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The Journal of Neuroscience, May 1, 2002, 22(9):3645-3655
Upregulation of a T-Type Ca2+ Channel Causes a
Long-Lasting Modification of Neuronal Firing Mode after Status
Epilepticus
Hailing
Su1, *,
Dmitry
Sochivko3, *,
Albert
Becker2,
Jian
Chen3,
Yanwen
Jiang1,
Yoel
Yaari1, and
Heinz
Beck3
1 Department of Physiology, Hebrew University-Hadassah
School of Medicine, 91120 Jerusalem, Israel, and Departments of
2 Neuropathology and 3 Epileptology, University
of Bonn Medical Center, D-53105 Bonn, Germany
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ABSTRACT |
A single episode of status epilepticus (SE) causes numerous
structural and functional changes in the brain that can lead to the
development of a chronic epileptic condition. Most studies of this
plasticity have focused on changes in excitatory and inhibitory synaptic properties. However, the intrinsic firing properties that
shape the output of the neuron to a given synaptic input may also be
persistently affected by SE. Thus, 54% of CA1 pyramidal cells, which
normally fire in a regular mode, are persistently converted to a
bursting mode after an episode of SE induced by the convulsant
pilocarpine. In this model, intrinsic bursts evoked by
threshold-straddling depolarizations, and their underlying spike
afterdepolarizations (ADPs), were resistant to antagonists of N-, P/Q-,
or L-type Ca2+ channels but were readily suppressed
by low (30-100 µM) concentrations of
Ni2+ known to block T- and R-type
Ca2+ channels. The density of T-type
Ca2+ currents, but not of other pharmacologically
isolated Ca2+ current types, was upregulated in CA1
pyramidal neurons after SE. The augmented T-type currents were
sensitive to Ni2+ in the same concentration range
that blocked the novel intrinsic bursting in these neurons
(IC50 = 27 µM). These data suggest that SE may persistently convert regular firing cells to intrinsic bursters
by selectively increasing the density of a
Ni2+-sensitive T-type Ca2+
current. This nonsynaptic plasticity considerably amplifies the output
of CA1 pyramidal neurons to synaptic inputs and most probably contributes to the development and expression of an epileptic condition
after SE.
Key words:
T-type Ca2+ channel; status
epilepticus; intrinsic burst discharge; plasticity; CA1; hippocampus
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INTRODUCTION |
Both in humans and in experimental
animals, continuous seizure activity as occurs during status
epilepticus (SE) results in a large number of plastic changes within
the hippocampus and adjacent brain areas (Coulter and DeLorenzo, 1999 ;
Sloviter, 1999 ; Ben Ari, 2001 ). The SE-induced modifications in
neuronal function may consist either of altered synaptic function or of
changes in the intrinsic membrane properties of neurons. Hitherto, a
multitude of structural and functional synaptic changes have been shown to follow SE, such as reorganization of excitatory axons (Sutula et
al., 1989 ), altered function of excitatory neurotransmitter receptors
(Turner and Wheal, 1991 ; Lothman et al., 1995 ; Chen et al., 1999 ), or
changes in GABAA receptor-mediated
inhibition (Mangan et al., 1995 ; Gibbs et al., 1997 ; Brooks-Kayal et
al., 1998 ; Cossart et al., 2001 ). Many of these synaptic changes have been suggested to contribute to the development of temporal lobe epilepsy (TLE) that is frequently the outcome of a single or multiple episodes of SE.
Much less is known about SE-induced changes in intrinsic neuronal
properties. However, a recent study in the pilocarpine model, in which
an episode of SE induced by the convulsant pilocarpine progresses to a
chronic epileptic condition resembling human TLE (Turski et
al., 1983 ), suggests that such alterations may be highly significant. In this model, Sanabria et al. (2001) found a marked upregulation of intrinsic neuronal bursting associated with the development of TLE. Although almost all pyramidal neurons in the hippocampal CA1 area are regular firing cells in normal conditions (Jensen et al., 1994 ), ~50% of CA1 pyramidal cells in hippocampal tissue removed from rats that experienced SE were found to be intrinsically burst-firing cells. Moreover, the upregulation of intrinsic bursting seemed to result from the de novo
appearance of Ca2+-dependent bursting that
is not ordinarily seen in this class of principal hippocampal neurons
(Azouz et al., 1996 ). It was also found that a subset of the newly
formed bursters, namely, the spontaneously bursting pyramidal cells,
acted as pacemakers of spontaneous interictal-like epileptiform bursts,
recruiting the entire CA1 population of pyramidal cells, nonbursters
and bursters alike, into synchronized discharge (Sanabria et al., 2001 ).
Because the switch in neuronal firing mode after SE may be
important for the development and expression of TLE, and because it may
represent a novel mechanism of activity-induced neuronal plasticity, we
have used a combination of electrophysiological and pharmacological
techniques to characterize in detail the ionic mechanisms underlying
the increased intrinsic bursting. Here we report that the dramatic
change in firing mode of CA1 neurons after SE is most probably caused
by the increased density of a Ni2+-sensitive T-type
Ca2+ current. Our findings demonstrate
that epilepsy-related changes in intrinsic neuronal properties may
result from activity-dependent differential regulation of specific ion
channel subtypes and suggest that subunit-selective T-type channel
antagonists may be promising future targets for rational anti-epileptic
drug design.
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MATERIALS AND METHODS |
Induction of SE. Experimental protocols were approved
by the local animal care and use committees. Male Sabra or Wistar rats (150-200 gm) were injected with a single high dose of the muscarinic agonist pilocarpine (300-380 mg/kg, i.p.), which induced SE in most
(~80%) animals. Peripheral muscarinic effects were reduced by
previous administration of methyl-scopolamine (1 mg/kg, s.c.; 30 min
before injection of pilocarpine). Diazepam (0.1 mg/kg, s.c.) was
administered to all animals 2 hr after the pilocarpine injection. It
terminated the convulsions in the responsive rats and sedated all
animals. Experiments were performed on hippocampal slices from rats
that experienced SE after pilocarpine injection (SE-experienced rats)
and from those that did not (sham-control rats). A third group of
untreated, age-matched rats served as an additional control
(naive-control rats). Previous work has found no differences in
electrophysiological properties between sham- and naive-control rats
(Sanabria et al., 2001 ).
Preparation of hippocampal slices and dissociated neurons.
Animals were decapitated under ether anesthesia 6-40 d after
pilocarpine treatment, and transverse hippocampal slices (250 or 400 µm) were prepared with a vibrating microslicer (Campden Instruments
or Leica) and transferred to a storage chamber perfused with oxygenated (95% CO2-5% O2)
artificial CSF (ACSF) containing (in mM):
NaCl 125, KCl 3, NaH2PO4
1.25, MgCl2 1, CaCl2 2, NaHCO3 25, and glucose 20, pH 7.4, osmolarity 305 mOsm, where they were maintained at room temperature. For
intracellular recordings, 400-µm-thick hippocampal slices were placed
in an interface chamber (33.5°C) and perfused with oxygenated ACSF
containing (in mM): NaCl 124, KCl 3.5, NaH2PO4 1.25, MgSO4 2, CaCl2 2, NaHCO3 26, and D-glucose
10. In experiments in which Ni2+ was used,
NaH2PO4 was omitted.
Ca2+ channel blockers, or the glutamate
receptor antagonists 6-cyano-7-nitro-quinoxaline-2,3-dione (CNQX) and
2-amino-5-phosphono-valeric acid (APV), were added to the ACSF as
indicated. For patch-clamp recordings in the slice preparation, 250 µM hippocampal slices were placed in a
submerged recording chamber (21-24°C) and perfused continuously (2.5 ml/min) with oxygenated ACSF containing (in mM):
NaCl 125, KCl 2.5, NaHCO3 26.7, CaCl2 2.5, MgCl2 1, HEPES
13, glucose 12.5, pH 7.3, osmolarity 300 mOsm. Pyramidal cells in the
CA1 field were visualized at 400× magnification with
Dodt-Gradient-Contrast optics (Luigs and Neumann) using a Zeiss
Axioskop microscope and an infra-red video camera (Hamamatsu,
Shizuoka, Japan).
Dissociated hippocampal neurons were prepared from 400-µm-thick
slices primarily as described previously (Beck et al., 1999 ). After an
equilibration period (>60 min), enzymatic digestion was performed for
10 min at 37°C and 5 min at room temperature in 5 ml of incubation
medium containing (in mM): sodium methanesulfonate 145, KCl
3, CaCl2 0.5, MgCl2 1, HEPES 10, glucose 15, and 2 mg/ml pronase (protease type XIV;
Sigma, St. Louis, MO) (pH 7.4, osmolarity 310 mOsm, 100%
O2). After washing with enzyme-free incubation medium, the CA1 region was dissected and triturated with fire-polished glass pipettes. The cell suspension was placed in a Petri dish and
superfused with modified ACSF containing (in mM): sodium
methanesulfonate 125, tetraethylammonium chloride (TEA) 20, 4-aminopyridine 4, BaCl2 5, MgCl2 1, KCl 3, glucose 10, HEPES 10, tetrodotoxin (TTX) 0.5 µM, pH 7.4, osmolarity 315 mOsm.
Cells were visualized on a inverted microscope (Zeiss Axiovert).
Sharp microelectrode recordings in slices. Intracellular
recordings were obtained using sharp glass microelectrodes containing 1 M K+-acetate (70-90
M ). An active bridge circuit in the amplifier (Axoclamp 2B, Axon
Instruments) allowed simultaneous injection of current and measurement
of membrane potential. The signals were filtered on-line at 5 kHz,
digitized at a sampling rate of 10 kHz, and stored on hard disk (TL-1
DMA and pClamp, Axon Instruments). In some experiments, bipolar
platinum (50 µm) electrodes connected to a stimulator by an isolation
unit were used for focal stimulation of afferent fibers in stratum
radiatum near the CA2/CA3 border (orthodromic stimulation).
Patch-clamp recordings in slices and dissociated neurons.
Recording patch pipettes (2-4 M ) were pulled from
borosilicate glass on a vertical puller (List-Medical or Narishige,
Tokyo, Japan). Pipettes were coated with Sylgard resin for
recordings in the slice preparation (Dow Corning Chemical) and filled
with an intracellular solution containing (in
mM): Cs-methanesulfonate 100, EGTA 5, HEPES 10, TEA 20, MgCl2 2, CaCl2 0.1, pH 7.35. For recordings from dissociated CA1 neurons, pipettes were
filled with (in mM): Cs-methanesulfonate 87.5, TEA 20, CaCl2 0.5, MgCl2 5, BAPTA 5, HEPES 10, glucose 10, Na+2-ATP
10, and GTP 0.5, pH 7.2 (NaOH), osmolarity adjusted to 300 mOsm with
sucrose. Tight-seal whole-cell recordings were obtained using a
patch-clamp amplifier (Axopatch 200A, Axon Instruments, or EPC9, HEKA
Instruments). The signals were collected on-line as described above.
Series resistance compensation was used to improve the voltage-clamp
control (60-85%) so that the maximal residual voltage error did not
exceed 5 mV. A liquid junction potential of ~10 mV was measured
between the intracellular and extracellular solutions and corrected
on-line.
Chemicals and drugs. In slice experiments the drugs were
applied via the perfusing ACSF. Application of drugs to dissociated neurons was performed via a pipette placed at a distance of 30-50 µm
from the cell body. All drugs were obtained from Sigma, except the
Ca2+ channel toxins (Bachem or Alomone
Labs) and CNQX (Tocris Neuroamin). Stock solutions of the toxins
(0.2-1 mM) were prepared in deoxygenated solution containing 0.1% BSA, 100 mM NaCl, 10 mM Trizma, 1 mM EDTA, pH
7.5. In experiments using the toxins, all solutions contained 0.1 mg/ml
cytochrome c to prevent unspecific peptide binding to tubing. Stock solutions (10 mM) of nifedipine and
nicardipine were prepared in DMSO.
Analysis. A measure for the size of the spike
afterdepolarization was provided by the area delimited by the ADP
waveform and resting membrane potential. The concentration-dependent
reduction of Ca2+ current amplitude was
fit with a modified Hill function of the form: E = Emax * cn/(cn + IC50n), where
E is the fraction of current blocked,
Emax corresponds to the maximal block,
c is the concentration of antagonist, n is the
Hill coefficient, and the IC50 is the
concentration at which half-maximal blocking effects were observed.
The decay of tail currents after mock action potentials was fit with a
biexponential equation of the form: I(t) = A1 * (1 exp( t/ f)) + A2 * (1 exp( t/ s)), where
I(t) is the current amplitude at the time point
t after onset of the voltage command, f and
s are the fast and slow decay time
constants, respectively, and A is the amplitude contribution
of the different time constants. Data were fit using a
Levenberg-Marquard nonlinear curve-fitting procedure.
Significant differences between groups were tested with a two-tailed
Student's t test with the significance level set to
p < 0.05.
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RESULTS |
Altered intrinsic bursting after pilocarpine-induced SE
First, we have replicated the recent findings of Sanabria et al.
(2001) , demonstrating enhanced bursting behavior in SE-experienced rats
compared with naive-control and sham-control animals, in a new set of
experiments. Sharp microelectrodes were used to impale CA1 pyramidal
cells and to stimulate them with threshold-straddling, long (200 msec)
and brief (4 msec) depolarizing current pulses (Azouz et al., 1996 ). In
both the naive-control (n = 15 cells; data not shown)
and sham-control (n = 42 cells) (Fig.
1A) groups, all except
one neuron fired a series of independent spikes in response to the long
pulse and a single spike in response to the brief pulse (Fig.
1Aa,B). The remaining neuron in each group
burst-fired in response to the long pulse. In marked contrast, more
than half of the CA1 neurons in the SE-experienced group (54%;
n = 97) generated a burst of action potentials as a
minimal response to threshold-straddling long current injections and in
many cases burst-fired also in response to brief stimulation (Fig.
1Ab,B). As expected (Sanabria et al.,
2001 ), the burst responses were unaffected by blocking synaptic
transmission with CNQX (15 µM), APV
(50 µM), and bicuculline methiodide (10 µM; n = 26). Thus, as described
previously, pilocarpine-induced SE triggers a long-lasting switch in
firing mode from a nonbursting to a bursting behavior in a large
fraction of CA1 pyramidal cells.

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Figure 1.
Upregulation of intrinsic burst-firing in CA1
pyramidal cells from SE-experienced versus control animals.
A, Representative responses of CA1 pyramidal cells from
sham-control (a) and SE-experienced animals
(b) 30 d after pilocarpine treatment. In
each panel, the responses of CA1 pyramidal cells to long
(leftmost traces) and brief (rightmost
traces) depolarizing current pulses (injected through the
recording microelectrode) are shown. Top and
bottom traces depict the neuronal response and the
current stimulus, respectively. B, Most of the CA1
pyramidal cells in the sham-control (n = 42) as
well as in the naive-control group (n = 15) were
regular firing cells, with only a small fraction displaying burst
discharges to threshold stimulation (white bars). In
contrast, CA1 pyramidal cells in the SE-experienced group showed a high
incidence of intrinsic bursting (54%, n = 97),
with bursting neurons displaying all-or-none bursts of three to four
clustered spikes in response to either brief or long current injection
(Ab).
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Critical role of Ni2+-sensitive
Ca2+ channels in SE-induced intrinsic bursting
Previous work has suggested that Ca2+
currents play a critical role in the SE-induced intrinsic bursting of
CA1 pyramidal cells (Sanabria et al., 2001 ). In normal tissue, CA1
pyramidal cells express multiple types of voltage-gated
Ca2+ channels, namely, L-, N-, P-/Q-, R-,
and T-types (Yaari et al., 1987 ; Takahashi et al., 1989 ; Fisher et al.,
1990 ; Thompson and Schwindt, 1991 ; Christie et al., 1995 ). To identify
the Ca2+ channel types that mediate
intrinsic bursting induced by SE, we have compared the effects of
selective organic Ca2+ channel blockers:
namely, nicardipine (10 µM; n = 6) or
nifedipine (30 µM; n = 5) to
block L-type, -conotoxin GVIA (1 µM;
n = 7) or neomycin (0.5 mM;
n = 6) to block N-type, -conotoxin MVIIC (5 µM; n = 5) to block
N-/P-/Q-type, and -agatoxin TK (300 nM; n = 3) to block P-type
Ca2+ channels. Additionally, the divalent
cation Ni2+ was applied at low
concentrations (50-100 µM; n = 32) that predominantly block T-/R-type
Ca2+ channels (Soong et al., 1993 ;
Williams et al., 1994 ; Lee et al., 1999b ). The blockers were added to
the ACSF perfusing the slices from SE-experienced animals for at least
45 min. The dihydropyridines (Fig.
2A, compare
a, b) did not affect bursting in any of the neurons tested, and neither did neomycin (data not shown) or the toxin
blockers of Ca2+ channels (Fig.
2B-D, compare a,
b).

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Figure 2.
Critical role of Ni2+-sensitive
Ca2+ channels in intrinsic burst firing in
SE-experienced animals. Recordings were performed on intrinsically
bursting CA1 neurons from SE-experienced rats (Aa,
Ba, Ca, and Da).
A-D, No change in intrinsic bursting
behavior could be observed after 40 min of perfusion with 10 µM nicardipine (Ab) or 1 µM
-conotoxin GVIA (Bb; 30 min). Likewise,
application of 5 µM -conotoxin MVIIC
(Cb; 40-80 min) or 300 nM -agatoxin TK
(Db; 40-60 min) did not affect intrinsic burst
generation. In all cases, additional perfusion of 50 µM
Ni2+ blocked bursting entirely (Ac,
Bc, Cc, and Dc).
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To test whether intrinsic bursting is generated synergistically by
several types of Ca2+ channels, we have
added the organic Ca2+ channel blockers
sequentially to the ACSF (without washing them out) while recording
from a single neuron. In these experiments (n = 5),
intrinsic bursting was unaffected in all cases (Fig. 3Aa1-d1).
In contrast, when 50 or 100 µM
Ni2+ was added to the ACSF containing one
or more of the organic Ca2+ channel
blockers, intrinsic bursting was entirely suppressed in 26 of 32 (81%)
neurons (Figs. 2Ac-Dc,
3Ae1). To confirm that the organic
Ca2+ channel blockers are
pharmacologically active when applied to the slice, we monitored their
effects on the orthodromically evoked EPSPs. In all experiments,
-conotoxin MVIIC, -conotoxin GVIA, -agatoxin TK, and
nicardipine produced a partial reduction of the EPSPs within 30 min
(Fig.
3Aa2-d2),
presumably consequent to blocking a subset of presynaptic voltage-gated
Ca2+ channels (Wu and Saggau, 1994 ; Qian
and Noebels, 2001 ).

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Figure 3.
Combined application of organic
Ca2+ channel antagonists fails to block bursting.
A, Ca2+ channel blockers were
sequentially added to the ACSF, and the efficacy of
Ca2+ channel blockade was assessed by the
progressive block of the EPSP evoked by orthodromic stimulation of the
Schaffer collaterals
(Aa2-Ae2).
Combined application of organic Ca2+
antagonists did not block bursting
(Aa1-Ad1)
but additional application of 50 µM
Ni2+ did (Ae1).
Blockers were applied for at least 30 min ( -conotoxin GVIA 1 µM, 62 min; -agatoxin TK 300 nM,
40 min; nicardipine 10 µM, 30 min;
Ni2+ 50 µM, 50 min).
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We also examined the consequences of blocking only T-/R-type
Ca2+ channels with low concentrations of
Ni2+. Addition of 10 µM
Ni2+ to the ACSF had no effect on
intrinsic bursting (n = 4), but 30 µM Ni2+ shortened
the bursts in two of four neurons. Addition of 100 µM Ni2+ to the
ACSF reversibly suppressed intrinsic bursts in 35 of 42 (83%) bursters
examined (Fig.
4Aa1-c1).
Raising the concentration of Ni2+ further
(up to 1 mM) did not block intrinsic bursts that
were insensitive to 100 µM
Ni2+ (n = 5; data not
shown), indicating that Ni2+-insensitive
bursting is not mediated by any type of voltage-gated Ca2+ channel. Rather, it may involve
activation of persistent Na+ channels
(Azouz et al., 1996 ; Su et al., 2001 ), but this mechanism was not
investigated further in this study.

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Figure 4.
Low concentrations of Ni2+
suppress burst firing by reducing the spike ADP. A,
Intrinsically bursting CA1 pyramidal neuron from an SE-experienced
animal in normal ACSF (a1), after
block of the burst discharge by perfusion of 50 µM Ni2+
(b1), and after washout
(c1). The slow depolarization
underlying the burst was unmasked by delivering a brief (4 msec)
hyperpolarizing current pulse immediately after the first spike
(a2-c2).
The time course of the ADP was similar in
a1 and
a2 (for comparison at larger
magnification, see d). Adding 50 µM
Ni2+ to the ACSF reversibly suppressed the ADP
(b2,
c2; for comparison at larger
magnification, see e). B, Regular firing
CA1 pyramidal cell in a sham-control animal before
(a) and after (b)
application of 100 µM Ni2+. The
ADP was not affected by Ni2+ (for comparison at
larger magnification, see c).
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Low concentrations of Ni2+ suppress intrinsic
bursting by reducing the spike afterdepolarization
In CA1 pyramidal cells, the fast spike activates a slow
somatodendritic inward current that generates a slow spike ADP in the
soma. Although in regular firing cells the ADP is subthreshold, in
bursters it redepolarizes the neuron sufficiently to generate additional spikes (Azouz et al., 1996 ). We tested in four bursters whether low Ni2+ concentrations suppress
the spike ADP underlying the burst discharge. This slow potential was
unmasked by delivering a brief (4 msec) hyperpolarizing current pulse
immediately after the first spike. The intensity of this pulse was
adjusted to the minimum required to inhibit further discharge (Wong and
Prince, 1981 ; Jensen et al., 1996 ). This procedure disclosed a large
ADP with a duration similar to that of the depolarizing burst envelope
(Fig.
4Aa1,a2; overlaid and enlarged in d). Adding 50 µM Ni2+ to the
ACSF suppressed the burst discharge (Fig.
4Aa1,b1)
and concurrently attenuated the size of the ADP in these cells (Fig. 4Aa2,b2;
overlaid and enlarged in e). We also examined the effect of
low Ni2+ concentrations on the spike ADP
in six regular firing CA1 pyramidal cells in sham-control hippocampal
slices. The spike ADPs in these neurons were significantly smaller than
in neurons from SE-experienced animals (108.0 ± 5.1 vs 250.8 ± 7.1 mV · msec, respectively) and were insensitive to 100 µM Ni2+ (Fig.
4Ba,b; overlaid and enlarged in c).
The Ni2+-insensitive ADP components most
likely are generated by persistent Na+
current (Azouz et al., 1996 ; Su et al., 2001 ).
Depolarization from resting membrane potential abolishes
intrinsic bursting
These data so far have suggested that in CA1
pyramidal cells from SE-experienced animals,
Ni2+-sensitive, T-/R-type
Ca2+ current furnishes the main
depolarizing drive for the spike ADP leading to burst generation. Both
T- and R-type Ca2+ channels are steeply
voltage-dependent and manifest inactivation after depolarization from
the resting membrane potential (Randall and Tsien, 1997 ; Kozlov et al.,
1999 ). To further explore their role in bursting, we tested how
depolarization with constant current injection affects this activity.
In five of seven neurons examined, the burst responses were suppressed
by depolarizing the neurons 3-5 mV from their resting membrane
potential (Fig. 5, compare Aa,
Ba). Depolarizing these neurons by >5 mV suppressed the
burst responses in all cases and induced the appearance of spontaneous single spike firing. Although there may be other explanations, these
results are consistent with the notion that bursting is generated by
T-/R-type Ca2+ currents. Further
supporting this notion was the finding that although
Ni2+ suppressed bursting at resting
membrane potential presumably by reducing the spike ADP (Fig.
5Aa,b; overlaid and enlarged in Ac),
it had no effect on the spike ADP at the slightly more depolarized potentials (Fig. 5Ba,b; overlaid and enlarged in
Bc).

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Figure 5.
Modest depolarization from resting potential
suppresses burst discharges. A, Pyramidal neuron from an
SE-experienced animal showing Ni2+-sensitive
bursting (compare a, b; for comparison at
larger magnification, see c). B,
Depolarization of the neuron from a resting potential of 61 mV to a
potential of 58 mV (compare Aa, Ba)
converts the burst discharge into a single spike. Under these
conditions, Ni2+ did not affect the time course of
the spike ADP (compare Ba, Bb; for
comparison at larger magnification, see c).
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Increase in T-type Ca2+ current density in
SE-experienced animals
The de novo appearance of
Ni2+-sensitive intrinsic bursting in CA1
pyramidal cells described above might be caused by a genuine increase
in the density of functional T-/R-type
Ca2+ channels, a more effective
recruitment of existing channels by the first somatodendritic spike, or
both. We have therefore directly measured the densities of T- and
R-type Ca2+ currents in CA1 pyramidal
cells in naive-control and SE-experienced rats using the whole-cell
patch-clamp technique.
We first compared the densities of these currents between the two
experimental groups in visually identified CA1 pyramidal cells in
hippocampal slices. Voltage steps from 90 to 60 and 50 mV evoked
transient Ca2+ currents (Fig.
6Aa) (example shown for
60 mV voltage steps). The densities of these currents were
significantly larger (2.2-fold and 1.9-fold increase for command pulses
to 60 and 50 mV, respectively; p < 0.01) in
SE-experienced animals (n = 10 cells; 6-12 d after pilocarpine-induced SE) compared with the naive-control animals (n = 12 cells) (Fig. 6Ac).

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Figure 6.
Increased density of T-type
Ca2+ currents in SE-experienced animals.
A, Recordings of T-type Ca2+ current
in a CA1 pyramidal cell in the slice preparation using voltage steps
from 90 to 60 or 50 mV (a) or in a
dissociated CA1 neuron perfused with ACSF containing 2 µM
-conotoxin GVIA, 3 µM -conotoxin MVIIC, 200 nM -agatoxin GIVA, and 10 µM nifedipine to
block most of the high-voltage-activated Ca2+
channel types (b; see also Fig.
8Ab). In this preparation,
Ca2+ currents were evoked with voltage steps to 50
mV from a holding potential of 80 mV after a conditioning prepulse to
100 mV (5 sec). Average T-type amplitudes measured in SE-experienced
versus naive-control animals in either CA1 neurons in slices
(n = 10 and 12, respectively) or dissociated CA1
neurons (n = 14 and 15, respectively) are depicted
in c. The current amplitudes were normalized to the cell
capacitance in all cases. The current density showed a significant
increase in SE-experienced animals (black bars) compared
with naive-control animals (white bars) for recordings
from both dissociated and intact CA1 neurons (*p < 0.05). B, Ni2+ sensitivity of the
T-type current in dissociated CA1 neurons. The T-type current was
markedly and reversibly reduced by micromolar concentrations of
Ni2+, as shown in an exemplary recording from an
SE-experienced animal (a).
Concentration-dependence of the T-type Ca2+ current
block by Ni2+ in both SE-experienced ( ) and
naive-control groups ( ) (SE-experienced group: n = 3, 6, 6, and 3 cells; naïve-control group:
n = 4, 2, 7, and 5 cells for 10, 30, 100, and 300 µM Ni2+; b). Data were
fit by a Hill equation using a Levenberg-Marquard nonlinear
curve-fitting procedure. The fitting curve is shown
superimposed on the data points.
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Similar experiments were performed in acutely dissociated CA1 pyramidal
cells using depolarizing voltage steps to 50 mV preceded by a 5 sec
prepulse to 100 mV (Fig. 6Ab). In these experiments we also superfused the neurons with ACSF containing organic
Ca2+ channel blockers (2 µM -conotoxin GVIA, 3 µM -conotoxin MVIIC, 200 nM -agatoxin GIVA, and 10 µM nifedipine) to avoid even a small
contribution of N-, P/Q-, or L-type Ca2+
channels (Avery and Johnston, 1996 ). As found in the slice preparation, the densities of T-type Ca2+ currents in
dissociated CA1 pyramidal cells were significantly larger (3.3-fold
increase; p = 0.0001) in SE-experienced
(n = 14 cells; 30-40 d after SE) compared with
naive-control animals (n = 15 cells) (Fig.
6Ac).
Ni2+ sensitivity of T-Type
Ca2+ current in SE-experienced animals
Recent studies of voltage-gated Ca2+
channels have identified three pore-forming 1
subunits, namely, 1G,
1H, and 1I, that give
rise to T-type Ca2+ channels (Cribbs et
al., 1998 ; Perez-Reyes et al., 1998 ; Lee et al., 1999a ). All three
subunits are expressed in hippocampal CA1 pyramidal cells (Talley et
al., 1999 ). They differ, however, in their sensitivity to blockage by
Ni2+, with 1H
being an order of magnitude more sensitive to
Ni2+ than 1G and
1I (Lee et al., 1999b ). We have therefore
examined the Ni2+ sensitivity of the
T-type Ca2+ current in these neurons in
SE-experienced as well as in the naive-control animals. In both groups,
100 µM Ni2+ almost
completely and reversibly blocked the T-type
Ca2+ current (Fig. 6Ba).
Dose-response curves for Ni2+ (10-300
µM) (Fig. 6Bb) yielded
similar IC50 values for SE-experienced (24.6 ± 2.6 µM; maximal block 84.5 ± 4.1%)
and naive-control animals (27.9 ± 1.6 µM;
maximal block 79.6 ± 2.0%).
T-type Ca2+ currents invariably show
characteristically slow deactivation rates that distinguish them from
the much more rapidly deactivating R-type channels (Randall and Tsien,
1997 ; Nakashima et al., 1998 ; Kozlov et al., 1999 ). Therefore, tail
currents after brief depolarizing steps that activate both T- and
R-type Ca2+ currents may be used to
analyze these two current components separately. As illustrated in
Figure 7Aa, activation of
pharmacologically isolated T-/R-type Ca2+
currents by mock action potentials as voltage commands was followed by
biphasic tail currents in both experimental groups of neurons. These
currents were best fitted by a biexponential curve (Fig. 7Ab). The fast ( f) and slow
( s) decay time constants of these tail
currents were, respectively, 478 ± 275 µsec and 4.1 ± 2.5 msec in naive-control animals (n = 7 cells),
and 712 ± 122 µsec and 4.7 ± 1.6 msec in SE-experienced
animals (n = 5 cells). The rapidly deactivating
component most probably corresponds to an R-type current, whereas the
slowly deactivating component is caused by T-type
Ca2+ currents (Kozlov et al., 1999 ).
Indeed, the amplitude of the slowly deactivating component of the tail
current derived from biexponential fitting was tightly correlated with
the amplitude of the T-type Ca2+ current
measured with rectangular voltage steps (correlation coefficient 0.88;
p = 0.0005; n = 12 cells). The
amplitude of the slow (presumably T-type) tail
Ca2+ current component was considerably
larger in the SE-experienced group than in the control group (3.9-fold
increase; p = 0.005), whereas that of the rapid
(presumably R-type) component was not different (Fig. 7B).
These results support our conclusion of a selective upregulation of
T-type Ca2+ current in CA1 pyramidal cells
in SE-experienced animals.

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Figure 7.
Increased T-type Ca2+ currents
after SE are associated with an increase in slowly deactivating
Ca2+ tail currents after mock action potentials.
A, Application of mock action potentials (rising phase 1 msec; decaying phase 2 msec; peak +30 mV) as a voltage command in
dissociated CA1 pyramidal neurons from naive-control animals
(a1) and SE-experienced animals
(a2). Current traces were derived by
subtraction of traces obtained in the presence of organic
Ca2+ blockers and 300 µM
Ni2+ from traces obtained only in the presence of
organic Ca2+ channel blockers and thus reflect
Ca2+ influx through T-/R-type channels. The decay of
the inward tail current immediately after termination of the mock
action potential was fit by a biexponential equation superimposed on
the data points (b). B, Amplitudes
of the fast and slowly decaying component of the tail currents
normalized to the cell capacitance. A significant increase was observed
only for the slower decaying component (*p < 0.005).
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Changes in densities of high voltage-activated
Ca2+ currents in SE-experienced animals
In the slice preparation, voltage steps to potentials above 40
mV evoked large Ca2+ currents that escaped
voltage-clamp control in neurons from both experimental groups.
Therefore, changes in the densities of high voltage-activated
Ca2+ currents were investigated only in
acutely dissociated CA1 pyramidal cells, in which these currents could
be adequately voltage clamped (Beck et al., 1999 ). Stepping the
membrane voltage from 100 to 0 mV evoked large
Ca2+ currents (69.5 ± 4.0 pA/pF in
naïve control animals; 69.0 ± 5.7 pA/pF in SE-experienced
animals), which were reduced to approximately one-third by perfusing
the neurons with ACSF containing the organic Ca2+ channel blockers (Fig.
8Aa,b). The
residual current evoked with test pulses to 0 mV comprises mostly
R-type Ca2+ currents, with a small
contribution of T-type currents (Thompson and Schwindt, 1991 ). Despite
the increase in T-type current amplitude, the density of the compound
T-/R-type current was not different between SE-experienced
(n = 21) and naive-control neurons (n = 20) (Fig. 8Ac), indicating that the R-type current is
either unaltered or slightly reduced. This conclusion is supported also
by the lack of change in amplitude of the rapidly decaying tail
Ca2+ current component after mock action
potentials (Fig. 7B).

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Figure 8.
Functional analysis of high-threshold current
components. A, Recordings were obtained in a dissociated
CA1 pyramidal neuron from a naive-control animal.
Ca2+ currents were evoked with the voltage paradigm
shown in the inset. To isolate the T-/R-type
Ca2+ current, the organic blockers -conotoxin
GVIA (2 µM), -conotoxin MVIIC (3 µM),
-agatoxin GIVA (200 nM), and nifedipine (10 µM) were co-applied, unmasking a rapidly inactivating
residual component (a). The current
traces in a were recorded at the time
points indicated by the lowercase letters in
b. Pharmacologically isolated T-/R-type
Ca2+ currents were compared in dissociated CA1
pyramidal neurons from SE-experienced (n = 21 cells) and naive-control animals (n = 20 cells)
(c). Current densities were obtained by
normalizing current amplitudes to cell capacitance. B,
In another dissociated neuron from a naive-control animal, the organic
Ca2+ channel blockers -conotoxin GVIA (2 µM), -agatoxin IVa (200 nM), and
nifedipine (10 µM) were added sequentially
(a; duration of application is indicated by
horizontal bars, b). This allowed
assessment of the individual contributions of N-, P/Q-, and L-type
Ca2+ current components to the whole-cell current
(indicated at right margin of b). The
current traces in a were recorded at the
time points indicated by the lowercase
letters in b. High-voltage-activated
Ca2+ current densities in naïve control
(n = 9-10) versus SE-experienced rats
(n = 10) are shown in c. The N-type
current density was significantly reduced (*p < 0.05), whereas the density of P/Q- and L-type currents was
unaltered.
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We also compared the densities of
Ni2+-insensitive, high-threshold
Ca2+ currents in acutely dissociated CA1
pyramidal cells from SE-experienced versus naive-control animals. The
amplitudes of N-, P/Q-, and L-type Ca2+
currents were determined by sequentially applying the selective antagonists 2 µM -conotoxin GVIA (n = 10 for both groups), 200 nM -agatoxin IVa
(n = 10 for both groups), and 10 µM nifedipine (naive-control, n = 9 cells; SE-experienced, n = 10 cells), respectively (Fig. 8Ba,b). The effects of -conotoxin
GVIA and -agatoxin IVa were primarily irreversible (Fig.
8Bb). The N-type Ca2+
current density was significantly reduced in the SE-experienced compared with the naive-control group, whereas the densities of P/Q-
and L-type currents were not significantly altered (Fig. 8Bc). Thus, of all the different types of
Ca2+ currents expressed in CA1 pyramidal
neurons, only T-type Ca2+ channel density
is upregulated in SE-experienced animals.
Impact of altered firing mode on neuronal responses to
synaptic excitation
The conversion of CA1 pyramidal cells from regular firing to
burst firing after pilocarpine-induced SE would be expected to amplify
their spike output in response to excitatory synaptic inputs. To
examine this notion, we compared the synaptic activation of regular
firing neurons in sham-control animals (Fig.
9Aa) (n = 8 cells) with that of bursting neurons in SE-experienced animals (Fig.
9Ba) (n = 4 cells). Single-shock stimuli
were applied to afferent fibers in stratum radiatum, and their
intensity was adjusted to evoke threshold-straddling EPSPs (Fig.
9Ab,Bb). As expected, the minimal response in
sham-control animals was a single spike (Fig. 9Ab). In
contrast, the minimal response in SE-experienced animals was a spike
burst similar in pattern to that evoked by direct current injection
(Fig. 9Bb). To confirm that in the latter group the
threshold EPSPs recruit the intrinsic burst mechanism rather than
produce multiple spiking by virtue of their longer duration (Fig. 9,
compare top panels in Ab, Bb), we
exposed them to Ni2+. Because a small
blocking effect of Ni2+ was observed on
EPSPs, the stimulus strength was readjusted to yield threshold EPSPs.
Adding 100 µM Ni2+
to the ACSF suppressed the intrinsic burst response (Fig.
9Bc) and reduced the burst responses to threshold EPSPs to
single spikes (Fig. 9Bd) without affecting the duration of
these EPSPs (Fig. 9Ba,c, top traces).
These data clearly demonstrate that SE, by modifying intrinsic neuronal
properties of CA1 pyramidal cells, markedly and persistently amplifies
the neuronal output to a given synaptic input.

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Figure 9.
Impact of intrinsic plasticity on neuronal
responses to synaptic excitation. These experiments were performed in
the absence of blockers of synaptic transmission in the control ACSF.
A, Recordings from a regular firing CA1 pyramidal cell
from a sham-control animal. Firing behavior was determined using long
depolarizing current injections through the recording microelectrode
(a). Single-shock stimuli were applied to
afferent fibers in stratum radiatum and adjusted to evoke
threshold-straddling EPSPs (b; different trials with
identical stimulation intensity are shown). B, A similar
experiment in a bursting neuron (a) from an
SE-experienced animal (n = 4 cells). All
suprathreshold EPSPs elicited a burst discharge (b;
three different trials with identical stimulation intensity; 1.4 V).
Application of 100 µM Ni2+ blocked the
intrinsic bursts induced by depolarizing current pulses (compare
a, c). It also slightly reduced the
amplitude of the EPSPs without affecting their duration (data not
shown). To elicit threshold EPSPs in the presence of 100 µM Ni2+, stimulation intensity was
increased to 1.5 V (d, top trace). Under
these conditions, the EPSP-evoked firing responses were converted to
single spikes (d; middle and
bottom traces).
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DISCUSSION |
In this study we demonstrate that the intrinsic discharge behavior
of hippocampal CA1 neurons is dramatically modified after pilocarpine-induced SE, in congruence with another recent study (Sanabria et al., 2001 ). This form of plasticity consists of a transition from regular firing to a burst-firing mode, in which the
minimal response of >50% of the neurons to threshold depolarization is a burst of several spikes. We also show that this abnormal burst
activity is resistant to blockers of L-, N-, and P/Q-types of
voltage-sensitive Ca2+ channels but is
readily suppressed by low concentrations of
Ni2+ that block R- and T-types.
Furthermore, we show that the appearance of
Ni2+-sensitive intrinsic bursting is
associated with a marked increase in the density of T-type, but not
R-type, Ca2+ channels. Cumulatively, these
data suggest that an increase in T-type
Ca2+ current density plays a critical role
in the intrinsic neuronal plasticity that is triggered by a single
episode of SE.
Role of T-type Ca2+ current in intrinsic
neuronal plasticity
It was shown previously that SE-induced intrinsic bursting in
pilocarpine-treated animals is suppressed by removal of
Ca2+ from, or the addition of 1 mM Ni2+ to, the ACSF, but not
by the intracellular application of a Ca2+
chelator, suggesting that this activity is driven directly by a
Ca2+ current (Sanabria et al., 2001 ). Our
further pharmacological experiments show that none of the organic
Ca2+ channel blockers that affect L-, N-,
and P-/Q-type Ca2+ channels, applied
individually or in combination, blocked intrinsic bursting in this
model. In contrast, both intrinsic bursting and its underlying spike
ADP were suppressed by low concentrations of
Ni2+ (30-100 µM), which
block both T- and R-type Ca2+ channels in
CA1 pyramidal cells. In addition, moderate depolarization of the neuron
from its resting membrane potential, which would augment the
steady-state inactivation of both T- and R-type
Ca2+ channels (Schneider et al., 1994 ;
Kozlov et al., 1999 ), abolished intrinsic bursting. These results by
themselves are consistent with a role of either T- or R-type
Ca2+ channels in intrinsic burst generation.
Two major lines of evidence, however, argue for a critical role of
T-type Ca2+ channels in mediating this
activity. First, the density of T-type Ca2+ current was considerably (1.9- to
3.3-fold) increased in CA1 pyramidal cells after SE, whereas the
density of all other types of Ca2+ current
(including the R-type) was either unaltered or decreased. Second,
T-type Ca2+ currents display biophysical
characteristics that make them particularly suitable to mediate burst
discharges (Huguenard, 1996 ). Thus, T-type, but not R-type,
Ca2+ channels display a slow rate of
deactivation (time constants in the order of several milliseconds) at
potentials close to the neuronal resting potential (Randall and Tsien,
1997 ; Kozlov et al., 1999 ). As a consequence of this feature, action
potentials induce a slow tail Ca2+ current
mediated by T-type Ca2+ currents. We have
found that the increase in T-type Ca2+
current amplitude after SE is associated with a marked and selective increase of the slowly deactivating tail current component after mock
action potentials. Clearly, an increase in slow inward currents after
action potentials could initiate a regenerative depolarization that
would boost the ADP beyond spike threshold and elicit additional discharge. Additionally, the low threshold for activation and enhanced
deinactivation during hyperpolarization of T-type
Ca2+ channels would allow them to furnish
the initial depolarizing drive for spontaneous burst discharges
(Huguenard, 1996 ).
In normal CA1 pyramidal cells, intrinsic bursting mediated by
Ca2+ currents has been demonstrated only
after blocking outward K+ currents by
millimolar concentrations of 4-aminopyridine (Magee and Carruth, 1999 ).
However, in that condition, bursting was generated by both
Ni2+-sensitive and
Ni2+-insensitive
Ca2+ currents (Magee and Carruth, 1999 ),
reflecting the complement of voltage-gated
Ca2+ channels normally expressed in these
neurons. It is improbable, therefore, that a persistent reduction in
outward K+ currents consequent to
pilocarpine-induced SE, by itself, accounts for the change in discharge
behavior reported here. However, changes in expression of voltage-gated
channels other than Ca2+ channels also may
contribute to the intrinsic neuronal plasticity. Indeed, it was found
previously (Sanabria et al., 2001 ), and confirmed in the present study,
that some CA1 neurons in SE-experienced animals display a
Ca2+-independent burst mechanism. A likely
candidate for mediating Ca2+-insensitive
bursting in CA1 pyramidal cells is the persistent Na+ current (Azouz et al., 1996 ; Su et
al., 2001 ), but the contribution of this current to SE-induced
intrinsic plasticity has yet to be demonstrated.
Molecular basis of intrinsic neuronal plasticity
Our data allow us to propose that of the three known T-type
Ca2+ channel 1
subunits (i.e., 1H,
1I, and 1G),
1H most probably underlies the augmented
T-type Ca2+ current and associated
intrinsic bursting after pilocarpine-induced SE. It was shown that when
expressed in human embryonic kidney cells, the
Ca2+ currents mediated by the three cloned
1 subunits are differentially blocked by
Ni2+, with the 1H
subunit being ~20-fold more sensitive (IC50
values, 12 µM) than 1G and
1I subunits (IC50
values, 250 and 216 µM, respectively) (Lee et al.,
1999b ). The T-type Ca2+ currents in CA1
pyramidal cells in both control and SE-experienced animals were highly
sensitive to Ni2+
(IC50 values of 24 and 28 µM,
respectively), suggesting that 1H subunits
contribute strongly to this current. Likewise, the slow (~4-5 msec)
Ca2+ tail currents that follow mock action
potentials suggest the involvement of 1H
and/or 1G subunits, which have a comparably slow deactivation kinetics (Kozlov et al., 1999 ). Clearly, more experiments will be required to prove unequivocally the role of the
1H Ca2+ channel
subunit in SE-induced intrinsic plasticity. Interestingly, it was shown
recently that intrinsic bursting in thalamic neurons relies on
expression of the 1G subunit (Kim et al.,
2001 ); thus intrinsic bursting in different classes of neurons may be
produced by distinct T-type Ca2+ channel subunits.
Functional consequences of altered intrinsic
neuronal properties
Modifications of intrinsic neuronal properties dependent on
neuronal activity have been described previously in invertebrate (Turrigiano et al., 1994 ) and vertebrate (Desai et al., 1999 ) culture
models. In these studies, long-term deprivation of activity causes
neurons to fire more rapidly in response to injected current (Desai et
al., 1999 ) or even to switch from a tonic to a burst firing mode
(Turrigiano et al., 1994 ). Such mechanisms are thought to be
homeostatic, i.e.,. they serve to stabilize the properties of neural
circuits (Stemmler and Koch, 1999 ; Turrigiano, 1999 ). The plasticity
that we describe here represents the converse: SE produces a
long-lasting gain in the input-output properties of CA1 neurons.
Increased bursting is observed up to 90 d after status epilepticus
(our unpublished data), suggesting that this form of plasticity
may be stable over prolonged periods of time.
Computer modeling studies of realistic neuronal networks have
previously suggested that intrinsic bursters are pivotal in the
generation of epileptiform activity (Traub and Wong, 1982 ; Miles and
Wong, 1983 ). There is also a large body of experimental evidence in
support of this contention. Increased intrinsic bursting is observed in
acute models of hippocampal epilepsy, such as the high-K+ model (Jensen et al., 1994 , 1996 ;
Azouz et al., 1996 , 1997 ; Su et al., 2001 ). Moreover, intrinsic
bursters were shown to be the forerunners of epileptiform events
in vitro, suggesting that they may be important in
initiating epileptiform discharges (Chagnac-Amitai and Connors, 1989 ;
Jensen and Yaari, 1997 ; Sanabria et al., 2001 ). Therefore,
identification of the mechanisms responsible for the abnormal intrinsic
bursting in epileptic tissue may permit pharmacological inhibition of
seizure initiation in experimental and human epilepsy. It should be
noted, however, that an episode of SE induced by pilocarpine or other
procedures triggers long-term changes in synaptic function that may
also play a role in the development of an epileptic condition
(McNamara, 1999 ).
In summary, our observations suggest that the transformation of CA1
pyramidal cells from regular firing to burst-firing after pilocarpine-induced SE involves the persistent augmentation of a T-type
Ca2+ current, possibly that mediated by
the 1H subunit. This SE-induced intrinsic
plasticity leads to a marked change in the input-output properties of
hippocampal neurons that, in concert with altered synaptic
connectivity, may underlie the hyperexcitability characteristic of TLE.
Furthermore, these results suggest that subunit-selective T-type
Ca2+ channel blockers may be promising
targets for rational anti-epileptic drug design in TLE.
 |
FOOTNOTES |
Received Dec. 17, 2001; revised Feb. 11, 2002; accepted Feb. 18, 2002.
*
H.S. and D.S. contributed equally to this work.
This research was supported by the German-Israel collaborative
research program of the Ministry of Science and the Bundesministerium für Bildung und Forschung, Deutsche Forschungsgemeinschaft EL 122/7,
the SFB 6006, the Israel Science Foundation, a University of
Bonn Medical Center "BONFOR" grant, the Erna D. and Henry J. Leir
Chair for Research in Neurodegenerative Diseases, and a Humboldt Research Award to Y.Y. We thank E. Perez-Reyes, T. Schneider, and A. Konnerth for critical comments.
Correspondence should be addressed to Dr. Heinz Beck, Department of
Epileptology, University of Bonn Medical Center, Sigmund-Freud Strasse
25, D-53105 Bonn, Germany. E-mail:
heinz.beck{at}ukb.uni-bonn.de.
 |
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