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The Journal of Neuroscience, September 1, 1999, 19(17):7334-7341
High Conductance Sustained Single-Channel Activity Responsible
for the Low-Threshold Persistent Na+ Current in Entorhinal
Cortex Neurons
Jacopo
Magistretti1, 2,
David S.
Ragsdale1, and
Angel
Alonso1
1 Department of Neurology and Neurosurgery, Montreal
Neurological Institute, McGill University, H3A 2B4, Montreal, Quebec,
Canada, and 2 Laboratorio di Biofisica e Neurofisiologia
dei Sistemi Corticali, Dipartimento di Neurofisiologia Sperimentale,
Istituto Nazionale Neurologico "Carlo Besta", 20133 Milano,
Italy
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ABSTRACT |
Stellate cells from entorhinal cortex (EC) layer II express both a
transient Na+ current
(INa) and a low-threshold persistent
Na+ current (INaP)
that helps to generate intrinsic theta-like oscillatory activity. We
have used single-channel patch-clamp recording to investigate the
Na+ channels responsible for
INaP in EC stellate cells. Macropatch (more
than six channels) recordings showed high levels of transient Na+ channel activity, consisting of brief openings
near the beginning of depolarizing pulses, and lower levels of
persistent Na+ channel activity, characterized by
prolonged openings throughout 500 msec long depolarizations. The
persistent activity contributed a noninactivating component to averaged
macropatch recordings that was comparable with whole-cell
INaP in both voltage dependence of
activation (10 mV negative to the transient current) and amplitude (1%
of the transient current at 20 mV). In 14 oligochannel (less than six
channels) patches, the ratio of transient to persistent channel
activity varied from patch to patch, with 10 patches exhibiting exclusively transient openings and one patch showing exclusively persistent openings. In two patches containing only a single persistent channel, prolonged openings were observed in >50% of test
depolarizations. Moreover, persistent openings had a significantly
higher single-channel conductance (19.7 pS) than transient openings
(15.6 pS). We conclude that this stable high-conductance persistent
channel activity is responsible for INaP in
EC stellate cells. This persistent channel behavior is more enduring
and has a higher conductance than the infrequent and short-lived
transitions to persistent gating modes that have been described
previously in brain neurons.
Key words:
Na+ channel; persistent Na+
current; patch clamp; single-channel recording; rat; entorhinal cortex; stellate cells; temporal lobe
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INTRODUCTION |
The familiar role for voltage-gated
Na+ channels is in the generation of the
transient Na+ current
(INa) responsible for the initiation
and propagation of action potentials. However, many mammalian brain
neurons also exhibit a low-voltage-activated, slowly inactivating
"persistent" Na+ current
(INaP), that contributes to
oscillatory activity (Alonso and Llinás, 1989 ; Silva et al.,
1991 ), boosting of synaptic potentials (Stuart and Sakmann, 1995 ), and
firing-pattern shaping (Llinás and Sugimori, 1980 ; Klink and
Alonso, 1993 ; Franceschetti et al., 1995 ; Parri and Crunelli, 1998 ; for
review, see Crill, 1996 ). INaP has
also been linked to the pathophysiology of epilepsy (Segal, 1994 ) and
other neurological diseases (Stys et al., 1993 ). Thus, it may be an
important target for the development of new pharmacological agents
(Taylor, 1993 ).
Despite its critical role in brain function, the biophysical and
molecular bases of INaP have remained
elusive. One widely held hypothesis is that
INaP is caused by rare,
short-lived transitions of conventional transient
Na+ channels to a slowly inactivating
gating mode (Alzheimer et al., 1993 ; Segal and Douglas, 1997 ). In
multichannel patches from sensorimotor cortex neurons, this slow-mode
gating was characterized by sustained bursts of channel activity in
~1% of depolarizing test pulses (Alzheimer et al., 1993 ). In
contrast, other single-channel studies in brain neurons (Masukawa et
al., 1991 ; Sugimori et al., 1994 ) have suggested the presence of a more
stable persistent channel activity. However, these studies did not give
a detailed analysis of this single-channel behavior. Furthermore, an
important element missing from previous studies has been direct
evidence that persistent single-channel openings recorded in patches
sum to give the low-threshold persistent
Na+ currents observed in whole-cell recordings.
A key population of neurons in the temporal lobe, the stellate cells of
entorhinal cortex (EC) layer II, possess a robust INaP (Alonso and Llinás, 1989 ;
Klink and Alonso, 1993 ; Magistretti and Alonso, 1999 ). This persistent
Na+ current generates intrinsic pacemaker
activity that is thought to contribute to the genesis of the limbic
theta rhythm (Bland, 1986 ; Alonso and García-Austt, 1987 ;
Alonso and Llinás, 1989 ), a brain rhythm that has been implicated
in memory function (Winson, 1978 ; Holscher et al., 1997 ). The
oscillatory properties of EC stellate cells may also play a role in
temporal lobe epileptogenesis (Dickson and Alonso, 1997 ; Klink and
Alonso, 1997 ). In this study, we investigated the
Na+ channels responsible for
INaP in EC stellate cells using
single-channel patch-clamp electrophysiological recording. In
cell-attached patches, we identified Na+
channel activity that was characterized by repeated prolonged openings
throughout 500-msec-long sweeps. In patches showing persistent activity, prolonged openings were observed in >50% of test
depolarizations. Furthermore, persistent channel activity displayed a
higher single-channel conductance than transient
Na+ channel activity in the same neurons.
Ensemble averages of persistent activity gave a persistent
Na+ current with an amplitude and voltage
dependence similar to whole-cell INaP.
We conclude that this stable high-conductance persistent channel
activity is responsible for INaP in
stellate cells of entorhinal cortex.
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MATERIALS AND METHODS |
Preparation of acutely dissociated neurons. The
procedure for acute isolation of EC layer II neurons was as described
previously (Magistretti and de Curtis, 1998 ). Briefly, male Long-Evans
rats [postnatal day 25 (P25) to P35] were decapitated, and the
brains were quickly removed, submerged into ice-cold dissociation
buffer [in mM: 115 NaCl, 3 KCl, 3 MgCl2, 0.2 CaCl2, 25 glucose, and 20 PIPES, pH 7.0, bubbled with
O2], and 400-µm-thick coronal slices were cut
with a vibratome. Using a fine scalpel, pieces of entorhinal cortex
layer II were dissected and transferred to dissociation buffer at
32°C. Protease type XIV (1 mg/ml; Sigma-Aldrich, Oakville, Ontario,
Canada) was added, and the pieces of brain tissue were incubated for 15 min with gentle agitation. The tissue was washed with dissociation
buffer, left at room temperature for 1 hr, and then dissociated by
trituration through Pasteur pipettes with fire-polished tips of
progressively smaller inner diameter. Suspensions of dissociated cells
were transferred to a recording chamber for electrophysiological experiments.
Electrophysiological recordings.
Na+ currents were recorded from acutely
dissociated neurons using the patch-clamp recording technique (Hamill
et al., 1981 ) in the whole-cell and cell-attached configurations. In
whole-cell experiments, cells were perfused with a solution containing
(in mM): 100 NaCl, 40 TEA-Cl, 10 HEPES, 2 CaCl2, 3 MgCl2, 0.2 CdCl2, 5 4-aminopyridine (4-AP), and 25 glucose,
pH 7.4. The pipette solution contained (in
mM): 110 CsF, 10 HEPES, 11 EGTA, and 2 MgCl2, pH 7.25. Whole-cell patch pipettes had a
resistance of 2-4 M when filled with this solution. Recordings were
performed with an Axopatch 1D amplifier and pCLAMP software (Axon
Instruments, Foster City, CA). Series resistance (6.5-14.0 M ) was
compensated by ~80%. All experiments were performed at room
temperature (23 ± 1°C). Persistent
Na+ currents were isolated by off-line
subtraction of current traces recorded after application of 1 µM TTX.
In single-channel experiments, cells were initially perfused with a
solution containing (in mM): 140 NaCl, 5 KCl, 10 HEPES, 2 CaCl2, 2 MgCl2, and 25 glucose, pH 7.4. The pipette solution contained (in mM):
130 NaCl, 35 TEA-Cl, 10 HEPES, 2 CaCl2, 2 MgCl2, and 5 4-AP, pH 7.4. Single-channel patch
pipettes had resistances ranging from 10 to 35 M when filled with
this solution. After obtaining the cell-attached configuration, the
extracellular perfusion was switched to a high-potassium solution
containing (in mM): 140 K-acetate, 5 NaCl, 10 HEPES, 4 MgCl2, 0.2 CdCl2, and 25 glucose, pH 7.4, to hold the neuron resting membrane potential at near 0 mV. Recordings were performed at room temperature with an Axopatch 200B amplifier (Axon Instruments). Capacitive transients were minimized with the built-in compensation circuitry of the
amplifier. Holding potential was 100 or 120 mV. Depolarizing
voltage steps were delivered at 5 sec intervals. Current signals were
low-pass filtered at 5 or 2 kHz and digitized at 100 or 10 kHz when
acquiring 50 or 500 msec sweeps, respectively. For single-channel
analysis, residual capacitive transients and leak currents were
nullified by off-line subtraction of fits of averaged blank traces.
Persistent single-channel open probability
(Po) was estimated, in both single sweeps and ensemble average traces, according to
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where Iavg is the average
current level over the last 455 msec of 500 msec test pulses,
N is the number of persistent channels in the patch
estimated from the maximum number of superimposed openings, and
i is the single-channel current amplitude.
Mean values in the text are presented ±SD. Statistical
significance of differences between groups were assessed with
Student's t test. All chemicals were obtained from
Sigma-Aldrich.
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RESULTS |
Whole-cell Na+ currents in EC stellate cells
show transient and persistent components
Figure 1 illustrates the properties
of whole-cell Na+ currents in EC stellate
cells. In whole-cell recordings, the predominant Na+ current evoked by membrane
depolarization was a transient current (INa), which rose rapidly to a peak
and then decayed to near baseline within a few milliseconds (Fig.
1A). The current-voltage
(I-V) relationship of
INa showed a threshold at
approximately 50 mV and a peak at approximately 20 mV (Fig.
1C, ). The decay phase of the current was best fit by the
sum of two exponential functions (typical fits are shown in Fig.
1A, insets), with a prominent fast
component that was strongly voltage-dependent over test potentials ranging from 50 to 5 mV (Fig. 1D). In addition to
this transient Na+ current, depolarizing
voltage steps also elicited a long-lasting, or persistent,
Na+ current
(INaP) (Fig. 1B).
The I-V relationship for
INaP was shifted ~10 mV negative
compared with INa (Fig. 1C,
), similar to previously described persistent
Na+ currents in brain neurons (French et
al., 1990 ). Also in agreement with previous findings, the amplitude of
INaP at 20 mV was 0.94 ± 0.82% of the peak current (n = 8). One micromolar TTX
abolished both INa and
INaP, indicating that both currents
were mediated by TTX-sensitive voltage-gated
Na+ channels. A TTX-sensitive
INaP of approximately the same
relative amplitude and with the same biophysical characteristics was
also recorded in EC layer II neurons in situ (data not
shown; but see Magistretti and Alonso, 1999 ).

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Figure 1.
Whole-cell INa and
INaP in EC layer II principal neurons.
A, Whole-cell Na+ currents elicited
in a representative neuron by depolarizing steps to potentials ranging
from 60 to 5 mV, in 5 mV increments. The holding potential was 80
mV. Calibration: 300 pA, 5 msec. The insets show current
traces at the test potentials of 50, 40 (top inset),
and 20 (bottom inset) mV, along with biexponential
fits (superimposed lines) of current decay. Time
constants for the fast and slow components of current decay were as
follows: 50 mV, f = 8.51 msec,
s = 20.12 msec; 40 mV, f = 3.5 msec, s = 14.34 msec; 20 mV,
f = 0.69 msec, s = 3.61 msec.
Calibration: top inset, 100 pA, 5 msec;
bottom inset, 300 pA, 5 msec. B,
INaP recorded, at higher gain, in a
different neuron. Depolarizing pulses were from 50 to 25 mV in 5 mV
steps, from a holding potential of 80 mV. Calibration: 25 pA, 50 msec. C, Mean current-voltage relationships for
INa ( ; n = 8) and
INaP ( ; n = 5).
INa amplitudes were measured at the current
peak. INaP amplitudes were derived by
averaging the data points between 400 and 500 msec from the start of
each test pulse. In this and subsequent figures, symbols and error bars
show means ± SD. D, Mean values for the fast
inactivation time constant ( f) for
INa (n = 7), plotted as
a function of test potential.
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Macropatches exhibit both transient and persistent
Na+ channel activity
To determine the properties of the channels responsible
for whole-cell INa and
INaP, we examined
Na+ channel behavior in patch-clamp
experiments in stellate cell somata, using the cell-attached recording
configuration. Na+ channel activity was
recorded in 67 of 68 patches. Most patches (n = 52)
contained more than six channels, as judged by the maximal number of
superimposed channel openings. Figure 2
shows an example of Na+ channel activity
in one of these "macropatch" experiments in response to 50 (Fig.
2A) or 500 (Fig. 2B) msec
depolarizing test pulses. A depolarizing step elicited a large
transient inward current in the first few milliseconds after the start
of the test pulse because of the superimposed opening of rapidly
activating and inactivating transient Na+
channels (Fig. 2A). When many consecutive traces were
averaged (Fig. 2A, inset), the transient
channel activity produced a transient ensemble current that
closely resembled INa recorded in
whole-cell experiments, in terms of both time course (Fig.
2A, inset, D) and
I-V relationship (Fig. 2C, ).

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Figure 2.
Na+ channel activity in
macropatch recordings. A, Na+ channel
currents evoked by consecutive 50 msec depolarizing pulses to 20 mV.
Calibration: 2 pA, 5 msec. The inset shows an ensemble
current trace obtained from the averaging a set of 20 consecutive
traces. The decaying phase of the ensemble current is fit with a
biexponential function with time constants f = 0.71 msec and s = 3.29 msec. Calibration:
inset, 2 pA, 5 msec. B, Consecutive
traces in the same patch as in A, elicited by 500 msec
depolarizing pulses to 30 mV. Calibration: 2 pA, 50 msec. The
inset shows the average of a set of 20 consecutive
traces, displayed at a high amplification, to illustrate the persistent
component of the ensemble current. Calibration: inset,
0.2 pA, 50 msec. C, Mean current-voltage relationships
for the transient ( ; n = 7) and persistent ( ;
n = 7) components of ensemble currents.
D, Mean f for ensemble transient
currents, plotted as a function of test potential. E,
Voltage dependence of persistent single-channel current amplitude. Only
openings occurring at least 20 msec after the start of the test pulse
were considered. Data points are from eight patches. In this and
subsequent single-channel I-V plots, the
straight line is a linear least squares fit of the mean
data points, with the slope conductance value given in the graph,
whereas conductance values reported in Results are means of slope
conductances determined for each individual experiment.
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In addition to the transient channel activity, test pulses in
macropatch experiments also elicited a lower level of sustained channel
activity, characterized by repeated episodes of prolonged openings
throughout even long-lasting depolarizations (Fig.
2B). These "persistent" channel openings were
observed in most sweeps in 16 of 20 macropatches in which we were able
to determine channel behavior using an extended series of 500-msec-long
test pulses. Ensemble averages of the late openings produced a
measurable persistent current (Fig.
2A,B, insets) that
closely resembled whole-cell INaP in
terms of both voltage-dependence of activation and relative amplitude.
The mean I-V relationship for ensemble persistent currents (Fig. 2C, ) was similar to that determined from
whole-cell recordings of INaP, and,
like INaP versus
INa, was shifted by ~10 mV in the negative direction with respect to the mean I-V
relationship of ensemble transient currents (Fig. 2C, ).
In addition, the mean amplitude of the persistent component in ensemble
current traces at 20 mV was 0.90 ± 0.71% (n = 20) of the peak amplitude of the transient component, a percentage very
similar to that of INaP versus
INa in whole-cell recordings. In 10 of
10 experiments, both transient and persistent single-channel currents
were absent when 1 µM TTX was included in the
patch pipette (data not shown), indicating that both types of channel
behavior were caused by TTX-sensitive Na+
channels. Together, these data indicate that the noninactivating channel activity recorded in macropatches was responsible for whole-cell INaP. The single-channel
conductance determined for late channel openings in eight macropatches
was 19.3 ± 2.3 pS (Fig. 2E).
Single Na+ channels exhibit distinct transient
and persistent gating behaviors
A more limited number of patches (n = 14)
contained from two to five channels. Ten of these "oligochannel"
patches exhibited exclusively transient channel activity. The voltage-
and time-dependent behavior of these transient single-channel currents
was similar to the typical transient Na+
channels that have been described previously in neurons (Fig. 3A) (Aldrich et al., 1983 ;
Kirsch and Brown, 1989 ; Alzheimer et al., 1993 ; Magee and Johnston,
1995 ). Ensemble currents decayed according to single exponential
functions, with time constants similar to the fast time constants
determined for both average transient currents of macropatches and
whole-cell INa (Fig. 3A, insets, C). In transient channel patches, late
channel activity was rarely observed and was almost entirely limited to
brief, infrequent reopenings (Fig.
3A,B). Furthermore, ensemble
currents did not show any detectable persistent component (Fig.
3A, insets), consistent with the idea that these
rare reopenings were not responsible for
INaP in EC neurons. The mean slope
conductance of fast channel activity was 15.6 ± 1.7 pS (Fig.
3D). This conductance is similar to the values reported
previously for transient Na+ channels in
various CNS neuron types (Kirsch and Brown, 1989 ; Alzheimer et al.,
1993 ; Magee and Johnston, 1995 ) but statistically significantly
different (p < 0.005) from the conductance of
late channel openings in multichannel patches.

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Figure 3.
Single-channel currents in oligochannel patches
showing exclusively transient activity. A,
Na+ channel currents evoked by 50 msec depolarizing
pulses to 40 or 20 mV in a patch containing at least three
transient Na+ channels. Calibration: 2 pA, 5 msec.
Insets show ensemble currents from 20 consecutive
traces, along with single exponential fits of the current decay. Time
constants were 2.55 ( 40 mV) and 0.84 ( 20 mV) msec. Calibration:
inset, 0.5 pA, 2 msec. B, Current traces
elicited by consecutive 500 msec depolarizing pulses to 30 mV in the
same patch as in A. Calibration: 2 pA, 50 msec.
C, Mean values for inactivation time constants,
determined by exponential fits of ensemble currents from eight patches
containing only transient Na+ channels. The data
were plotted as a function of test potential. D, Voltage
dependence of transient single-channel current amplitude. To ensure
that conductance measurements were not distorted by brief openings that
are truncated because of the low-pass filter, only unequivocal, square
single-channel openings, such as those indicated by
arrows in A, were considered for these
measurements. Data points are from seven patches.
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Four oligochannel patches showed persistent
Na+ channel activity. For example, Figure
4A shows consecutive
sweeps from a patch that contained five channels (based on the maximum
number of superimposed openings) and showed a high level of persistent
behavior. Persistent single-channel activity was observed in this patch
at test potentials as negative as 60 mV at which it appeared as
intensely flickering and incompletely resolved openings (Fig.
4A, left traces). With stronger
depolarizations, channels exhibited repeated prolonged openings that
sometimes lasted for the entire duration of 500-msec-long test pulses
(Fig. 4A, right traces). When traces from
this experiment were averaged (Fig. 4A,
insets), the ensemble currents showed a rapid activation
time course, followed by a very slow rate of inactivation, with a
prominent persistent component at the end of the 500-msec-long test
pulse. The absence of any detectable transient component in the
ensemble traces (Fig. 4A, inset)
argues that there was little or no transient activity in this patch. A
transient component to the ensemble currents would be expected if most
sweeps were a mixture of transient and persistent single-channel currents (Fig. 5A). The high
level of persistent gating behavior throughout this experiment is also
illustrated in Figure 4B, which shows the estimated
single-channel open probability, Po
(determined as described in Materials and Methods), plotted for
consecutive 500-msec-long sweeps, over a range of test potentials.
Po values were high for every sweep,
indicating that a high level of persistent channel activity was present
throughout the entire 17-min-long experiment. Together, these results
indicate that Na+ channels in stellate
cells could exhibit high levels of persistent activity with little or
no transient activity for prolonged periods of time.

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Figure 4.
Single-channel currents in a patch exhibiting a
high level of persistent activity. A,
Na+ channel currents evoked by consecutive 500 msec
depolarizing pulses to 60 or 10 mV. Calibration: 2 pA, 50 msec.
Insets show ensemble average currents obtained from sets
of 20 consecutive sweeps. Calibration: right inset, 0.5 pA, 50 msec; left inset, 1 pA, 50 msec.
B, Plot of Po for individual
500-msec-long test pulses in the same experiment as in
A. Each bar corresponds to a single
sweep. The test-potential levels are depicted in the
top. The omitted time interval corresponds to recordings
at more negative test potentials ( 50 to 80 mV).
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Figure 5.
Single-channel currents in a patch containing both
a persistent Na+ channel and a transient
Na+ channel. A, Consecutive sweeps
recorded in response to 500 msec depolarizing pulses to -20 mV.
Calibration: 1 pA, 50 msec. Inset, Ensemble current
obtained from a set of 20 consecutive traces. Calibration:
inset, 0.2 pA, 50 msec. B,
Po values per sweep for the experiment shown
in A. C, Mean voltage dependence of persistent
single-channel current amplitude determined from four persistent
Na+ channel patches.
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Figure 5A shows consecutive sweeps at 20 mV from a
different experiment that illustrates the properties of a single
Na+ channel exhibiting persistent
behavior. This patch contained two channels and displayed both
transient and persistent openings in most sweeps. It is most probable
that the persistent activity in this patch was mediated by only one of
the two channels. The alternative possibility is that the two channels
in the patch were independently switching between transient and
persistent gating during the experiment, and thus a different channel
was mediating persistent openings from one sweep to the next. However, this explanation is unlikely, because we never observed sweeps consisting of overlapping persistent openings, as would be likely to
occur if both channels had by chance simultaneously switched to
persistent gating. Figure 5B shows a diary plot of
Po per sweep for the persistent
channel over the course of the 12-min-long experiment. The values were
determined from 5 to 500 msec after the start of the test pulse to
exclude the transient channel activity, which was clustered near the
beginning of each depolarization. Po
values were between 0.1 and 0.9 in most sweeps, reflecting the robust
persistent activity in this patch throughout the entire experiment.
Persistent openings (defined as openings of at least 25 msec in
duration) were observed in 54 of 100 test pulses. In a second patch
with only one persistent channel, persistent openings were seen in 48 of 80 sweeps. These experiments demonstrate that single
Na+ channels could exhibit high levels of
persistent gating behavior for prolonged periods of time.
Po at 20 mV was 0.170 for the channel shown in
Figure 5 and 0.176 ± 0.139 for all four persistent oligochannel patches.
The average slope conductance of persistent
Na+ currents in oligochannel patches was
20.7 ± 1.1 pS (n = 4) (Fig. 5C). These data were pooled with the conductance for sustained currents in macropatches to give a mean slope conductance for persistent
Na+ channels of 19.7 ± 2.1 pS
(n = 12). This conductance value is statistically
significantly higher than the mean conductance of 15.6 pS for fast
Na+ channels in EC neurons
(p < 0.0005) and higher than values typically reported for neuronal Na+ channels in
other single-channel studies (Kirsch and Brown, 1989 ; Alzheimer et al.,
1993 ; Magee and Johnston, 1995 ).
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DISCUSSION |
The entorhinal cortex, hippocampal formation, and perirhinal
cortex form a medial temporal lobe memory system that is critical for
early stages of declarative memory formation (Scoville and Milner,
1957 ; Squire and Zola, 1996 ). The entorhinal cortex has a key
location within this circuitry (Suzuki and Amaral, 1994 ). Multimodal
sensory information from various regions of neocortex converge on EC
layers II and III, which then convey this information to the dentate
gyrus of the hippocampal formation by way of the perforant path.
Hippocampal outputs, primarily from CA1 and subiculum, project to EC
layers V-VI, which in turn send outputs that reciprocate the
neocortical inputs to the entorhinal cortex. In addition, EC layers
V-VI project to superficial EC layers, closing an EC-hippocampal loop. Layer II stellate cells, the focus of this study, are a major
group of glutamatergic projection neurons that contribute to the
perforant path connecting entorhinal cortex to the hippocampus. A
striking intrinsic property of stellate cells is that they are capable
of generating sustained 5-10 Hz subthreshold oscillations in membrane
potential (Alonso and Llinás, 1989 ). These subthreshold oscillations are proposed to play a role in the genesis of the temporal
lobe theta rhythm, which is thought to be important for binding of
polymodal information from different cortical regions (Winson, 1978 ;
Holscher et al., 1997 ). Furthermore, the intrinsic oscillatory behavior
of entorhinal cortex neurons, combined with the reverberatory and
highly plastic nature of the EC-hippocampal circuitry may contribute
to epileptogenesis in the temporal lobe (Dickson and
Alonso, 1997 ; Klink and Alonso, 1997 ). Previous work has shown that
INaP contributes to the depolarizing
phase of stellate cell oscillations, whereas the repolarizing phase of
the oscillations is attributable to the deactivation of a
hyperpolarization-activated cation current
(Ih) (Alonso and Llinás, 1989 ;
Dickson and Alonso, 1998 ).
Our results show that INaP in EC
stellate cells is caused by Na+ channel
behavior that is distinguished from conventional transient Na+ channel activity responsible for
INa by a sustained, high open probability throughout long depolarizations, as well as a significantly higher single-channel conductance. In patches containing persistent channel activity, prolonged late openings were seen in the majority of
sweeps throughout experiments lasting up to 17 min. In macropatch recordings, which give an approximation of the channels in the whole-cell soma, persistent Na+ channel
openings represented a small fraction of the total
Na+ channel activity. However, this
persistent channel activity contributed a persistent component to
ensemble currents that was comparable with whole-cell
INaP in both voltage dependence of
activation (10 mV more negative than the transient current) and
amplitude (~1% of the transient current at 20 mV). The observation
that averaged macropatch recordings can accurately reproduce both the transient and persistent components of whole-cell
Na+ currents supports the hypothesis that
the persistent Na+ channel activity
detected in these patches is responsible for whole-cell
INaP in stellate cells. This
persistent channel behavior is responsible for the emergence of a
cellular property, theta subthreshold oscillations, which is implicated
in governing the population behavior of the entorhinal-hippocampal network.
Biophysical mechanisms for INaP in brain neurons
A number of hypotheses have been proposed to explain persistent
Na+ currents. For example, it has been
suggested that INaP results from a
window current attributable to the overlap between channel steady-state
activation and inactivation (Attwell et al., 1979 ) or from slow
closed-state inactivation at intermediate membrane potentials (Cummins
et al., 1998 ). One widely held hypothesis is that
INaP results from transitions of
conventional transient Na+ channels to
noninactivating gating modes. Slow-mode gating of Na+ channels was first observed in heart
(Patlak and Ortiz, 1985 ) and skeletal muscle (Patlak and Ortiz, 1986 )
and in Xenopus oocytes expressing cloned
Na+ channel subunits (Moorman et al.,
1990 ; Zhou et al., 1991 ). Subsequently, several studies have
demonstrated that transient Na+ channels
in brain neurons can also switch to slow gating modes (Alzheimer et
al., 1993 ; Segal and Douglas, 1997 ). However, in these studies,
transitions to slow gating behavior were extremely rare and short-lived
events. For example, in multichannel patches from neocortex neurons,
bursts of persistent activity were observed in only 1% of test
depolarizations (Alzheimer et al., 1993 ). Compared with this type of
channel behavior, the persistent activity that we observed in stellate
cells was much more stable. For example, in the two patches containing
only a single persistent Na+ channel, we
observed prolonged openings in >50% of test depolarizations. Furthermore, the persistent channel activity in stellate cells had a
higher single-channel conductance than the transient channel activity,
whereas previously described persistent gating modes had the same
conductance as transient openings (Alzheimer et al., 1993 ). Other
single-channel studies have suggested that a similar type of stable
persistent Na+ channel activity may be
responsible for INaP in cultured
hippocampal neurons (Masukawa et al., 1991 ) and cerebellar Purkinje
cells (Sugimori et al., 1994 ), although in Purkinje cells, the reported single-channel conductance was only 7 pS. Thus, stable persistent Na+ channel activity may be a widespread
mechanism for generating INaP in brain
neurons. The results presented here add to these previous
single-channel studies in several ways. First, we describe persistent
activity that is stable throughout long experiments. Second, we
demonstrate that this persistent activity has a higher single-channel
conductance than transient activity. Third, we show that persistent
activity can sum to give the low-threshold persistent
Na+ current seen in whole-cell recordings.
Intracellular application of proteolytic enzymes can destroy sodium
channel inactivation (Armstrong et al., 1973 ). Thus, it may be argued
that the persistent channel activity described in this study resulted
from the proteolytic treatment used to dissociate EC neurons. However,
several observations argue against this explanation. First, in
whole-cell recordings of stellate cells in slices, we observed
persistent sodium currents with the same relative amplitude and the
same biophysical properties as the whole-cell persistent sodium
currents in dissociated stellate cells (Magistretti and Alonso, 1999 ).
This finding indicates that persistent sodium currents in dissociated
cells are not a consequence of the dissociation procedure. Second,
persistent single-channel activity in stellate cells exhibited a
single-channel conductance that was significantly higher than the
conductance of the transient activity. In contrast, moderate
intracellular proteolytic treatment does not typically result in
changes in single-channel conductance (Cukierman, 1991 ; Valenzuela and
Bennett, 1994 ).
Molecular basis for persistent Na+
channel activity
Although we do not know the molecular basis for persistent
Na+ channel activity in EC stellate cells,
we can envision a number of plausible hypotheses. At one extreme,
transient and persistent activity could be caused by distinct
Na+ channel isoforms. Alternatively, the
same channels could mediate both transient and persistent activity,
perhaps with channel kinetics and conductance regulated by
phosphorylation, auxiliary subunits, or some other type of
long-lasting modulation. In between these two extremes is the
possibility that some types of transient
Na+ channels may be particularly
predisposed to modulation to persistent gating modes, whereas others
are more dedicated to transient gating.
Brain Na+ channels consist of a
pore-forming subunit that associates with two smaller auxiliary
subunits, designated 1 and 2 (for review, see Ragsdale and Avoli,
1998 ). The subunit is the main molecular determinant of
Na+ channel behavior. Brain neurons
express multiple subunit isoforms, encoded by at least four genes,
designated Scn1a, Scn2a, Scn3a, and Scn8a. Preliminary results using
reverse transcription-PCR suggest that subunits encoded by
all four of these genes are expressed in cells from adult rat
entorhinal cortex (L. Meadows, J. Magistretti, A. Alonso, and D. S. Ragsdale, unpublished observations). Thus, subunits
encoded by one of these genes could mediate persistent channel activity
(Joho et al., 1990 ; Raman et al., 1997 ; Smith and Goldin, 1998 ; Smith
et al., 1998 ). Alternatively, persistent activity could be mediated by
a novel subunit isoform that has yet to be cloned and/or yet to be
functionally characterized. Other possible explanations for persistent
activity include modulation of channel function by subunits (Isom
et al., 1992 ), phosphorylation (Numann et al., 1991 ), or direct
G-protein interactions (Ma et al., 1997 ). Ultimately, the molecular
basis for persistent Na+ currents will
most likely be determined using expression of cloned Na+ channel subunits in heterologous cell
systems. The findings presented in this study provide new functional
data in brain neurons against which these subsequent molecular analyses
will need to be compared and evaluated.
 |
FOOTNOTES |
Received April 14, 1999; revised June 17, 1999; accepted June 18, 1999.
This work was supported by grants from the Medical Research Council of
Canada (MRC) and the Human Frontier Science Program Organization
(HFSPO) to A.A. and grants from the MRC and the Natural Science and
Engineering Research Council of Canada to D.R. J.M. thanks Dr. M. de Curtis, the Instituto Nazionale Neurologico "C. Besta", and the
HFSPO for support.
Correspondence should be addressed Dr. David S. Ragsdale, Department of
Neurology and Neurosurgery, Montreal Neurological Institute, McGill
University, 3801 University Street, Montreal, Quebec, H3A 2B4, Canada.
 |
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