is a subtype-specific antagonist of GABAA
receptors (Tia et al., 1996 ; Wafford et al., 1996 ) that was shown
previously to reduce the amplitude of evoked GABAA,fast
(80% at 0.6 mM), with little effect on the amplitude of
GABAA,slow (Pearce, 1993 ). We found that the fast and slow
sIPSCs similarly exhibit a differential sensitivity to furosemide (Fig.
9). Furosemide (0.6 mM)
reduced the amplitude of the fast sIPSCs without affecting the
amplitude of the slow sIPSCs, whereas bicuculline (10 µM)
completely blocked both populations of sIPSCs (Fig. 9A; data
were recorded at 24°C).

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Figure 9.
Furosemide selectively blocks fast sIPSCs.
A, sIPSCs recorded from a cell at 24°C in control
solution (a), 0.6 mM furosemide (b), and 0.6 mM furosemide plus 10 µM bicuculline (c). The effect of
bicuculline was reversible for both the fast and slow events. Traces
are consecutive within each panel. Slow sIPSCs are indicated with
asterisks. Calibration: 200 msec, 200 pA.
B, Cumulative amplitude distributions for fast-rising
sIPSCs (left) and slow-rising sIPSCs (right) in control solution (dashed
lines) and 0.6 mM furosemide (solid
lines). Insets show raw amplitude histograms,
normalized by their area.
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To quantify the blocking effect of furosemide, we compared the
amplitude distributions of the two classes of spontaneous IPSCs with
and without the drug. Because the rising phases of slow sIPSCs are much
less likely to be contaminated by fast sIPSCs than are the decay
phases, it is easier to discriminate unambiguously between individual
fast and slow events by classifying sIPSCs on the basis of rise time
alone. However, as noted above (see Fig. 6), there was significant
overlap in rise times between the two populations. We chose, therefore,
to compare the fastest rising of the fast sIPSCs and the slowest of the
slow sIPSCs. In the cell illustrated in Figure 9, furosemide blocked
the fastest sIPSCs (trise < 2 msec) by 53%,
with no effect on the slowest sIPSCs (trise > 10 msec; Fig. 9B). In five cells, 0.6 mM
furosemide blocked the fast sIPSCs by 48.5 ± 9.1%, with no
consistent effect on the amplitude of the slowest sIPSCs (+4.65 ± 17.06%; control, n = 75 events; furosemide,
n = 124 events). Furosemide also appeared to slow the
kinetics of both populations of sIPSCs. For example, in this cell,
furosemide increased the average rise time of the slow sIPSCs by >40%
(control, 5 msec; furosemide, 7.2 msec) and nearly doubled the decay
time (control, 95 msec; furosemide, 172 msec). Similar effects were
observed in the other four cells. The effect of furosemide on the
kinetics of fast sIPSCs was variable, possibly because of a presynaptic
component to the effect (see below).
Furosemide blocks fast mIPSCs
To evaluate the relative contributions of presynaptic and
postsynaptic actions of furosemide on fast sIPSCs, and presumably also
on evoked GABAA,fast current, we tested its effect on fast mIPSCs. If we assume that mIPSCs recorded in the presence of TTX are
the responses to single quanta of neurotransmitter, presynaptic drug
effects would be manifested only in changes in mIPSC frequency, whereas
postsynaptic drug effects would be manifested in changes in mIPSC
amplitude [Katz (1962) ; but see Vautrin and Barker (1994) ]. In seven
cells we found that, in the presence of TTX, furosemide (0.6 mM) reduced mIPSC amplitude by 36.9 ± 4.1% (Fig.
10) while reducing mIPSC frequency by
12.9 ± 5.7%. Unlike the case for fast sIPSCs, furosemide
consistently slowed the decay of fast mIPSCs. However, when we
attempted to quantify these results, we found that the particular fit
parameter that was affected was variable. The results were much more
consistent with the weighted decay time constant
( dec,Wt; see Materials and Methods).
dec,Wt increased from 8.30 ± 0.89 msec in control
to 12.9 ± 1.4 msec in furosemide (n = 5;
p < 0.05). Furosemide had no effect on the rise time
of fast mIPSCs (control, 0.44 ± 0.12 msec; furosemide, 0.43 ± 0.01 msec). The mIPSC rates in the other two cells were too high to analyze the rise and decay kinetics reliably. (The low frequency of
slow mIPSCs precluded an analysis of furosemide effects on these
events. It seems unlikely, however, that slow mIPSCs would be blocked
when slow sIPSCs were not.)

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Figure 10.
Furosemide blocks miniature IPSCs. Shown is a
time series plot of normalized mIPSC amplitude
(A) and cumulative amplitude distribution
(B) for a cell exposed to 0.6 mM
furosemide in the presence of 1 µM TTX.
Insets show raw amplitude histograms, normalized by
their area. Furosemide reduced mIPSC amplitude, with a small effect on
mIPSC frequency (data not shown). Recording was at 35°C.
|
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The discrepancy in blocking potency between evoked and miniature IPSCs
and the small reduction in mIPSC frequency suggest that furosemide
reduces presynaptic release probability. More important to the issue at
hand, however, is that furosemide appears to have a potent postsynaptic
effect, as well. This suggests that the receptors underlying
GABAA,fast and GABAA,slow have different pharmacological properties and thus are likely to be structurally distinct, differing, for example, in their subunit composition.
Furosemide blocks the responses of excised
GABAA receptors
To confirm that furosemide was acting directly on the postsynaptic
receptors, we investigated its effect on GABAA receptors excised from the somata of pyramidal cells. We tested the responses of
excised receptors in outside-out patches to brief pulses (2.6 ± 0.2 msec) of 1 mM GABA to simulate synaptic transmitter
transients. All of these recordings were performed at 24°C and 60
mV. Currents in response to these applications of agonist were
qualitatively similar to fast IPSCs, with rapid rates of rise
(t10-90% = 1.3 ± 0.1 msec) and
biexponential decays [23.4 ± 2.1 msec (57 ± 3%) and
107 ± 6 msec; n = 21]. As in other preparations,
the excised responses were consistently slower to decay than the fast IPSCs (Puia et al., 1994 ; Galarreta and Hestrin, 1997 ).
Application of 0.6 mM furosemide reduced the peak response
to brief pulses of GABA by 47.0 ± 5.8% (n = 6;
Fig. 11A,B), an
effect slightly larger than its effect on mIPSCs recorded in these
cells (Fig. 10). Although we did not investigate the mechanism of block in detail, two observations suggest that furosemide may be acting as an
open-channel blocker: there was an increase in channel flicker (Fig.
11C) and a decrease in deactivation rate (Fig.
11A) in the presence of furosemide. We quantified the
latter effect by comparing the weighted time constant
( dec,Wt) in the presence and absence of
furosemide (as was the case for mIPSCs, the effects on the individual
fit parameters were variable). Furosemide prolonged dec,Wt from 44.9 ± 8.9 to 79.0 ± 10.9 msec
(p < 0.005), a slightly larger effect than was
the case for mIPSCs. The rise times of the responses also were slowed
by furosemide (control, 1.41 ± 0.36 msec; furosemide, 2.02 ± 0.33 msec; p < 0.05). Further elucidation of the
mechanism of block awaits a more complete analysis, but these data
confirm that part of the blocking effect of furosemide is attributable
to an interaction with the postsynaptic receptors.

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Figure 11.
Furosemide blocks excised patch responses.
A, Responses recorded from an outside-out patch excised
from the cell body of a CA1 pyramidal cell in response to 1 mM GABA in the absence and presence of furosemide (0.6 mM). Asterisks in a and
b refer to the data in C. Calibration:
100 msec, 25 pA. Inset, 1 msec. B, Time
series plot of the peak responses for the experiment in
A. Furosemide rapidly and reversibly blocked the
response by 48%. The dotted line is an exponential fit
to the baseline to compute accurately the percentage of block in the
presence of rundown. a, b, and c refer to
the traces in A. C, Data
from the tails of the responses in B are replotted on an
expanded scale to show single channel behavior. Calibration: 10 msec, 2 pA.
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|
 |
DISCUSSION |
We have presented evidence that the two types of
GABAA-mediated inhibitory responses observed in hippocampal
CA1 pyramidal neurons, GABAA,fast and
GABAA,slow, are both synaptic in origin. Our data
suggest further that the synaptic terminals generating these responses
arise from distinct pools of interneurons that differ in their
spontaneous firing rates and that these synapses incorporate
structurally distinct postsynaptic receptors.
GABAA,slow is a synaptic current
Several results from previous studies have called into question
the synaptic basis of the slow evoked GABAA current.
Primary among these was a failure to observe corresponding populations of slow miniature and spontaneous IPSCs. In addition, relatively large
stimuli were required to evoke slow responses (Pearce, 1993 ), and GABA
uptake inhibitors enhanced the slow component of a mixed (biexponential) IPSC in CA1 neurons (Roepstorff and Lambert, 1994 ). These results suggested that the slow evoked IPSC might be an artifact
of gross electrical stimulation, for example, attributable to
transmitter spillover from the synaptic cleft to extrasynaptic receptors as a consequence of the synchronous activation of large numbers of presynaptic fibers.
In our recordings from CA1 neurons we observed minimally evoked
GABAA,fast and GABAA,slow responses (see Fig.
3), as well as two kinetically distinct populations of spontaneous and
miniature IPSCs (see Fig. 6). The two populations of spontaneous events have kinetic (see Fig. 5, Table 1), anatomical (see Fig. 8), and
pharmacological (see Figs. 9, 10) properties strikingly similar to the
evoked GABAA,fast and GABAA,slow currents.
These observations indicate that both GABAA,fast and
GABAA,slow are synaptic in origin and that the evoked
currents accurately reflect the responses of the postsynaptic neurons
to physiologically appropriate stimuli.
The reason that previous studies of spontaneous and miniature IPSCs in
the hippocampus have reported only a single homogenous population of
fast-rising, fast-decaying events (Collingridge et al., 1984 ; Edwards
et al., 1990 ; Mody et al., 1991 ; Otis and Mody, 1992 ; De Koninck and
Mody, 1994 ) is very likely the extremely low rate of occurrence of the
slow events, even at near-physiological temperatures. Also, both rise
and decay kinetics must be examined to distinguish the second
population of events, because analyses that are based on one kinetic
parameter alone yield single, continuous populations of events (see
Fig. 6). Furthermore, some studies deliberately excluded slowly rising
events from analysis to operate on a homogenous population (De Koninck
and Mody, 1994 ).
Different interneuron types generate fast and slow IPSCs
Several observations indicate that the fast and slow
GABAA responses arise from distinct pools of interneurons.
First, GABAA,fast and GABAA,slow responses,
including "minimal" or all-or-none responses, can be evoked
selectively by electrical stimuli applied to different locations (see
Figs. 1, 3). Also, the synapses that produce the currents are
segregated spatially (see Fig. 8) (Pearce, 1993 ). Although these
observations alone do not preclude the possibility that multiple axonal
projections of a single interneuron type produce both responses,
anatomical studies have revealed several classes of interneurons that
are distinguished by their cell body locations and lamina-specific
axonal projections (Freund and Buzsáki, 1996 ). Furthermore,
stimulating single interneurons in stratum lacunosum-moleculare elicits
IPSCs with slower rise and decay kinetics than those evoked by
stimulating single cells in stratum pyramidale or oriens (Ouardouz and
Lacaille, 1997 ). Thus, it is reasonable to expect that the anatomically
segregated responses are produced by different interneuron classes.
The spontaneous rates for the fast and slow events differed by four
orders of magnitude, consistent with the synapses arising from two
groups of interneurons with different spontaneous firing rates. It is
also possible that the difference in IPSC rates arises because of
differences in numbers of synapses or because selective electrotonic
filtering of the slow events reduced their measured amplitudes below
noise level. However, we found that the maximum evoked amplitudes of
GABAA,fast and GABAA,slow differed by <10-fold (data not shown), implying that selective dendritic filtering or
differences in the numbers of synapses cannot account for the difference in rates. In addition, the total number of inhibitory synapses contacting any one pyramidal cell is probably in the hundreds
(Gottlieb and Cowan, 1972 ; Buhl et al., 1994a ), so it is not physically
possible for there to be 104 more synapses
underlying fast IPSCs than slow IPSCs.
The spatial restrictions of the axonal projections and the level of
spontaneous firing activity of different classes of interneurons provide some clues to the identity of the cells underlying
GABAA,fast and GABAA,slow. Basket cells are the
most likely candidates to underlie GABAA,fast,
because they project to stratum pyramidale and proximal stratum
radiatum exclusively (Lorente de No, 1934 ; Gulyas et al., 1993 ; Buhl et
al., 1994a ,b ; Sik et al., 1995 ). Axo-axonic, bistratified, and
horizontal trilaminar cells also project to somatic and perisomatic
regions and thus also may contribute to GABAA,fast. All of
these cell types have been reported to exhibit spontaneous firing
activity (Schwartzkroin and Mathers, 1978 ; Ashwood et al., 1984 ;
Lacaille et al., 1987 ; Buhl et al., 1994a ,b , 1996 ). Interneurons in
stratum lacunosum-moleculare are likely to underlie
GABAA,slow, because they project to dendritic
regions exclusively and exhibit no spontaneous activity (Williams et
al., 1994 ). Consistent with this, stimulation of single SL-M
interneurons in the slice elicits slowly rising and decaying unitary
IPSCs in pyramidal cells (Ouardouz and Lacaille, 1997 ).
Why are the time courses of GABAA,fast and
GABAA,slow different?
The differential sensitivity of GABAA,fast and
GABAA,slow to furosemide (see Figs. 9-11) and the atypical
proconvulsant benzodiazepine 4'-chlorodiazepam (Banks and Pearce, 1996 )
suggests that the receptors underlying these two currents are
structurally distinct. It does not necessarily follow, however, that
the decay kinetics of the two currents differ because the two types of
receptors have different binding or gating kinetics. Delayed clamp
experiments demonstrated that the conductance underlying
GABAA,slow has a slow decay component and that the current
is not prolonged simply because the synapses are electrotonically
remote (Pearce, 1993 ). However, it is still possible that the dendritic
IPSC is slower to decay because transmitter is present in the synaptic
cleft for an extended period of time. The observation that GABA uptake
inhibitors prolonged the slow decay phase of a biphasic IPSC in CA1
pyramidal cells (Roepstorff and Lambert, 1994 ) is consistent with this
hypothesis. At some central glutamatergic synapses the prolonged
presence of transmitter has been shown to underlie a slow decay phase
of the resulting postsynaptic current (Trussell et al., 1993 ; Barbour
et al., 1994 ; Rossi et al., 1995 ; Takahashi et al., 1995 ; Otis et al.,
1996 ). However, these synapses have morphological specializations that limit transmitter diffusion out of the synaptic cleft (Morest and
Jean-Baptiste, 1975 ; Mugnaini et al., 1994 ), and such specialized synapses have not been reported in hippocampus (Freund and
Buzsáki, 1996 ).
It should be noted that the delayed clamp experiments of Pearce (1993)
did not exclude the possibility that dendritic filtering does obscure a
rapid rising phase and initial decay phase of GABAA,slow and that the current is qualitatively similar to excised patch responses from the somata of these cells (see Fig. 11) and recorded in
other preparations (Puia et al., 1994 ; Verdoorn, 1994 ; Jones and
Westbrook, 1995 ). It may be possible to resolve this question by using
a recently developed analysis of the delayed clamp experiment (Hausser
and Roth, 1997 ).
Receptor subtypes mediating furosemide-sensitive currents
in CA1
We have shown that receptors mediating fast IPSCs and excised
patch responses are sensitive to furosemide but that receptors mediating slow IPSCs are not (see Figs. 9-11). Furosemide is a
selective blocker of 4- and 6-containing
GABAA receptors at the concentration used here (0.6 mM) (Wafford et al., 1996 ). Although the 6
subunit is expressed only in cerebellum (Laurie et al., 1992 ),
4 is expressed in CA1, suggesting that both the
receptors underlying fast IPSCs and receptors excised from pyramidal
cell somata are likely be composed of
4 x x.
Functional implications of kinetically distinct GABAA
inhibitory circuits
The properties of GABAA,fast and
GABAA,slow are consistent with distinct functional roles
for these two inputs. The somatic current GABAA,fast
controls the spike output of pyramidal cells in response to summed
excitation at the soma (Pearce, 1993 ; Miles et al., 1996 ), whereas the
dendritic current GABAA,slow acts locally, controlling the
level of dendritic polarization and thereby modulating the efficacy of
specific excitatory inputs in the dendrites of these cells (Davies et
al., 1991 ; Mott and Lewis, 1991 ; Kanter et al., 1996 ; Miles et al.,
1996 ; Kapur et al., 1997 ). Their kinetics also suggest different roles
in temporal patterning in hippocampal circuits, for example, with
GABAA,slow underlying theta (3-8 Hz) and
GABAA,fast underlying gamma (20-80 Hz) oscillations that
are thought to play separate functional roles in memory and arousal (Gray, 1994 ; Huerta and Lisman, 1995 ; Vinogradova, 1995 ). Further characterization of the properties of these currents and other elements
of cortical inhibitory circuits will improve our understanding of how
these circuits contribute to specific behaviors and will permit more
rational development of targeted therapeutic interventions in the
brain.
 |
FOOTNOTES |
Received Oct. 10, 1997; revised Dec. 2, 1997; accepted Dec. 3, 1997.
This work was supported by National Institutes of Health Grant NS01548
(to R.A.P.) and the Department of Anesthesiology, University of
Wisconsin-Madison. We thank Lew Haberly for valuable comments on this
manuscript and Phil Shils for technical support.
Correspondence should be addressed to Dr. Matthew I. Banks, Department
of Anesthesiology, University of Wisconsin, 43 Bardeen Labs, 1300 University Avenue, Madison, WI 53706.
 |
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