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Volume 17, Number 21,
Issue of November 1, 1997
pp. 8427-8442
Copyright ©1997 Society for Neuroscience
Synaptic Communication among Hippocampal Interneurons: Properties
of Spontaneous IPSCs in Morphologically Identified Cells
Norbert Hájos and
Istvan Mody
Departments of Neurology and Physiology, Reed Neurological Research
Center, University of California, Los Angeles, School of Medicine, Los
Angeles, California 90095-1769
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
DISCUSSION
FOOTNOTES
REFERENCES
ABSTRACT
The properties of spontaneous IPSCs (sIPSCs) recorded with
whole-cell patch-clamp techniques were investigated in various anatomically identified hippocampal CA1 interneurons and were compared
with those recorded in pyramidal cells. Neurons labeled with biocytin
or neurobiotin were classified on the basis of their dendritic and
axonal arborizations, leading to the identification of previously
unknown interneuron types projecting to the dendritic region of
pyramidal cells. In most interneurons, the average sIPSCs decayed
slower than did those observed in pyramidal cells. The properties of
sIPSCs were homogeneous within a given morphologically identified
neuron type. Many interneurons had comparable somatic size, location,
and dendritic arbor but displayed extremely different axonal
projections paralleled by distinct sIPSC properties. Thus, physiological comparisons are only meaningful after the complete morphological identification of the recorded cells. The decay of sIPSCs
matched for amplitudes and rise times could vary over 10-fold in a
given interneuron, consistent with electrotonic filtering and possibly
with different GABAA receptor subunit assemblies present at
distinct synapses. Our findings demonstrate an extensive connectivity
among hippocampal interneurons through GABAA synapses of
various properties that may underlie complex network oscillations at
different frequencies.
Key words:
hippocampus;
nonpyramidal cells;
intracellular labeling;
inhibition;
network;
oscillation;
GABA;
GABAA receptors
INTRODUCTION
The anatomical, physiological, and
biochemical characterization of different types of hippocampal
interneurons has expanded considerably (for review, see Freund and
Buzsáki, 1996 ). Intracellular labeling studies have begun to
classify interneurons according to the spatial selectivity of their
axonal and dendritic trees (Gulyás et al., 1993 ; Han et al.,
1993 ; Buhl et al., 1994 ; Buckmaster and Schwartzkroin, 1995 ; Sik et
al., 1995 ). These studies have defined two main groups of interneuron,
the perisomatic and the dendritic inhibitory cells, each likely
controlling distinct aspects of postsynaptic electrogenesis by
innervating specific spatial domains of principal cells (Miles et al.,
1996 ). Perisomatic interneurons, including the axo-axonic and basket
cells, are less multiform than are dendritic inhibitory cells such as
the O-LM, HIPP, bistratified, or horizontal trilaminar cells that show
a high variety in their input and output characteristics (Han et al.,
1993 ; Buhl et al., 1994 ; McBain et al., 1994 ; Sik et al., 1995 ).
As we learn more and more about interneurons, the classical view
about their purely inhibitory function is also changing. Interneurons
are now thought to provide the necessary timing mechanism for both low
and high frequency firing of principal cells (Soltesz and
Deschênes, 1993 ; Bragin et al., 1995 ; Buzsáki and Chrobak, 1995 ; Cobb et al., 1995 ; Whittington et al., 1995 ; Jefferys et al.,
1996 ). Connected interneuronal networks can sustain gamma oscillations
(20-70 Hz) without any requirement for fast excitatory synaptic drive
(Whittington et al., 1995 ; Traub et al., 1996 ) and, by sustaining such
oscillations, may participate in higher cognitive functions (Singer,
1993 ; Gray, 1994 ). Various modeling studies (Traub et al., 1996 ; Wang
and Buzsáki, 1996 ) have suggested that the frequency for such
network oscillations is critically dependent on the kinetic properties
of GABAA receptor-mediated events in interneurons and on
the nature of the connectivity among them. A specific control of
interneuronal networks may originate from a recently identified new
class of hippocampal interneuron specialized to innervate only other
interneurons (Acsády et al., 1996b ; Gulyás et al., 1996 ;
Hájos et al., 1996 ).
To better understand the operation of the interneuronal network, it is
important to determine the specific properties of GABAA receptor-mediated synaptic currents in different interneurons. To date,
the properties of spontaneous IPSPs and IPSCs (sIPSCs) have been
examined mainly in principal cells of the hippocampus, neocortex, and
cerebellum (Otis and Mody, 1992 ; Vincent et al., 1992 ; Puia et al.,
1994 ; Salin and Prince, 1996 ). The only GABAergic interneuron examined
so far for its sIPSCs is the cerebellar stellate cell in which IPSCs
with rapid rise and slow decay could be recorded (Llano and
Gerschenfeld, 1993 ). Such data are not available for morphologically
identified hippocampal interneurons. Some previous studies have
examined the inhibition in interneurons using sharp microelectrodes or
have recorded evoked IPSCs (Misgeld and Frotscher, 1986 ; Lacaille et
al., 1987 ; Lacaille and Schwartzkroin, 1988a ,b ; Lacaille, 1991 ;
Williams et al., 1994 ; Morin et al., 1996 ). These studies, however,
lacked proper morphological identification of the recorded cells and
may have failed to achieve the high resolution afforded by patch-clamp
techniques that is necessary to reveal small amplitude synaptic
activity (Soltesz and Mody, 1994 ). In the present study we recorded
GABAA receptor-mediated spontaneous IPSCs in hippocampal
interneurons of the CA1 region using the whole-cell patch-clamp
technique. We filled each cell with biocytin or neurobiotin and
reconstructed their axonal and dendritic arbors, allowing a complete
anatomical identification. The synaptic communication among hippocampal
interneurons shows a large heterogeneity of sIPSC kinetics that most
likely results from the presence of different GABAA
receptor subunit assemblies at distinct synapses.
MATERIALS AND METHODS
Slice preparation. Young (20-28 d old) male Wistar
rats were decapitated under deep sodium pentobarbital anesthesia (70 mg/kg, i.p.). After the skull was opened, the head was immersed in cold (~4°C), modified artificial CSF (ACSF), and the brain was removed. This ACSF contained (in mM): 126 NaCl, 2.5 KCl, 26 NaHCO3, 0.5 CaCl2, 10 MgCl2, 1.25 NaH2PO4,
10 glucose, and 2 kynurenic acid (Sigma, St. Louis, MO). Coronal slices
(350-450 µm thick) were prepared using a Lancer Series 1000 Vibratome. The slices were sagittally bisected along the midline and
were incubated in a storage chamber in ACSF (containing
CaCl2 and MgCl2 at 2 mM) for 30 min
at 32°C, and then the whole chamber was transferred to room
temperature (22-23°C). For the preparation of longitudinal slices,
the whole brain was sagittally cut into two halves, and the hemispheres
were glued on their callosal side onto a slope of 45° before slicing
with the Vibratome. Longitudinal sagittal slices (400 µm thick) were
cut parallel to the axis of the hippocampus.
Whole-cell recordings. Whole-cell voltage-clamp recordings
were obtained from interneurons and pyramidal cells visualized by
infrared DIC (IR-DIC) (Axioscope; Zeiss) videomicroscopy (Sakmann and
Stuart, 1995 ). Patch electrodes were pulled from borosilicate glass
capillaries with inner filament (KG-33, 1.5 mm outer diameter; Garner
Glass) using a two-stage vertical Narishige PP-83 puller and had a
resistances of 2-6 M . The intrapipette solution was prepared from
Omnisolve water (EM Science, Gibbstown, NJ) and contained (in
mM): 135 Cs gluconate, 5 CsCl, 20 HEPES, 2 MgCl2, 2 Mg-ATP, and 1-1.5% biocytin (Sigma, St.
Louis, MO) or neurobiotin (Vector Laboratories, Burlingame, CA) at pH
7.2-7.3, adjusted with CsOH yielding an approximate
Cl reversal potential (ECl ) of 45
mV. Final osmolarity was 290-310 mOsm.
During experiments, slices were superfused continuously with oxygenated
(95 %O2/5% CO2) ACSF containing
2 mM kynurenic acid to block fast ionotropic glutamate
receptors. All experiments were performed at room temperature
(22-23°C) within 6.5 hr of slicing. Neurons were mainly sampled in
coronal slices unless indicated otherwise. Recordings were made with an
Axopatch 2A or B amplifier (Axon Instruments), digitized at 88 kHz
(Neurocorder; NeuroData), and stored on videotape. Off-line, the data
were filtered at 1-1.5 kHz (eight pole Bessel; Frequency Devices
9002), digitized at 5-10 kHz (National Instruments Lab PC+
analog-to-digital board), and analyzed using the Strathclyde
Electrophysiology Software (courtesy of Dr. J. Dempster). The series
resistances were constant (±10%) during the period of analysis of
sIPSCs (2-5 min) and are indicated for each neuron in Table
1. The liquid junction potential was
reduced using an agar bridge (Neher, 1992 ). Events were detected as
described in detail elsewhere (Otis and Mody, 1992 ). The distributions of amplitudes, 10-90% rise times, and half decay times (T50%, i.e.,
the time required for an IPSC to decay to 50% of its peak amplitude)
of sIPSCs are plotted as cumulative probabilities drawn on a
probability scale ordinate (Origin 4.1; Microcal). In all cases, the
average sIPSCs were obtained from the most frequent 60% of all events,
i.e., from those IPSCs falling between 20 and 80% of the cumulative
probability distributions of amplitudes. The sIPSC time course was
determined by fitting single or average events using a least-squares
Simplex-based algorithm with the sum of two (one rising and one
decaying) or three (one rising and two decaying) exponentials (Soltesz
and Mody, 1995 ) of the form:
|
(1)
|
where I(t) is the sIPSC as a function of
time; A1 + A2 = A are constants; and R,
D1, and D2 are the
rise, fast decay, and slow decay time constants, respectively. For
single exponential decays, A2 was set to zero.
To evaluate the improvement of the fit by adding a second exponential
decay component, we used an F test as described in detail
elsewhere (Soltesz and Mody, 1995 ). The Kolmogorov-Smirnov (K-S)
statistical test was used to compare two different cumulative
distributions using SPSS for Windows. We have chosen a significance
level of 10 4 for the K-S statistic. Data are
presented as mean ± SE (n = number of cells).
Table 1.
sIPSC properties in morphologically identified hippocampal
CA1 neurons
| Cell types |
Code # |
Rs M |
sIPSC
frequency (Hz) |
Average amplitude
(pA)a |
R of average
(msec) |
Median T50% (msec) |
10-90% Range of T50% (msec)
|
|
| O-LM cells in coronal slices, Fig.
1C |
H0416 |
10.6 |
1.4 |
17.3 |
0.38 |
8.2 |
2.1-16.8 |
|
H0630 |
15.5 |
1.7 |
22.0 |
0.65 |
8.7 |
3.1-16.2 |
|
H0749 |
13.6 |
1.3 |
12.2 |
0.44 |
11.1 |
3.7-22.1 |
|
H0754 |
11.7 |
1.6 |
17.6 |
0.38 |
11.2 |
4.5-18.9 |
|
H0756 |
10.0 |
1.5 |
16.1 |
0.35 |
9.6 |
1.9-18.9 |
| O-LM cells in longitud.
slices |
H0763 |
10.1 |
5.3 |
19.3 |
0.37 |
7.2 |
2.8-13.5
|
|
H0946 |
14.3 |
2.9 |
14.6 |
0.49 |
7.0 |
2.5-13.2
|
| Bistartified cell, Fig.
6A |
H0759 |
8.6 |
1.2 |
19.0 |
0.30 |
8.1 |
1.5-15.9 |
| Radial trilaminar cells as in Fig.
5A |
H0741 |
10.6 |
3.1 |
22.0 |
0.31 |
9.7 |
4.9-12.6 |
|
H0742 |
11.0 |
0.8 |
18.9 |
0.59 |
9.3 |
5.1-11.1 |
| Radial trilaminar cells as in Fig.
5B |
H0405 |
11.6 |
3.3 |
21.3 |
0.32 |
7.2 |
1.3-14.8 |
|
H0414 |
11.7 |
0.5 |
19.5 |
0.31 |
9.4 |
2.1-13.3 |
|
H0634 |
8.6 |
3.1 |
36.7 |
0.51 |
8.7 |
2.5-11.4
|
| Multipolar cells projecting to strata
|
H0413 |
10.1 |
0.7 |
16.8 |
0.35 |
6.0 |
1.3-11.4
|
| radiatum and lacusosum-moleculare
|
H0619 |
8.3 |
6.4 |
31.3 |
0.51 |
6.4 |
2.1-13.2 |
| as
in Fig.
7Bb |
H0628 |
11.9 |
1.8 |
22.8 |
0.45 |
7.0 |
2.1-14.4 |
| Str. radiatum cells as in Fig.
7A |
H0352 |
15.4 |
3.0 |
35.3 |
0.57 |
10.8 |
4.8-18.9 |
|
H0740 |
10.5 |
1.6 |
16.9 |
0.41 |
14.1 |
4.9-19.2 |
|
H0758 |
9.2 |
3.4 |
24.5 |
0.64 |
8.1 |
2.1-16.5
|
| Cell with axon in all CA1
stratab |
H0766 |
12.3 |
3.8 |
18.2 |
0.56 |
10.5 |
3.3-18.1 |
| Cells in strata oriens or radiatum with
|
H0368 |
6.7 |
3.3 |
46.4 |
0.37 |
5.1 |
2.2-8.5
|
| projection to these layers, Fig.
6Bb |
H0627 |
9.1 |
4.3 |
31.8 |
0.29 |
6.0 |
3.1-8.5 |
| R-LM cells Figs 5A,
B |
H0637 |
11.1 |
1.1 |
13.4 |
0.34 |
8.7 |
2.1-19.6 |
|
H0408 |
13.6 |
1.3 |
16.7 |
0.40 |
14.5 |
4.3-31.8 |
| Pyramidal
cells |
H0242 |
7.9 |
5.5 |
35.0 |
0.39 |
8.7 |
2.8-13.6
|
|
H0403 |
11.0 |
10 |
37.4 |
0.48 |
7.8 |
2.4-12.2
|
|
H0411 |
10.0 |
1.2 |
27.6 |
0.52 |
9.6 |
1.2-15.0
|
| Giant radiatum cell in a longitud.
sliceb |
H0947 |
8.7 |
1.9 |
20.7 |
0.31 |
7.4 |
1.5-15.1 |
|
|
O-LM cells, Oriens/alveus interneurons projecting to
str. lacunosum-moleculare; R-LM cells, cells in str.
radiatum projecting to str. lacunosum-moleculare; Rs, access
resistance during the period used for analysis of sIPSCs properties
(2-5 min).
a
Measured at a holding potential of 0 ± 5 mV.
b
See Results for morphological details.
|
|
Anatomical identification of interneurons. At the end of the
recordings, slices were placed back into the storage chamber for 1 hr
and then fixed overnight in 4% paraformaldehyde, 0.05% glutaraldehyde, and 15% picric acid in 0.1 M phosphate
buffer (PB), pH 7.4. The slices were resectioned at 80 µm with the
Vibratome, incubated in cryoprotecting solution (0.01 M PB
containing 12% glycerol and 25% sucrose) for 30 min, freeze-thawed
three times above liquid nitrogen, and treated with 0.5%
H2O2 in 0.1 M PB for 30 min to
reduce endogenous peroxidase activity. Injected neurons were visualized
using avidin-biotinylated horseradish peroxidase complex reaction (ABC;
Vector Laboratories, Burlingame, CA) with nickel-intensified
3,3 -diaminobenzidine (Sigma, St. Louis, MO) as chromogen (dark blue
reaction product). After dehydration and embedding in Durcupan, the
representative neurons were reconstructed with the aid of a drawing
tube at 40-100× magnification. The lengths of the dendrites were
measured using the National Institutes of Health image program after
digitization with a CCD camera.
Reagents. Bicuculline (Sigma, St. Louis, MO) was applied by
bath perfusion in final concentrations of 30 µM. All
other salts and reagents were obtained from Fluka.
RESULTS
In the presence of the ionotropic glutamate receptor antagonist
kynurenic acid (2 mM), the frequencies of the sIPSCs varied between 0.5 and 6.4 Hz in interneurons and 1.2 and 10 Hz in pyramidal cells (Table 1). The sIPSCs were outward at a holding potential of
0 ± 5 mV, were reversed at ECl (near 45 mV),
and were blocked by the GABAA receptor antagonist
bicuculline (30 µM; n = 4; data not
shown).
Recordings were obtained from a total of 72 interneurons and 5 pyramidal cells. After visualization of biocytin or neurobiotin, the
neurons were classified according to their morphology. Only 36%
(n = 28) of the cells were included in the detailed
analysis of sIPSC properties. In these cells, the morphology could be
properly described, i.e., the neurons had well-stained dendritic
and axonal arbors. The interneurons excluded from our study
could not be completely reconstructed either because of their proximity
to the slice surface or because of the incomplete labeling.
Differences in sIPSC properties between pyramidal cells
and interneurons
The amplitudes of sIPSCs recorded in pyramidal cells (Fig.
1A) were larger than
those found in interneurons (Fig.
1D,F), but the distributions
of the rise times were similar (Fig. 1F). In general,
the half decay times (T50%) were also different (see the comparison of
pyramidal cells and an O-LM cell in Fig.
1E,F), but some
interneurons, e.g., radial trilaminar cells, had sIPSC T50% similar to
those recorded in pyramidal cells (Table 1). In three anatomically
identified pyramidal cells, the average sIPSC properties were
homogeneous (Fig. 1D). The mean amplitude and fast
rise-time constant of the averages were 34.3 ± 2.7 pA and
0.49 ± 0.05 msec, respectively (n = 3).
Furthermore, the cumulative distributions of sIPSC amplitudes, rise
times, and T50% were also well matched between pyramidal cells (Fig.
1F; Table 1). A recording in a longitudinal slice
from a neuron with pyramidal cell-like morphology in the stratum (str.)
radiatum, spiny dendrites located in strata radiatum and
lacunosum-moleculare, and its axon projecting to str. oriens
(Maccaferri and McBain, 1996 ) revealed sIPSC kinetics similar to those
found in pyramidal cells (Table 1) but with a smaller average amplitude
(20.7 pA).
Fig. 1.
Comparison of sIPSC kinetics in pyramidal
cells and an O-LM cell. A, B, Images of
an intracellularly filled pyramidal cell (A;
PC) and of an O-LM cell (B) were
digitized after visualization of biocytin or neurobiotin (the
arrow shows the main axon originating from a proximal
dendrite). C, Camera lucida reconstruction of the O-LM
cell in B from three 80-µm-thick vibratome sections. The cell had a spiny dendritic tree restricted to the str. oriens, whereas most axon collaterals were found in the str.
lacunosum-moleculare. D, The averages of sIPSCs in three
morphologically identified pyramidal cells are very similar, in
contrast to the average sIPSC in the O-LM cell. E, The
sIPSC averages (shown normalized) in a pyramidal cell and an O-LM cell were fitted by the sum of
rising and decaying exponentials (indicated by solid
line). The fitted amplitudes of sIPSC averages markedly
differed in the pyramidal cell and the O-LM cell (35.0 vs 12.2 pA), but
the rise-time constants were comparable (0.39 vs 0.44 msec). The
decaying phase of the average sIPSC in the O-LM cell was slower than
that in the pyramidal cell. F, Cumulative probability
plots of amplitude and T50% distributions show marked differences
between pyramidal cells (n = 3) and an O-LM cell
(arrow). The 10-90% rise times were not different.
Kolmogorov-Smirnov (K-S) statistics indicate nonsignificant p values
(p > 10 4) for T50%
among the three pyramidal cells, but the T50% distribution of the O-LM
cell significantly differed from that of the pyramidal cells.
Generally, pyramidal cells had sIPSCs with larger amplitudes and faster
decays compared with those recorded in interneurons. Note that the
cumulative distributions are comparable in all pyramidal cells.
S.O., Str. oriens; S.P., str. pyramidale;
S.R., str. radiatum; S.L-M., str.
lacunosum-moleculare; and S.MOL., str. moleculare. Scale
bars: A, B, 20 µm; C,
100 µm.
[View Larger Version of this Image (48K GIF file)]
Properties of sIPSCs in oriens/alveus interneurons projecting to
stratum lacunosum-moleculare (O-LM cells)
The cell bodies and dendrites of anatomically identified O-LM
cells were confined to str. oriens and alveus (Fig. 1
B,C). A common morphological
feature of these cells was the presence of spiny dendrites giving rise
to some short branches close to their tips. In all seven cases, the
main axon without varicosities originated from a proximal dendrite and
crossed the pyramidal cell layer and str. radiatum. After reaching the
border of strata radiatum and lacunosum-moleculare, the axon arborized
almost exclusively in the str. lacunosum-moleculare where the axon
collaterals became fine and varicose. Neurons with similar arborization
patterns in the CA1 region have been described previously both in
vitro and in vivo (McBain et al., 1994 ; Sik et al.,
1995 ). Four of the seven O-LM cells had some axon collaterals in the
str. oriens as well. A camera lucida reconstruction of an O-LM cell
from three 80-µm-thick sections is shown in Figure 1C. The
properties of sIPSC averages recorded in O-LM cells in coronal slices
were homogeneous (Fig.
2B). Their average
amplitude was 17.0 ± 1.5 pA, whereas the mean
R had a value of 0.44 ± 0.05 msec
(n = 5). The distributions of amplitudes, 10-90% rise
times, and T50% had similar plots in all anatomically identified O-LM
cells (Fig. 2A; Table 1).
Fig. 2.
sIPSC kinetics in O-LM cells
(n = 5) recorded in coronal slices were
homogeneous. Accordingly, cumulative probability distributions of
amplitudes, 10-90% rise times, and T50% (A),
as well as averages (B, thinner traces),
were similar among the five cells. Two additional O-LM cells sampled in
longitudinal slices had matching sIPSCs (B,
thicker traces; A, B,
arrows) that differed in decay times and frequencies
from sIPSCs of O-LM cells recorded in coronal slices (see Results for
details). C, Three populations of sIPSC decay time
constants denoted by the means (x1,
x2, and
x3) were found in both coronal versus
longitudinal slices. Note that the proportion of sIPSCs with fast decay
time constants was considerably higher in longitudinal slices. This
change caused the shift to the left on cumulative
distributions of T50% (A, arrow) and
affected the averages as well (see Table 1).
[View Larger Version of this Image (36K GIF file)]
O-LM cells and other interneurons with a horizontal dendritic tree in
the str. oriens may receive GABAergic innervation from neurons with
axonal projections in a plane different from the plane of a coronal
slice. Electrical stimulation experiments in the str. oriens support
the possibility of such oriented projections (Lacaille and
Schwartzkroin, 1988a ). For example, interneuron-specific inhibitory
cells immunoreactive for vasoactive intestinal polypeptide (VIP) and
for the calcium-binding protein calretinin (CR) form a dense axonal
plexus at the str. oriens and alveus border and may project mainly
along the longitudinal axis of the hippocampus (Acsády et al.,
1996a ) (L. Acsády, personal communication) to innervate
horizontal interneurons including O-LM cells in this layer
(Acsády et al., 1996b ). This anatomical finding together with the
higher probability of recording spontaneous synaptic events originating
from long, intact axon collaterals (Staley and Mody, 1991 ) would ensure
a higher probability of recording O-LM cell sIPSCs in a slice cut in
the longitudinal plane. Therefore, we investigated the possibility that
cutting a slice along the longitudinal axis of the hippocampus may
better preserve the inhibitory inputs onto O-LM cells. We obtained
recordings from two additional identified O-LM cells in such a slice
preparation. The overall frequency of sIPSCs in these O-LM cells was
markedly higher (4.1 ± 1.2 Hz; n = 2) than that
found in coronal slices (1.52 ± 0.06 Hz; n = 5;
see also Table 1). We measured the total dendritic length of O-LM cells
in both types of slices to ensure that the difference in sIPSC
frequency is not a consequence of the different size of the dendritic
tree spanning in coronal versus longitudinal slices. The average total
dendritic lengths of O-LM cells were 1633 ± 200 µm (between
1201 and 2256 µm; n = 5) in coronal slices and
1683 ± 342 µm (1341 and 2025 µm; n = 2) in
longitudinal slices. Therefore, the observed difference in frequency of
sIPSCs cannot result from a significantly different dendritic
morphology but rather from the different input these neurons receive in
the two slice preparations. In addition to the increased frequency, the ratio of sIPSCs with fast decay time constants increased to 70% in an
O-LM cell of a longitudinal slice compared with only 31% in an O-LM
cell of a coronal slice (Fig. 2C). The other O-LM cells had
similar ratios for IPSC decay time constants depending on the slice
preparation. The change in the ratio of fast IPSCs is also reflected by
a shift to the left on the cumulative probability distributions of T50% (Fig. 2A, arrow),
but the amplitude and rise-time distributions were indistinguishable in
the two preparations. The T50% values, but not the rise times, of
sIPSCs recorded in the two O-LM cells in longitudinal slices were
significantly different (K-S p < 10 4) from the average of all O-LM cells recorded
in coronal slices. In agreement with this observation, the average
sIPSCs in O-LM cells from the longitudinal slices showed faster decay
phases (Fig. 2B) but had similar amplitudes
(16.9 ± 2.3 pA) and rise times (0.43 ± 0.06 msec) compared
with the averages in O-LM cells of coronal slices (Table 1).
Regardless of the slice orientations, the amplitude of average sIPSCs
in O-LM cells was smaller than that in pyramidal cells (Table 1). To
examine the IPSC conductance in O-LM cells, we recorded sIPSCs at
different holding potentials (+15, 0, 70, or 75 mV) in three
identified cells (two in coronal slices and one in a longitudinal
slice). The conductance was linear, and the sIPSCs reversed at
ECl of 44.6 ± 2.6 mV (n = 3). The slope conductance of average sIPSC was between 0.35-0.45 nS in
O-LM cells, approximately half of the conductance recorded in pyramidal
cells (also see Cohen et al., 1992 ).
The complete anatomical identification of recorded cells helps
explain the differences in sIPSC properties
Two cells located in the upper part of the str. radiatum close to
str. lacunosum-moleculare showed similar small round somata and were
indistinguishable by IR-DIC videomicroscopy. Moreover, after the
biocytin was visualized, both cells had comparable multipolar dendritic
trees at low magnification by light microscopy (Fig. 3A,B).
In spite of their similar appearance, they possessed markedly different
sIPSC properties (Fig. 3F). The cell (H0741) in Figure 3A had a larger average amplitude (22.0 pA) and faster decay
time than did the cell (H0637) in Figure 3B (13.4 pA) (Fig.
3C-E), but their rise-time constants were similar (0.31 and
0.34 msec, respectively).
Fig. 3.
A, B, Images of two
interneurons with similar small round cell bodies and multipolar
dendritic trees in the upper part of str. radiatum (close to str.
lacunosum-moleculare). The arrowhead in A
marks the origin of the axon. C, D, In
contrast to their matching appearance, the decaying phases of sIPSC
averages showed marked differences (C, D
for cells in A, B, respectively) that are
more pronounced in normalized and superimposed averages
(E). F, Differences in cumulative
probability distributions of amplitudes, rise times, and T50% are
significant (K-S p < 10 4;
solid lines represent the cell in A;
dashed lines represent the cell in B).
For abbreviations, see legend for Figure 1. Scale bars:
A, B, 20 µm.
[View Larger Version of this Image (46K GIF file)]
Figure 4 illustrates another example of
two cells with large somata at the strata radiatum and
lacunosum-moleculare border with indistinguishable appearance under
IR-DIC visualization and after development of the tracer. Both cells
were located close to the border of strata radiatum and
lacunosum-moleculare and gave rise to several dendritic branches,
including one branch toward the pyramidal cell layer. In spite of their
similar morphology at low magnification in the light microscope, their
sIPSC kinetics diverged considerably. A proportion of the synaptic
currents from the cell in Figure 4A (H0408) had slow
rise and decay times, as shown on the cumulative probability plots. The
difference in the average sIPSCs was even more pronounced than in the
previous example. Although the rise-time constants were comparable
(0.40 and 0.51 msec), both the amplitudes (16.5 vs 36.6 pA) and the
decay of the averages were distinct in these two cells (Fig.
4C-E).
Fig. 4.
A, B, Images of two
interneurons close to the border of strata radiatum and
lacunosum-moleculare match in somata and dendritic arbors.
C, D, Their average sIPSCs, however, show
strikingly different decay kinetics (C and
D for cells in A and B,
respectively) that are more visible after superimposing the normalized
traces (E). F, In
line with this observation, the cumulative probability plots of the
kinetic parameters are also significantly different (K-S p < 10 4; solid
lines represent the cell in A; dashed
lines represent the cell in B). For
abbreviations, see legend to Figure 1. Scale bars: A,
B, 20 µm.
[View Larger Version of this Image (46K GIF file)]
Only a detailed camera lucida reconstruction of these interneurons with
remarkably different sIPSC kinetics could confirm that they belonged to
distinct morphological categories. The sparsely spiny dendrites of the
cell in Figure 3A (H0741) spanned all layers of the CA1
subfield, whereas the axon ran in str. radiatum and descended into the
str. oriens as well (Fig. 5A).
In contrast, the axon of the cell in Figure 3B (H0637)
occupied the termination zone of the entorhinal projection, i.e.,
mainly the str. lacunosum-moleculare, but some varicose branches also
entered and ramified in the outer two-thirds of the str. moleculare in
the dentate gyrus (Fig. 5A). Some axon collaterals were
found in the str. radiatum close to the str. lacunosum-moleculare. The
beaded multipolar dendritic tree of the cell bore a few spines confined
to strata lacunosum-moleculare and radiatum without reaching the str.
pyramidale.
Fig. 5.
Camera lucida reconstructions of interneurons in
Figures 3 and 4 from three to four 80-µm-thick vibratome sections.
A, The radial trilaminar cell in Figure
3A gave rise to dendrites ascending and descending to
all layers of the CA1 region, whereas its axon ramified mainly in str.
radiatum and, after crossing the pyramidal cell layer, partly in str.
oriens (dendritic arbor of the cell, red; axon tree,
blue). The dendritic tree of the R-LM cell in Figure
3B was found to extend to strata radiatum and
lacunosum-moleculare. In contrast to the radial trilaminar cell, its
axonal arbor was predominantly located in conjunction with the
entorhinal afferents (dendrites, black; axon cloud of
the R-LM cell, green). B, The other R-LM
cell in Figure 4A had dendrites spanning all
strata of the CA1 region, but its axonal arbor was restricted to str. lacunosum-moleculare (dendrites, black; axon,
green). In sharp contrast to the R-LM cell, the axon
cloud of another radial trilaminar cell in Figure
4B occupied all of the layers of this subfield except the str. lacunosum-moleculare, but its dendritic tree was similar (dendrites, red; axon, blue). For
abbreviations, see legend to Figure 1. Scale bars: A,
B, 100 µm.
[View Larger Version of this Image (38K GIF file)]
The other pair of interneurons with matching somata and radial
dendritic arbors but different sIPSC properties (Fig.
4A,B) had strikingly different
axonal arborizations (Fig. 5B). Both cells gave rise to
dendrites ascending to the str. lacunosum-moleculare and to descending
branches toward str. pyramidale, one of them entering the str. oriens.
In both cases, some spines were observed on the beaded dendritic tree.
In sharp contrast to their comparable dendritic morphology, their
axonal arborizations were entirely different (Fig. 5B). The
cell in Figure 4A (H0408) arborized almost exclusively in str. lacunosum-moleculare without crossing the fissure.
Some axon branches of this cell were also localized in the str.
radiatum close to the border of str. lacunosum-moleculare. In contrast,
the axon cloud of the other neuron shown in Figure 4B
(H0414) covered all layers of the CA1 region except the str. lacunosum-moleculare (Fig. 5B). The majority of the axon
collaterals were found in the entire str. radiatum, but a portion was
also observed in both strata pyramidale and oriens.
The morphological and physiological similarities between the
cells located in str. radiatum and projecting to the str.
lacunosum-moleculare (R-LM cell, H0637, H0408) suggest that these cells
most likely belong to a novel, yet undescribed, interneuron type in the
CA1 region of the hippocampus. Some minor morphological differences were present (e.g., some axon collaterals in the str. moleculare of the
dentate gyrus of the cell in Fig. 5A), but we will
collectively refer to these interneurons as R-LM cells. In these
interneurons, a considerable portion (~20%) of sIPSCs had extremely
slow rise times (>10 msec), and a large fraction of sIPSCs had
exceptionally slow decays, slower than those recorded in any other
interneurons (see Figs. 3, 4, 8; Table 1). The other reconstructed
interneurons in Figure 5A and B (H0741, H0414)
may also represent the same category of nonpyramidal cells based on the
comparable sIPSC kinetics and arborization patterns. Radial trilaminar
cell type with comparable morphological properties has been mentioned
previously without any reconstructions (Freund and Buzsáki,
1996 ). Therefore, in the present study we denote all interneurons in
str. radiatum with ascending and descending dendrites projecting mainly
to the str. radiatum and partly to strata pyramidale and oriens as
radial trilaminar cells.
Fig. 8.
Rise times and decay time constants of sIPSCs in
two interneurons belonging to different cell groups. A,
The rise times of sIPSCs in the 16-25 pA amplitude range are plotted
against their decay time constants (log scale). The individual events
of the radial trilaminar cell (H0741) are open circles,
whereas solid circles indicate sIPSCs of the R-LM cell
(H0408). Note the high variability of decay time constants of sIPSCs
around their averages (Figs. 3C, 4C).
Also note that the events with large decay time constants are more
abundant in the R-LM cell than in the radial trilaminar cell. The
events in two boxes with fast and slow rise times were
selected and averaged based on the three Gaussian distributions of the
rise times (see Results for details). For the radial trilaminar cell
(H0741), the trimodal distribution of the rise times (solid line) had the following means (± SD): 0.55 ± 0.13, 1.09 ± 0.53, and 2.57 ± 0.44 msec. The distributions for
the R-LM cell (H0408) are shown with dashed lines and
had the following means (± SD): 0.60 ± 0.07, 1.14 ± 0.62, and 3.50 ± 0.96 msec. Fast (B) and slow (C) rise-time sIPSC averages from both cells are
shown superimposed. The insets show the rising phases at
a higher time resolution. Although they had similar fast rise times,
two groups of sIPSCs in the radial trilaminar cell (thicker
traces; D, 10.8 and 22.4 msec) were
seen, whereas three types of decays could be seen in the R-LM cell
(thinner traces; D, 12.3, 23.4, and 36.2 msec). The decay time constants of average sIPSCs with slow rise times were 17.7 msec in the radial trilaminar cell and 39.9 msec in R-LM cells.
[View Larger Version of this Image (30K GIF file)]
Recordings from three additional radial trilaminar cells, one with a
similar morphology to the cell in Figure 5A (H0741) and two
others more like the interneuron in Figure 5B (H0414),
revealed comparable sIPSC properties as described above (see Table
1).
Comparable morphology of interneurons does not imply similar
sIPSC properties
In the previous section, we have stressed the importance
of a detailed anatomical distinction of interneurons to correlate with
the diverse sIPSC properties. Conversely, sIPSC properties might be
expected to be similar in interneurons with relatively similar
morphologies. However, we have found some exceptions to this
assumption. For example, Figure 6 shows
two interneurons with dendritic and axonal arborization in strata
radiatum and oriens in which sIPSC properties were remarkably
different. A bistratified cell (Fig. 6A; H0759),
analogous to that first reported by Buhl et al. (1994) , had its cell
body in str. pyramidale and gave rise to ascending and descending
vertical dendrites that did not penetrate the str.
lacunosum-moleculare. The axon cloud of the cell covered strata
radiatum and oriens with only traversing collaterals in the pyramidal
cell layer. The soma and the majority of dendrites of the cell depicted
in Figure 6B (H0368) were located in str. oriens and
had a rather horizontal appearance. Two dendritic branches ascended to
str. radiatum, but they did not enter into the str.
lacunosum-moleculare. The main axon originated from a primary dendrite,
passed through the str. pyramidale, and predominantly ramified in str.
radiatum. The axonal arbor was only partially reconstructed because,
after curving back into the str. oriens, two main axon branches were
cutoff. In summary, based on the location of their processes, both
interneurons might have shared similar input and output
characteristics, but they differed somewhat in their dendritic length
confined to various layers.
Fig. 6.
Interneurons with comparable morphology may
show differences in their sIPSC kinetics. A, A
bistratified cell gave rise to both axons and dendrites to strata
radiatum and oriens avoiding str. lacunosum-moleculare. The main axon
originated from a secondary dendrite. B, A cell with the
soma and with the majority of the dendrites in str. oriens had axon
collaterals mainly in str. radiatum, where two dendritic branches were
also found. Note the two main axon collaterals left the slice in the
str. oriens. (For a detailed morphological description, see Results)
C-E, The average sIPSCs of these cells
(C for bistratified cell and D for the
cell in B) were remarkably distinct in amplitudes and
decays, more visible after normalization and superimposition
(E). F, The cumulative probability
distributions of amplitudes, 10-90% rise times, and T50% of these
interneurons differed significantly (K-S p < 10 4; solid lines represent the
bistratified cell; dashed lines represent the other
cell). For abbreviations, see legend to Figure 1. Scale bars:
A, B, 100 µm.
[View Larger Version of this Image (29K GIF file)]
In sharp contrast to their comparable morphology, the distributions of
amplitudes, rise times, and T50% recorded in the bistratified cell and
in the cell projecting to the str. radiatum (and probably to the str.
oriens as well) (H0368) markedly differed (Fig. 6F; Table 1). In line with these data, the average sIPSCs also showed differences in amplitudes (19.1 vs 46.4 pA) and decays (Fig.
6C-E); however the rise-time constants were practically the
same ( R, 0.30 vs 0.37 msec). The cell shown
in Figure 6B (H0368) and another interneuron (H0627;
Table 1) with matching rise-time and T50% distributions had the
fastest-decaying average sIPSCs among all interneurons in the present
study (also see Table 1). This latter cell (H0627) with fast sIPSC
kinetics was found in the str. radiatum and projected to strata
radiatum and oriens, but some axonal branches could be followed into
the str. lacunosum-moleculare.
The properties of sIPSCs were also measured in interneurons with axonal
arbors confined to the apical dendritic region of CA1 pyramidal cells.
One group of cells had axon and dendritic arbors restricted to the str.
radiatum (str. radiatum cells; n = 3). Two of the three
cells had similar morphology, displaying a sparsely spiny dendritic
tree (Fig. 7A). The other
neuron (H0352; Table 1) gave rise to aspiny beaded dendrites and
frequently bifurcated varicose axon collaterals similar to the cell
reported by Gulyás et al. (1993) . The sIPSC properties of the
str. radiatum cells and their distributions were homogeneous (Fig.
7C,E,F; also see Table
1).
Fig. 7.
sIPSCs in interneurons with different
morphologies. A, A cell in the apical dendritic region
of pyramidal cells gave rise to both the axonal and dendritic branches
restricted to the str. radiatum (str. radiatum cell). B,
The dendrites and the axons of a multipolar cell with primary dendrites
bifurcating close to the soma ramified mainly in str. radiatum and
partly in str. lacunosum-moleculare, only one dendritic branch entered
the str. oriens. The averages of sIPSCs show similar appearances
(C for the str. radiatum cell and D for
the multipolar cell); however after they were normalized and
superimposed, the average sIPSC of the str. radiatum cell has a
somewhat slower decay than that found in the multipolar cell projecting
to strata radiatum and lacunosum-moleculare (E).
F, This small difference in decays of the averages is
more noticeable on the cumulative probability plots of T50%, although
the rise times are comparable (solid lines represent the
str. radiatum cell; dashed lines represent the
multipolar cell). The K-S statistics indicate a nonsignificant
p value of 1.2 × 10 2 for the
rise time and a significant p value of < 10 4 for the T50% distributions. Similar
deviations of sIPSC decays were noticed in other identified str.
radiatum cells and multipolar cells projecting to strata radiatum and
lacunosum-moleculare as well (Table 1). For abbreviations, see legend
to Figure 1. Scale bars: A, B, 100 µm.
[View Larger Version of this Image (33K GIF file)]
Another set of interneurons in the str. radiatum had an aspiny
multipolar dendritic tree (Fig. 7B; n = 3).
Several (five to seven) primary dendrites arose from the large somata
and bifurcated close to their origin, giving a stellate-like appearance
to these cells. The varicose axons were predominantly confined to str. radiatum, but numerous collaterals could be traced to str.
lacunosum-moleculare but never crossed the fissure. Their dendritic
arbors passed through all layers of the hippocampus, but the bulk of
the dendrites was located in str. radiatum (n = 2). One
such cell (H0413; Table 1) had a small round soma, and its dendrites
were only confined to strata radiatum and lacunosum-moleculare. The
kinetic properties of sIPSCs in these cells were homogeneous (Fig.
7D-F; Table 1), but their decays were faster than those
recorded in str. radiatum cells (Table 1). This difference is less
visible on the normalized and superimposed averages (Fig.
7E) but is clearly evident in the probability distribution
plots of T50% (Fig. 7F; Table 1).
We have also recorded from an interneuron similar to that reported
previously by Lacaille and Schwartzkroin (1988a) and Kunkel et al.
(1988) . This cell (H0766; Table 1) had a mainly horizontal dendritic
tree located at the border of strata radiatum and lacunosum-moleculare, two branches descended into str. oriens. The axon emitted branches in
all layers of the CA1 region (from str. lacunosum-moleculare to str.
oriens), and some collaterals crossed the fissure and ramified in str.
moleculare of dentate gyrus, reaching the granule cell layer as well.
The sIPSCs kinetics were comparable with those recorded in radiatum
cells (Table 1) with similar cumulative probability distributions (data
not shown).
Table 1 summarizes the properties of sIPSCs recorded in the 28 cells of
this study grouped according to their detailed anatomical identification.
Variability of sIPSCs in a given interneuron
Most sIPSCs decayed with time constants ranging between
5 and 40 msec (as long as 80 msec in the R-LM cells), showing a high degree of variability around the mean. In a given interneuron, the vast
majority of individual sIPSCs (>98%) were well fitted by a single
exponential decay. The multipolar cells projecting to strata radiatum
and lacunosum-moleculare (Fig. 7B) were an exception. In all
three of these cells, the fraction of events with double exponential
decays was 5-8%. The variability in decay times recorded in a given
cell type may result from electrotonic filtering and/or from different
GABAA channel properties at different synapses. Because in
CA1 interneurons rise times of synaptic events are as sensitive to
electrotonic filtering as are decay times (Thurbon et al., 1994 ), we
selected events based on their similar rise times. To avoid bias caused
by different amplitudes, we selected all events over an amplitude range
of 16-25 pA. The decay time constants of these selected events were
plotted against the 10-90% rise times. The majority of the
interneurons had plots similar to those shown for the radial trilaminar
cell (H0741) in Figure 8A. In both cells, the
10-90% rise times could be well fitted with three Gaussian
distributions (Fig. 8A). We chose to compare IPSCs
with fast (0.2-0.9 msec) and slow (2.5-3.5 msec) rise times. Such
sIPSCs selected on the basis of similar rise times could still be
assigned to three groups based on their decay time constants. The decay
time constants for the three groups ranged between 5 and 12 msec, 12 and 25 msec, and 25 and 45 msec. The decays of the average sIPSCs
resulting from this grouping were fitted with a single exponential. In
the radial trilaminar cell (H0741), sIPSCs with fast rise times could
be separated into two groups with decay time constants of 10.8 and 22.4 msec, whereas the fast rise-time events in the R-LM cell (H0408) had
decays of 12.3, 23.4, and 36.2 msec (Fig. 8B).
Averages of sIPSCs with comparatively slow rise times showed the
following decay time constants: 17.7 msec in radial trilaminar cell and
39.9 msec in the R-LM cell. These results indicate a large
heterogeneity of spontaneous GABAA events in a given cell
and among interneuron types. Although interneurons are less compact
electrotonically than is suggested by their anatomy (Thurbon et al.,
1994 ; Mott et al., 1997 ), the lower variance of rise times than that of
decay time constants in similar amplitude events implies that distinct
GABAA receptor kinetics at different synapses may
contribute more importantly than electrotonic filtering to determining
sIPSC diversity.
DISCUSSION
The major findings of the present study may be summarized as
follows: (1) the kinetic properties of IPSCs in interneurons are
different than those of pyramidal cells; (2) the characteristics of
GABAA receptor-mediated synaptic transmission among
interneurons show a high variability; and (3) new hippocampal CA1
interneuron types could be identified with intracellular labeling.
Kinetic properties of sIPSCs differ between pyramidal cells
and interneurons
The general features of GABAA receptor-mediated
spontaneous synaptic currents recorded in pyramidal cells were similar
to those reported previously in pyramidal cells of the hippocampus (Collingridge et al., 1984 ; Cohen et al., 1992 ) or the neocortex (Salin
and Prince, 1996 ). The decay time constants of sIPSCs recorded in
pyramidal cells ( D, ~12-14 msec) differed
from those recorded in dentate granule cells at room temperature
(Collingridge et al., 1984 ; Otis and Mody, 1992 ; Salin and Prince,
1996 ). Under the same experimental conditions, the decay time constant
of sIPSCs in dentate granule cells ranged between 19 and 23 msec (N. Hájos and I. Mody, unpublished observations), similar to those
recorded by Otis and Mody (1992) . The difference between sIPSC kinetics of the pyramidal cells and of granule cells may reflect the expression of distinct GABAA receptor subunits with different
physiological properties, for example, more abundant 5 expression in
pyramidal cells but more subunits in granule cells (Wisden et al.,
1992 ).
As demonstrated for O-LM cells and pyramidal cells, the sIPSC averages
and cumulative probability distributions of amplitudes, rise times, and
T50% are homogeneous in a given cell type but can differ across the
neuronal types. High-resolution immunocytochemistry for the
GABAA receptor subunits has demonstrated the localization of 1, 2/3, and 2 subunits in both principal cells and
interneurons even at the same synapses. The main difference between the
two cell groups seems to be the higher density of some
GABAA receptor subunits on interneurons (Nusser et al.,
1995 ; Somogyi et al., 1996 ). Our physiological data are consistent with
the presence of distinct GABAA receptor subunit assemblies
at various synapses on interneurons as reflected by the variety of IPSC
properties.
Synaptic communication among interneurons through
GABAA receptors
The GABAA receptor-mediated spontaneous synaptic
currents recorded in hippocampal interneurons may originate from at
least three different intrinsic and extrinsic sources: (1) from
interneurons without target selectivity (for example, basket cell or
str. radiatum cell; Gulyás et al., 1993 ; Sik et al., 1995 ), (2)
from interneurons specifically innervating other interneurons
(Acsády et al., 1996b ; Gulyás et al., 1996 ; Hájos et
al., 1996 ), and (3) from the GABAergic septohippocampal pathway (Freund
and Antal, 1988 ; Tóth et al., 1997 ). These different inputs in a
given interneuron may use different subunit combinations of
GABAA receptors with distinct kinetic properties, giving an
anatomical basis for this variability. This assumption is supported by
our findings in O-LM cells, if interneuron-specific inhibitory cells
projecting to the str. oriens/alveus border act through
GABAA channels with characteristic properties that produce rapidly decaying IPSCs. The first anatomical evidence of the different localization of a GABAA receptor subunit at synapses
derived from distinct hippocampal interneuron populations has been
recently published (Nusser et al., 1996 ). In addition to the
heterogeneity of the GABAergic input, the subunit expression in various
hippocampal interneurons may also differ. As shown by double
immunocytochemical labelings, the 1 subunit has been found in
different subsets of neurochemically characterized interneurons (Gao
and Fritschy, 1994 ), providing the anatomical substrate for a diversity
of sIPSC kinetics among interneurons. Further research using
GABAA receptor subunit selective drugs (Lüddens et
al., 1995 ) is under way to determine the precise molecular assembly of
synaptic GABAA receptors on different interneurons. The
extremely slow spontaneous events with up to 40 msec decay time
constants in R-LM cells may reflect distinct desensitization properties
of GABAA channels in these cells. Repeated binding of GABA
to the receptors at these synapses should result in a multiexponential
decay kinetics (Jones and Westbrook, 1995 ), such as seen in a small
fraction (5-8%) of sIPSCs recorded in multipolar cells projecting to
the strata radiatum and lacunosum-moleculare.
Novel type of hippocampal CA1 interneurons with axonal arbors in
the dendritic region of pyramidal cells
Recent in vitro and in vivo studies using
intracellular labeling methods have identified several hippocampal CA1
interneuron types and have classified them according to their input and
output features (Buhl et al., 1994 ; McBain et al., 1994 ; Sik et al., 1995 ; Freund and Buzsáki, 1996 ; Halasy et al., 1996 ; Maccaferri and McBain, 1996 ). Numerous physiological recordings were obtained from
interneurons in this hippocampal subfield, but only two groups of
dendritic inhibitory cells, namely bistratified cells and O-LM cells
(Buhl et al., 1994 ; McBain et al., 1994 ; Sik et al., 1995 ; Halasy et
al., 1996 ), have been morphologically characterized in detail. These
cell types have been confirmed in our study as well. More recent
in vivo studies have extended further the morphological variety to horizontal trilaminar and back-projection cells (Sik et al.,
1994 , 1995 ).
The R-LM cells in our study represent a novel interneuron type based on
the characteristic sIPSC kinetics and morphological features. The
presence of such cells in the CA1 region suggests that two different
interneuron classes (O-LM and R-LM cells) are specialized to control
the effect of entorhinal afferents on CA1 pyramidal cells with distinct
input properties. The O-LM cells are likely to be excited in feedback
manner, receiving their innervation mainly from local collaterals of
CA1 pyramidal cells (Blasco-Ibanez and Freund, 1995 ; Maccaferri and
McBain, 1995 ). In contrast, the excitatory input of R-LM cells may
derive predominantly from CA3 pyramidal cells and entorhinal afferents
(Ishizuka et al., 1990 ; Witter, 1993 ); thus they are likely to
participate in feed-forward inhibition (Buzsáki, 1984 ). Their
function may be to enhance the contrast between a Schaffer
collateral-driven state and the entorhinal-driven state of CA1
pyramidal cells.
Interneurons with appearance similar to our str. radiatum and radial
trilaminar cells have been previously alluded to, but with less
complete anatomical details (Kawaguchi and Hama, 1987 , 1988 ; Bergles et
al., 1996 ). The multipolar cells with axon clouds in strata radiatum
and lacunosum-moleculare have not been described previously, although
cells with stellate-like appearance containing neuropeptide Y (NPY) and
immunoreactive for substance P receptor (SPR) have been reported
without any axon staining (Acsády et al., 1997 ). The similar
dendritic morphology may mean that these multipolar cells labeled in
the present study belong to the NPY and SPR-immunopositive category of
interneurons.
The cells mentioned above showed similar sIPSC kinetics but displayed
different morphological features. Therefore, it is not clear whether
these cells represent a continuum of the dendritic inhibitory cells or
whether they belong to a functionally distinct type of hippocampal
interneurons.
Functional implications
According to recent modeling studies, the frequency of interneuron
network oscillations should depend on the conductance and decay time
constant of GABAA receptor-mediated events (Traub et al.,
1996 ; Wang and Buzsáki, 1996 ). Our recordings in a variety of
interneurons show a high variability of the sIPSC decay time constants
(5-80 msec) at room temperature (22-23°C). Assuming the temperature
dependence of sIPSCs in interneurons is similar to that recorded in
dentate granule cells (Otis and Mody, 1992 ), the decay time constants
would vary from 2 to 30 msec at body temperature. Simulation studies of
Wang and Buzsáki (1996) used connected basket cells to model an
interneuron network. The critical decay time constant for generating 40 Hz oscillations was estimated to be ~10 msec (also see Traub et al.,
1996 ). This matches the most frequently occurring sIPSC decay kinetics,
between 16 and 20 msec at room temperature. Furthermore, in a
morphologically identified hilar basket cell, all properties of sIPSCs
(amplitude, rise time, and T50%) had very similar distributions to
those found in O-LM cells or in the bistratified cell (data not shown),
raising the possibility of such network activity among basket cells. In contrast to events with decay time constants in the 16-20 msec range,
the fast (8-10 msec) and the much slower (30-80 msec) IPSCs at room
temperature (i.e., 2-3 and 15-25 msec at 37°C) may serve as
clockworks for the ultrafast (200 Hz) and theta (4-7 Hz) oscillation patterns (Buzsáki et al., 1983 , 1992 ; Buzsáki and Chrobak,
1995 ; Cobb et al., 1995 ), respectively.
In conclusion, the high variability of sIPSCs kinetics may ensure the
basis for modulating network oscillations at different frequencies. The
synaptic interactions among interneurons are highly diverse but cannot
be adequately resolved unless the physiological findings are always
accompanied by detailed anatomical identification of the recorded
interneurons.
FOOTNOTES
Received April 21, 1997; revised Aug. 12, 1997; accepted Aug. 15, 1997.
This work was supported by National Institutes of Health Grants NS
27528 and NS 30549 to I.M. N.H. was also supported by OTKA (F17115). We thank Drs. T. F. Freund and S. R. Williams for
critical comments on this manuscript, Dr. C. R. Houser for
allowing us to use the camera lucida, and Brian K. Oyama and Michael T. Kim for excellent technical assistance.
Correspondence should be addressed to Dr. Istvan Mody, Departments of
Neurology and Physiology, Reed Neurological Research Center, University
of California Los Angeles School of Medicine, 710 Westwood Plaza, Los
Angeles, CA 90095-1769.
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