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The Journal of Neuroscience, June 15, 2001, 21(12):4173-4182
Extracellular Calcium Modulates Persistent Sodium
Current-Dependent Burst-Firing in Hippocampal Pyramidal Neurons
Hailing
Su,
Gil
Alroy,
Eilon D.
Kirson, and
Yoel
Yaari
Department of Physiology, Institute of Medical Sciences, The Hebrew
University-Hadassah Faculty of Medicine, Jerusalem 91120, Israel
 |
ABSTRACT |
The generation of high-frequency spike bursts ("complex
spikes"), either spontaneously or in response to depolarizing stimuli applied to the soma, is a notable feature in intracellular recordings from hippocampal CA1 pyramidal cells (PCs) in vivo.
There is compelling evidence that the bursts are intrinsically
generated by summation of large spike afterdepolarizations
(ADPs). Using intracellular recordings in adult rat hippocampal slices,
we show that intrinsic burst-firing in CA1 PCs is strongly dependent on
the extracellular concentration of Ca2+
([Ca2+]o). Thus, lowering
[Ca2+]o (by equimolar substitution
with Mn2+ or Mg2+) induced
intrinsic bursting in nonbursters, whereas raising
[Ca2+]o suppressed intrinsic bursting
in native bursters. The induction of intrinsic bursting by low
[Ca2+]o was associated with
enlargement of the spike ADP. Low
[Ca2+]o-induced intrinsic bursts and
their underlying ADPs were suppressed by drugs that reduce the
persistent Na+ current
(INaP), indicating that this current
mediates the slow burst depolarization. Blocking
Ca2+-activated K+ currents with
extracellular Ni2+ or intracellular chelation of
Ca2+ did not induce intrinsic bursting. This and
other evidence suggest that lowering
[Ca2+]o may induce intrinsic bursting
by augmenting INaP. Because repetitive neuronal activity in the hippocampus is associated with marked decreases in [Ca2+]o, the
regulation of intrinsic bursting by extracellular
Ca2+ may provide a mechanism for preferential
recruitment of this firing mode during certain forms of hippocampal activation.
Key words:
intrinsic bursting; calcium; persistent sodium current; pyramidal cell; hippocampus; phenytoin; gap junction; PKC; rat
 |
INTRODUCTION |
The discharge of many hippocampal
CA1 pyramidal cells (PCs) in vivo is a mixture of single
spikes and high-frequency bursts of several spikes (Kandel and Spencer,
1961
; Fujita, 1975
; Nuñez et al., 1990
). There is convincing
evidence that the spike bursts (or "complex spikes") are generated
intrinsically by slow, voltage-gated membrane currents (Kandel and
Spencer, 1961
; Fujita, 1975
; Nuñez et al., 1990
; Kamondi et al.,
1998
). Such bursts are thought to play important roles in electrical
signaling, in neuronal synchronization, and in the induction of
long-term synaptic plasticity (for review, see Lisman, 1997
).
In isolated hippocampal slices perfused with standard saline, only a
small fraction (~20%) of CA1 PCs manifest an intrinsic tendency to
burst-fire; most of these neurons are regular firing cells
(Schwartzkroin, 1975
; Masukawa et al., 1982
; Jensen et al., 1994
). The
scarcity of intrinsic bursters in CA1 in vitro may reflect
the fact that the firing pattern of an individual PC is not an
invariable attribute. Rather, it is strongly modulated by the ionic
composition of the extracellular fluid. Thus, modest increases in
extracellular pH (Church and Baimbridge, 1991
) or concentration of
K+
([K+]o) (Jensen et
al., 1994
), or modest decreases in extracellular osmolality (Azouz et
al., 1997
), can convert regular firing PCs to intrinsic bursters.
Because these factors vary as a function of ongoing neuronal activity
in the brain, it is possible that the intrinsic firing pattern of CA1
PCs in vivo may alternate between nonbursting and bursting
in different states of hippocampal activation.
The baseline concentration of free extracellular
Ca2+
(Ca2+o) is
1.2-1.5 mM, but neuronal activity can cause Ca2+o concentration
([Ca2+]o) to
decrease considerably (Heinemann et al., 1977
). Therefore, it is
important to establish how changes in
[Ca2+]o affect the
firing pattern of hippocampal neurons. In a previous study we concluded
that somatic bursting in CA1 PCs is neither driven by
Ca2+ currents nor terminated by
Ca2+-activated
K+ currents (Azouz et al., 1996
). However,
we noted that lowering [Ca2+]o increases
the propensity of these neurons to burst in response to depolarization.
In this study we describe this effect of low [Ca2+]o in more
detail and examine three putative hypotheses regarding its underlying
mechanism: (1) suppression of repolarizing
Ca2+-activated
K+ currents, (2) upmodulation of
persistent Na+ current
(INaP), and (3) increase in
electrotonic coupling through gap junctions. Our data are consistent
only with the second hypothesis.
A preliminary report of these findings has been published previously in
a recent abstract (Su et al., 1999
).
 |
MATERIALS AND METHODS |
Slice preparation. All experimental protocols were
approved by the Hebrew University Animal Care and Use Committee.
Transverse hippocampal slices were prepared from adult Sabra rats
(150-200 gm). Animals were anesthetized with ether and decapitated
with a guillotine. The brain was removed and immediately immersed in ice-cold, oxygenated (95% O2, 5%
CO2) dissection saline. The caudal two-thirds of
one hemisphere (containing one hippocampus) were glued to the stage of
a Vibratome (Campden Instruments). Transverse slices (400 µm thick)
were cut from the region of the hemisphere containing the anterior
hippocampus. The hippocampal portion was dissected out of each slice
and transferred to an incubation chamber containing oxygenated saline
at room temperature (21-24°C). For experimental recordings, the
slices were transferred to an interface slice chamber and perfused from
below with oxygenated (95% O2, 5%
CO2) saline at 33.5°C. The upper surface of the
slices was exposed to the humidified gas mixture. The slices were
allowed to recover at least 1 hr before the experiment was started.
Solutions and drugs. The standard saline solution contained
(in mM): NaCl 124, KCl 3.5, MgSO4 2, CaCl2 2, NaHCO3 26, and D-glucose 10, pH 7.3. Low-Ca2+ salines were prepared
by equimolar substitution of CaCl2 with MnCl2. In some experiments, where indicated,
CaCl2 was replaced with
MgCl2. High-Ca2+
saline was prepared by replacing MgSO4 with
CaCl2.
All of the salines also contained the glutamate receptor antagonists
6-cyano-7-nitro-quinoxaline-2,3-dione (CNQX; 15 µM) and 2-amino-5-phosphono-valeric acid (50 µM) to block fast EPSPs and the
GABAA receptor antagonist bicuculline methiodide
(10 µM) to block fast IPSPs.
Salts and drugs were purchased from Sigma (St. Louis, MO), with the
exception of CNQX (RBI, Natick, MA) and doxyl-stearic acid (Aldrich,
Milwaukee, WI). Phenytoin was dissolved in 1N NaOH. The phorbol esters
4
-phorbol 12,13-dibutyrate (PDB) and 4
-phorbol 12,13-didecanoate
(PDC) were dissolved in dimethyl sulfoxide (DMSO), and doxyl-stearic
acid was dissolved in ethanol before it was added to the saline.
Control salines contained equivalent concentrations of DMSO or ethanol
(not >0.1%), which had no effects on the measured parameters.
Intracellular recordings. Current-clamp recordings from the
somata of PCs in the CA1 pyramidal layer were made using sharp, K+-acetate-filled (4 M) glass microelectrodes (60-90 M
). In some experiments, where indicated, 200 mM BAPTA, or
2% biocytin, were included in the filling solution. An active bridge
circuit in the amplifier (Axoclamp 2A, Axon Instruments) allowed
simultaneous injection of current and measurement of membrane
potential. The bridge balance was carefully monitored and adjusted
before each measurement. Bipolar platinum electrodes (50 µm)
connected to a stimulator by an isolation unit were used for focal
stimulation (1-20 V, 50-70 µsec) of pyramidal axons in the alveus.
Neurons were identified as PCs if they responded with short latency
spikes to antidromic stimulation and manifested strong spike frequency adaptation during a sustained depolarization. The PCs accepted for this
study had stable resting potentials of at least
55 mV and
overshooting action potentials.
Cell staining. For assessing the incidence of gap junctions
among CA1 PCs, some neurons were injected with biocytin. After the
experiment, the slices were fixed overnight in 4% paraformaldehyde, cut into thin (120 µm) sections, and incubated with avidin-biotin complex (Vectastain ABC elite kit, Vector Laboratories, Burlingame, CA). The stained cells were photographed at 200× magnification.
Data measurement and analysis. The intracellular signals
were digitized and stored on a personal computer using a data
acquisition system (TL-1, Axon Instruments). Off-line data analyses
were performed using pCLAMP software (Axon Instruments).
To measure passive membrane properties, the PCs were injected with
small (0.1-0.5 nA) 200 msec negative current pulses. The input
resistance was provided by the slope of the linear regression line
fitted through the linear portion of the steady-state voltage versus
current amplitude plot. The apparent membrane time constant (
m) was taken as the slowest component
(
0) of multiexponential function fitted to the
charging curve produced by application of a small negative current step
(from onset to steady state), as suggested by Rall (1977)
. The fast
spike afterhyperpolarization (AHP) was measured as the potential
attained at the end of fast spike repolarization. A measure for the
size of the spike and subthreshold afterdepolarizations (ADPs) was
provided by the area delimited by the ADP waveform and resting membrane
potential. This measure was sensitive to both ADP amplitude and
duration. Inward rectification was evaluated from the nonlinear voltage responses to slow (0.9 sec long) depolarizing current ramps. The membrane potential at which the membrane began to rectify was determined by extrapolating a line fitted to the linear portion of the
voltage-current relation. The initial and mean firing rates during a
burst were calculated from the first interspike interval and from the
mean interspike interval, respectively.
Averaged data are expressed as mean ± SD. The significance of the
differences between the measured spike parameters was evaluated using
Student's paired t test or Wilcoxon's paired-sample test with a significance level of 0.05. Correlation between the firing pattern and the incidence of dye coupling of the PCs was tested with
the Spearman rank order correlation.
Classification of PC firing patterns. In this study we
defined a burst as a cluster of three or more closely spaced action potentials, riding on a distinct slow depolarizing envelope. As suggested previously (Jensen et al., 1994
, 1996
; Azouz et al., 1997
),
PCs were classified into three groups according to their response to
long (150-200 msec) depolarizing current pulses of increasing
intensity (in steps of 30-100 pA). The variant firing patterns
observed in CA1 PCs perfused with nominally
Ca2+-free saline are portrayed in Figure
1. Nonbursters generated accommodating trains of independent action potentials in response to
all suprathreshold stimuli (Fig. 1A). High-threshold
bursters (HTBs) generated burst-like responses only when subjected to
strong suprathreshold stimuli (Fig. 1B), whereas
low-threshold bursters (LTBs) fired in burst mode in response to
threshold-straddling stimuli. To quantify the propensity to generate a
burst, the latter heterogeneous group was further divided into three
subgroups of increasing tendency for burst generation. Grade I LTBs
fired only one spike in response to a brief (3-5 msec) depolarizing
current pulse (Fig. 1C); grade II LTBs generated a burst
also in response to a brief stimulus (Fig. 1D); and
grade III LTBs also fired spontaneously in burst mode (Fig.
1E). It should be stressed that this classification of CA1 PCs into five different subgroups does not imply a fundamental difference in mechanisms and is used only for descriptive purposes.

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Figure 1.
Variant firing patterns of CA1 PCs in low
[Ca2+]o. Intracellular recordings were
made in five PCs in slices perfused with nominally
Ca2+-free saline. The PCs were injected with long
(200 msec) and brief (3-5 msec) positive current pulses of increasing
intensity (in steps of 50-100 pA). The top panels
(a) in A-D
illustrate the firing patterns of four different PCs evoked by two long
current pulses. The bottom panels
(b) depict the respective responses to brief
stimuli. The injected current pulses are indicated below the voltage
traces. A, A nonburster (NB). This neuron
generated nonclustered spike trains in response to long current pulses
(a) and a single spike in response to brief
current pulses (b). B, A
high-threshold burster (HTB). This neuron generated an
initial burst only in response to strong long current pulses
(a) and a single spike in response to brief
current pulses (b). C, Grade I
low-threshold burster (LTB I). This neuron
generated bursts in response to threshold and suprathreshold long
current pulses (a), but a single spike in
response to brief current pulses (b).
D, Grade II LTB (LTB II). This
neuron fired bursts in response to both long (a)
and brief (b) current pulses. E,
Grade III LTB (LTB III). In addition to firing
bursts in response to any threshold stimuli (data not shown), this
neuron displayed spontaneous, rhythmic burst firing. The spontaneous
burst marked with an asterisk in the top
trace of E is shown in the bottom
trace on an expanded time scale. In this and the following
Figures, dashed lines indicate truncated spikes. Resting
potentials are provided to the left of topmost
panels.
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 |
RESULTS |
Effects of lowering [Ca2+]o on the
firing patterns of CA1 PCs
In standard saline, the proportion of intrinsically bursting CA1
PCs was small and the bursting threshold in these bursters was high, as
described previously (Jensen et al., 1994
). Of 136 neurons examined,
112 (82%) were nonbursters and 24 (17%) were bursters (of which 20 were HTBs and 4 grade I LTBs). Lowering [Ca2+]o markedly
increased the incidence of, and decreased the threshold for, intrinsic
bursting in most PCs. In the representative experiment illustrated in
Figure 2, changing from standard to 1.2 mM Ca2+ saline converted the
nonbursting PC (Fig. 2A) into an HTB (Fig. 2B). Further reduction of
[Ca2+]o to 0.5 mM converted the PC into a grade I LTB (Fig.
2C). Finally, in nominally
Ca2+-free saline the PC changed into a
grade II LTB (Fig. 2D).

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Figure 2.
Effect of lowering
[Ca2+]o on the intrinsic firing
pattern of a CA1 PC. Recordings were made in a slice perfused with
salines containing different concentrations of Ca2+.
A, In standard saline, the PC was a nonburster, as
determined from its responses to 200 msec (a) and
3 msec (b) depolarizing current pulses.
B, After a 30 min wash in 1.2 mM
Ca2+-saline, the PC became an HTB, firing a burst in
response to a strong 200 msec depolarization (a).
C, After a 30 min wash in 0.5 mM
Ca2+-saline, the PC became a grade I LTB, firing a
burst also in response to a threshold 200 msec depolarization
(a). D, Finally, after a 30 min
wash in Ca2+-free saline, the PC became a grade II
LTB, firing a burst in response to any threshold depolarization
(a, b). E, The transition
from regular firing to bursting was associated with a progressive
decrease in the fast AHP and an increase in size of the spike ADP, as
shown in the overlay of the expanded traces from b in
A-D.
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Similar concentration-dependent effects were seen in 15 of 20 PCs
exposed to graded reductions in
[Ca2+]o, although
the final grade of bursting attained in
Ca2+-free saline varied among the neurons.
As summarized in Figure 3, lowering
[Ca2+]o from 2 to
1.2 mM converted 8 of 17 nonbursters to HTBs. Further reduction to 0.5 mM converted many of the HTBs to LTBs.
Subsequent exposure to Ca2-free saline
further augmented the bursting propensity of these LTBs. Spontaneous
intrinsic bursters (grade III LTBs) were encountered only in nominally
Ca2+-free saline in 5 of the 20 PCs (25%)
in this sample.

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Figure 3.
The firing patterns of CA1 PCs in different
Ca2+o concentrations. The firing
patterns of 20 CA1 PCs was monitored while
[Ca2+]o was reduced in a stepwise
manner from 2 mM (standard saline) to 0 mM
(Ca2+-free saline). In control conditions, 17 PCs
were nonbursters, 2 were HTBs, and only 1 was a grade I LTB. The
lines in the graph depict the direction
of change in firing pattern within each subclass of PCs when
[Ca2+]o is lowered to the next
concentration. Thus, of the 17 native nonbursters, 8 PCs became HTBs in
1.2 mM Ca2+ and LTBs in 0.5 mM Ca2+, another 4 PCs became HTBs in
0.5 mM Ca2+, and the remaining 5 PCs did
not change at all.
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The waveform of intrinsic bursts in low
[Ca2+]o was
similar to that of native intrinsic bursts (Jensen et al., 1994
, 1996
). The number of intraburst spikes varied between three and seven across
different cells (averaging 3.5 ± 1.1; n = 40) but
was rather constant in any given cell. The initial and mean firing
rates during a burst were 178.7 ± 28.8 and 134.7 ± 28.2 Hz
(n = 40), respectively.
Effects of lowering [Ca2+]o on the
spike ADP
Lowering
[Ca2+]o did not
significantly affect resting membrane potential, input resistance, or
time constant, nor did it affect spike threshold or amplitude (Table
1). However, it strongly modulated the
spike afterpotentials, namely the fast AHP and ADP, in most
PCs. As illustrated in Figure 2E, lowering
[Ca2+]o reduced
the fast AHP and augmented the size of the ADP in a concentration-dependent manner. On average, changing from standard to
Ca2+-free saline reduced the fast AHP by
5.8 ± 4.0 mV and variably augmented the spike ADP by 63.2 ± 54.8% (n = 40) (Table 1).
During the lowering of
[Ca2+]o, the size
of the spike ADP and the propensity to burst increased in parallel
(Fig. 2). Accordingly, the final size of the spike ADP in
Ca2+-free saline was significantly larger
in bursters (275.9 ± 103.7 mV · msec;
n = 33) than in nonbursters (196.4 ± 54.2 mV · msec; n = 7). These observations are
consistent with the notion that intrinsic bursts are triggered by
suprathreshold spike ADPs (Kandel and Spencer, 1961
; Jensen and Yaari,
1996
).
Effects of INaP blockers on low
[Ca2+]o-induced intrinsic bursting
In pharmacologically untreated CA1 PCs, somatic intrinsic bursting
is driven by INaP (Azouz et al.,
1996
). We examined whether a similar ionic mechanism underlies
intrinsic bursting in low [Ca2+]o by testing
its sensitivity to three drugs previously shown to reduce
INaP in CA1 PCs, namely tetrodotoxin
(TTX), the anti-epileptic drug phenytoin, and the protein kinase C
(PKC) activator PDB. Representative results are shown in Figure
4.

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Figure 4.
Blockers of INaP
suppress intrinsic bursting in low
[Ca2+]o. Recordings were made
from four grade II LTBs in Ca2+-free saline.
Burst firing was evoked by 3 msec depolarizing stimuli.
A, The responses of the neuron are shown before
(a) and 5 and 20 min after (b and
c, respectively) adding 0.1 µM TTX to the
Ca2+-free saline, which caused a gradual suppression
of intrinsic bursting. B, The responses of the neuron
are shown before (a), 30 min after adding 50 µM phenytoin to the Ca2+-free saline
(b), and 30 min after wash of phenytoin
(c). C, The responses of
the neuron are shown before (a) and 30 min after
(b) adding 5 µM PDB to the
Ca2+-free saline (b). Both
phenytoin and PDB blocked the burst response completely but affected
the first spike very little. D, The responses of the
neuron are shown before (a) and 45 min after
(b) adding 50 µM PDC to the
Ca2+-free saline. No effect of this drug was
noted.
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Tetrodotoxin
This agent blocks both transient Na+
current and INaP in CA1 PCs (French et
al., 1990
). As illustrated in Figure 4A,
adding 0.1 µM TTX to the saline caused a
progressive block of the burst responses concurrent with an increase in
spike threshold. Longer exposures to TTX caused complete suppression of
spike responses (data not shown). Similar results were consistently
obtained in seven PCs.
Phenytoin
Phenytoin was shown to preferentially reduce
INaP in CA1 PCs (Chao and Alzheimer,
1995
; Segal and Douglas, 1997
). We tested in nine PCs the effects of
50-100 µM phenytoin on low
Ca2+-induced intrinsic bursting. In all
cases, phenytoin reversibly suppressed intrinsic bursting, as
illustrated in Figure 4B. Concurrently, phenytoin
caused a small (3.36 ± 3.26 mV) but significant increase in spike
threshold (from
54.0 ± 2.6 to
50.8 ± 2.9 mV;
n = 9) but did not significantly affect spike
amplitude. Unlike TTX, phenytoin did not suppress the initiation of
single spikes even after a prolonged (>1 hr) exposure.
Phorbol esters
In CA1 PCs, activation of PKC suppresses
INaP (Alroy et al., 1999
). Application
of 2-10 µM PDB, a phorbol ester that potently activates PKC (Castagna et al., 1982
), suppressed low
Ca2+-induced intrinsic bursting within
30-45 min (Fig. 4C). The effect was irreversible with 1 hr
wash, but similar effects were seen in all nine bursters tested with
this drug. Like phenytoin, PDB also caused a small (~4 mV) increase
in spike threshold but did not significantly affect spike amplitude.
To control for unspecific phorbol ester effects, we exposed
slices for up to 1 hr to 50 µM PDC, a phorbol
ester that does not activate PKC (Castagna et al., 1982
). In all cases
(n = 4), PDC did not affect intrinsic bursting (Fig.
4D).
Effects of INaP blockers on low
[Ca2+]o-enhanced spike ADPs
In a fraction of the PCs, changing to
Ca2+-free saline enhanced the spike ADP,
but not sufficiently to trigger a burst in response to a brief stimulus
(i.e., HTBs and grade I LTBs) (Fig.
1B,C). We tested in these neurons
the effects of the three INaP blockers on the enhanced spike ADPs. As illustrated in Figure
5, the spike ADP was consistently
suppressed by 0.1-0.2 µM TTX (Fig.
5A) (n = 4), 50-100
µM phenytoin (Fig. 5B)
(n = 9), and 2-10 µM PDB (Fig. 5C) (n = 9), but not by 50 µM PDC (n = 3; data not shown).
These results are consistent with the notion that the enhanced spike ADPs in low
[Ca2+]o are driven
primarily by INaP.

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Figure 5.
Blockers of INaP
suppress spike ADPs in low [Ca2+]o.
A-C, Recordings of single spikes evoked by 3 msec
stimuli were made in three CA1 PCs in slices perfused sequentially with
standard saline (2 Ca2+),
Ca2+-free saline (0
Ca2+), and Ca2+-free
saline containing a drug known to suppress
INaP. In the three PCs the native spike was
followed by an active ADP. Lowering
[Ca2+]o caused spike broadening,
blocked the fast AHP, and enhanced the active ADP. The latter potential
was completely depressed after 20 min exposure to 0.2 µM TTX (A). Likewise, it was
markedly reduced after 30 min exposure to 50 µM
phenytoin (B) or 5 µM PDB
(C).
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Effects of INaP blockers on low
[Ca2+]o-enhanced subthreshold ADPs
When CA1 PCs are depolarized with a brief current pulse to near
threshold potential, the membrane potential decays back to resting
potential more slowly than expected from the membrane time constant.
These subthreshold ADPs are readily blocked by TTX, but not by
Ca2+ channel blockers (Azouz et al.,
1996
), suggesting that they are generated by
INaP, the activation threshold of
which is slightly more negative than spike threshold (French et al.,
1990
). We tested the effects of lowering
[Ca2+]o on these
potentials. In all cases (n = 22), as illustrated in
Figure 6, deleting
Ca2+o markedly
enhanced the subthreshold ADPs. Thus, the waveform of these potentials
increased significantly from 134.9 ± 50.3 to 333.5 ± 71.2 mV · msec after changing from standard to
Ca2+-free saline. Consistent with the
notion that they are generated by
INaP, these potentials were readily
blocked by 0.1-0.2 µM TTX (Fig.
6A) (n = 4), 50-100
µM phenytoin (Fig. 6B)
(n = 9), and 2-10 µM PDB (Fig.
6C) (n = 9).

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Figure 6.
Blockers of INaP
suppress subthreshold ADPs in low
[Ca2+]o. A-C,
Recordings of subthreshold ADPs evoked by 3 msec threshold-straddling
stimuli were made in three CA1 PCs in slices perfused sequentially with
standard saline (2 Ca2+),
Ca2+-free saline (0
Ca2+), and Ca2+-free
saline containing a drug known to suppress
INaP. In the three PCs, when the stimulus
failed to trigger a spike, it evoked a slow depolarizing
potential that declined more slowly to resting potential than
expected from passive membrane charging. Lowering
[Ca2+]o induced a subthreshold ADP in
these PCs. The latter potential was suppressed by 0.2 µM TTX (20 min; A), 50 µM phenytoin (30 min; B), and 2 µM PDB (40 min; C).
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Effects of Ca2+ current block
with Ni2+
The results described above established that low
[Ca2+]o-induced
intrinsic bursting is most likely driven by
INaP. However, they did not indicate
the mechanism by which lowering
[Ca2+]o augments
the slow potentials that trigger the burst discharge. One possibility
is that lowering
[Ca2+]o reduces
outward Ca2+-activated
K+ currents, thereby increasing the
depolarizing impact of INaP (Azouz et
al., 1996
). Alternatively, lowering
[Ca2+]o may
upmodulate INaP itself. The first
hypothesis predicts that blocking Ca2+
channels pharmacologically also would induce intrinsic bursting. We
tested this notion in four nonbursters by adding 1 mM Ni2+ (in
replacement of 1 mM
Mg2+) to the standard saline that perfused
the slices. Consistent results were obtained in all cases and are
illustrated in Figure 7. Adding
Ni2+ suppressed the fast AHP (Fig. 7,
compare a in A and B), as expected from block of the fast Ca2+-activated
K+ current
(Ic) (Storm, 1987
). Likewise, it
suppressed the slow AHP that follows a train of several spikes, which
is generated by the slow Ca2+-activated
K+ current
(IAHP) (Madison and Nicoll, 1984
), as
well as the associated spike frequency accommodation (Fig. 7, compare
b in A and B). Despite the apparent
block of these K+ currents, the
nonbursting pattern of the PC did not change (Fig. 7, compare
c in A and B). Yet, bursting was
readily induced in the Ni2+-containing
saline by deleting Ca2+ from the solution
(Fig. 7C, c).

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Figure 7.
Block of Ca2+-activated
K+ currents with Ni2+ does not
induce intrinsic bursting. Recordings were obtained from a native
nonbursting CA1 PC. Shown are the responses of the neuron to 4 msec
(a), 400 msec (b), and 200 msec depolarizing stimuli (c) in three conditions.
A, In standard saline, the solitary spike was followed by
distinct fast AHP and ADP (a), and repetitive firing was
followed by a medium AHP and slow AHPs (b). B,
After the change to standard saline containing 1 mM Ni2+, the fast
and slow AHPs were suppressed, whereas the medium AHP was preserved
(a, b). Despite the reduction in spike frequency
accommodation (b), the nonbursting firing pattern of the PCs
was unaltered (c). C, Changing to
Ca2+-free saline containing 1 mM Ni2+
(b) converted the PC to a grade I LTB (c).
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Effects of buffering intracellular Ca2+
with BAPTA
As an additional test for the role of
Ca2+-activated currents in shaping the
firing mode of CA1 PCs, we injected seven neurons with the
Ca2+ chelator BAPTA by applying negative
current pulses (up to 0.5 nA; 10-30 min). The effects of BAPTA were
similar in all cases. As illustrated in Figure
8, BAPTA injection expectedly suppressed the fast AHP (Fig. 8, compare a in A and
B), the slow AHP, and the associated spike frequency
accommodation (Fig. 8, compare b in A and
B). Despite these effects, BAPTA injection did not induce
intrinsic bursting (Fig. 8, compare c in A and
B). However, bursting was readily induced in the
BAPTA-injected neuron by removing Ca2+o (Fig.
8C, c).

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Figure 8.
Buffering of intracellular Ca2+
concentration with BAPTA does not induce intrinsic bursting. Recordings
were obtained from a native nonbursting CA1 PC. Shown are
the responses of the neuron to 4 msec
(a), 400 msec (b), and 200 msec depolarizing stimuli (c) in three conditions.
A, In standard saline, the solitary spike was followed by
distinct fast AHP and ADP (a), and repetitive firing was
followed by a medium and slow AHPs (b). B,
Injecting BAPTA into the neuron suppressed the fast and slow AHPs and
reduced spike frequency accommodation (a, b), but
the nonbursting firing pattern of the PC was unaltered (c).
C, Changing to Ca2+-free saline
converted the PC to a grade I LTB (c).
|
|
Effect of low [Ca2+]o on
slow spikes
Perfusing CA1 PCs with standard saline containing 10 mM TEA, which blocks various voltage-gated
K+ currents in these neurons (e.g.,
delayed rectifier and M-current) (Storm, 1990
), induces compound
slow (duration 100-400 msec) and fast spike responses to brief
depolarizing stimuli. Deleting
Ca2+o converts the
slow spikes to "plateau" potentials lasting 1-2 sec
(García-Muñoz et al., 1993
; Jensen et al., 1996
). These
potentials are blocked by TTX at low concentrations that do not affect
the fast spikes, indicating that they are generated by
INaP. Accordingly, they are also
blocked by phenytoin (H. Su and Y. Yaari, unpublished observations) and
PKC activation (Alroy et al., 1999
).
We tested whether blocking Ca2+-activated
K+ currents with
Ni2+ also induces plateau potentials in
TEA-containing saline. A representative experiment is illustrated in
Figure 9A. In standard saline
containing 10 mM TEA, a brief depolarizing pulse
evoked a complex of several fast spikes riding on a slow spike,
followed by a slow AHP (Fig. 9A, a). Adding 1 mM Ni2+ abolished
the slow AHP and slightly enhanced the slow spike, but did not induce a
plateau potential (Fig. 9A, b). However, deleting
Ca2+ from the
Ni2+-containing saline induced a prolonged
(~1.8 sec) plateau potential (Fig. 9A, c). This
slow potential was blocked entirely by 0.2 µM
TTX before the primary fast spike was affected (Fig. 9A,
d). Similar results were obtained in all experiments
(n = 4).

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Figure 9.
Lowering of
[Ca2+]o, but not block of
Ca2+-activated K+ currents,
induces TTX-sensitive plateau potentials. A, In this
experiment the slice was perfused with standard saline containing 10 mM TEA to block several voltage-gated K+
currents. A constant negative current was injected into the cell to
maintain the native resting membrane potential ( 63 mV).
Suprathreshold responses were evoked by 5 msec positive current pulses.
Salines were exchanged every 30 min. In standard saline containing TEA,
the PC generated a compound response, consisting of fast spikes riding
on a slow spike, and followed by a slow AHP (a).
Adding 1 mM Ni2+ to the saline
suppressed the slow AHP completely and slightly prolonged the slow
spike (b). Deleting Ca2+ from
the saline induced a prolonged plateau potential lasting ~1.8 sec
(c), which was suppressed by 0.2 µM
TTX within 10 min of exposure (d).
B, In another slice perfused with salines containing 10 mM TEA, [Ca2+]o was
reduced in a stepwise manner every 30 min. The responses of the PC to 5 msec pulse stimulation are shown in standard saline
(a), 1.2 mM Ca2+
saline (b), 0.5 mM
Ca2+ saline (c), and
Ca2+-free saline (d). The
control response comprised fast and slow spikes
(a). The duration of the plateau potential
increased as [Ca2+]o decreased
(b-d).
|
|
These results indicated that blocking
Ca2+-activated
K+ currents itself is not sufficient to
induce plateau potentials in TEA-containing saline. Rather,
Ca2+o removal per se
is required for this effect. Indeed, we found that even partial
Ca2+o replacement is
effective in prolonging the slow spike component in TEA-containing
saline (n = 4). As illustrated in Figure 9B,
reducing [Ca2+]o
in a stepwise manner caused a concentration-dependent growth of the
plateau potential (Fig. 9B, a-d).
Effect of low [Ca2+]o on
inward rectification
CA1 PCs display inward rectification, manifested as an apparent
increase in input resistance near action-potential threshold (Hotson et
al., 1979
). A component of inward rectification persists after
suppression of Ca2+ currents and is
blocked by TTX, indicating that it is caused by activation of
INaP (Benardo et al., 1982
). If low
[Ca2+]o
upmodulates INaP, then it should
augment TTX-sensitive inward rectification. We tested this notion in
five slices perfused with saline containing 1 mM
Ni2+ by injecting slow current ramps
(duration 0.9 sec) of increasing magnitude into the PCs. In the example
illustrated in Figure 10, the current
was linearly increased from 0 to 160 pA, causing the neuron to
depolarize from
72 mV to spike threshold potential (approximately
60 mV). In standard saline containing
Ni2+, inward rectification was seen at
membrane potentials more positive than
63.8 mV (Fig.
10A, a). After changing to
Ni2+-containing
Ca2+-free saline, inward rectification
occurred already at
67.1 mV (Fig. 10, trace b). Adding 1 µM TTX completely blocked the inward rectification (Fig. 10, trace c). Similar results were
obtained in all five experiments. On average, the membrane potential at which the membrane began to rectify shifted from
62.0 ± 2.9 to
67.2 ± 2.0 mV after removal of
Ca2+o (a significant
difference of
5.2 ± 1.4 mV).

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Figure 10.
Lowering [Ca2+]o
enhances TTX-sensitive inward rectification. Recordings were obtained
from a native nonbursting CA1 PC. The neuron was injected with current
ramps from 0 to 160 pA (duration 0.9 sec). Plotted are the subthreshold
voltage responses of the neuron to these ramps. Each trace is an
average of four consecutive responses. The slice was first perfused
with standard saline containing 1 mM
Ni2+ to block voltage-sensitive
Ca2+ currents. In these conditions (trace
a), the membrane potential first depolarized linearly from its
resting level ( 72 mV) until 63.8 mV, after which it depolarized
exponentially until spike threshold was attained (at 60 mV). After 30 min of perfusion with Ni2+-containing
Ca2+-free saline (trace b), the
nonlinear response began already at 67.1 mV and was steeper than in
control. Addition of 0.1 µM TTX (trace c)
completely suppressed the nonlinear subthreshold response of the neuron
in 10 min.
|
|
Effects of increasing [Ca2+]o on
native intrinsic bursting and slow spikes
In three experiments we tested how elevating
[Ca2+]o affects
native intrinsic bursting. A representative experiment is illustrated in Figure 11A. In
standard saline, strong positive current pulses evoked an initial burst
response of three spikes (Fig. 11A, a). Raising [Ca2+]o to
4 mM (by substituting 2 mM
Mg2+ with 2 mM
Ca2+) blocked the burst response at all
stimulation intensities (Fig. 11A, b).
This effect reversed after wash with standard saline (Fig. 11A, c). Similar results were obtained in
two additional PCs. The suppression of intrinsic bursting by doubling
[Ca2+]o was
associated with a small (~3 mV) increase in spike threshold.

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Figure 11.
Raising [Ca2+]o
blocks native intrinsic bursting and slow spikes. A, In
this experiment recordings were obtained from a native HTB. Shown are
the responses of the neuron to 200 msec depolarizing stimuli in
standard saline (a), 30 min after switching to
saline containing 4 mM Ca2+
(b), and 30 min after changing back to standard
saline (c). Raising
[Ca2+]o reversibly increased the
threshold for evoking spikes and suppressed the initial burst response
to the depolarizing pulses. B, In another slice perfused
with salines containing 10 mM TEA,
[Ca2+]o was increased to 4 mM. The responses of the PC to 5 msec pulse stimulation are
shown in standard saline (a), after 20 min in 4 mM Ca2+ saline
(b), and after 30 min wash back to standard
saline (c). The slow spike was reversibly
suppressed by doubling [Ca2+]o
(a-c).
|
|
We also tested the effects of raising
[Ca2+]o on the
slow spikes in TEA-containing saline (n = 3). As shown
in Figure 11B, raising [Ca2+]o to 4 mM selectively and reversibly blocked the slow
spike component but spared the fast spike (Fig. 11B,
a-c). Consequently, the slow AHP also was
reversibly blocked by doubling
[Ca2+]o. Similar
results were obtained in all three experiments.
Dye coupling and firing patterns of CA1 PCs in low
[Ca2+]o
Previous work in CA1 PCs suggested that bursters are more likely
to be electrically coupled to each other via gap junctions than
nonbursters (Church and Baimbridge, 1991
). It was suggested that there
may be a causal relationship between electrical coupling and intrinsic
bursting. Presumably, the spread of spikes within a small network of
electrically coupled neurons can generate a burst response in each
neuron, which would appear as an "intrinsic" burst. Because
lowering [Ca2+]o
reportedly increases gap junctional communication and, by implication, electrotonic coupling between CA1 PCs (Perez Velazquez et al., 1994
), we examined whether this effect may contribute to low
[Ca2+]o-induced
intrinsic bursting. To this end, we injected 46 PCs with the dye tracer
biocytin during perfusion with nominally
Ca2+-free saline. Of these, nine
neurons (21.4%) were found to be dye coupled to one, two, or three
other PCs (mean number of PCs in a coupled cluster 2.6 ± 0.9).
However, we found no significant correlation between the firing pattern
of the neuron and the incidence of dye coupling (Table
2). Figure
12 illustrates two exemplary biocytin-injected neurons, a grade II LTB (Fig. 12A,
a and b), which was not coupled to other neurons
(Fig. 12A, c), and a regular firing cell
(Fig. 12B, a and b), which was
coupled to two other PCs (Fig. 12B,
c).

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Figure 12.
Dissociation between dye coupling and intrinsic
bursting in low [Ca2+]o.
A, B, Recordings from two native
nonbursters 30 min after changing to
Ca2+-free saline. Both PCs were stained with
biocytin to detect dye coupling. A, This neuron became a
grade II LTB in low [Ca2+]o, as
is evident from its burst responses to 200 msec
(a) and 3 msec depolarizing current pulses
(b). As shown in the photomicrograph of the
neuron (c), it was not dye coupled to other
cells. B, This neuron remained nonbursting in low
[Ca2+]o (a,
b). Biocytin injection into this cell resulted in the
staining of three PCs (c), suggesting that the
neuron formed gap junctions with one or two other PCs.
|
|
It has been argued recently that in some neurons dye coupling may not
be a reliable indicator for the presence of electrical coupling via gap
junctions (Gibson et al., 1999
). Therefore, we also tested the effect
of the gap junctional blocker doxyl-stearic acid (Strata et al., 1997
;
Zahs and Newman, 1997
) on low
[Ca2+]o-induced
intrinsic bursting. This drug was chosen because unlike other commonly
used gap junction blockers tested (propionate, octanol, halothane, and
carbenoxolone), it exerted no deleterious effects on intrinsic neuronal
properties at concentrations that block neuronal gap junctions (Su and
Yaari, unpublished observations). Addition of 50 µM
doxyl-stearic acid to the Ca2+-free saline
did not affect intrinsic bursting during 45-60 min of perfusion in all
cases (n = 6; data not shown).
Taken together, these data do not support a role for electrical
coupling in the generation of intrinsic bursting in low
[Ca2+]o.
 |
DISCUSSION |
The main finding in this study is that
Ca2+o regulates the
intrinsic firing mode of CA1 PCs. In standard saline containing 2 mM Ca2+, only a small fraction
of these neurons burst-fire in response to somatic depolarization.
Lowering [Ca2+]o
increases, whereas elevating
[Ca2+]o decreases,
the propensity of these neurons to generate bursts. We also show that
intrinsic bursts induced by lowering
[Ca2+]o are driven
by INaP. The simplest hypothesis that
accounts for our findings is that Ca2+
acting extracellularly exerts a depressant effect on noninactivating Na+ channels that generate
INaP. Accordingly, decreases in
[Ca2+]o enhance
intrinsic bursting via increases in
INaP.
Ionic mechanism of intrinsic bursts in low
[Ca2+]o
Several slow inward currents have been implicated in the
generation of somatic bursts in cortical neurons, including
voltage-sensitive Ca2+ (Wong and Prince,
1981
; Foehring and Waters, 1991
; Deisz, 1996
) and
Na+ currents (Franceschetti et al., 1995
;
Azouz et al., 1996
; Mattia et al., 1997
), and a
Ca2+-activated cationic current (Kang et
al., 1998
). In CA1 PCs in vitro, native somatic bursting, as
well as that induced by elevating [K+]o (Jensen et
al., 1994
), are insensitive to block of
Ca2+ currents. Rather, they are suppressed
by blockers of INaP, implicating the
latter current in their generation (Azouz et al., 1996
;
Alroy et al., 1999
). Somatic bursting can be induced in these neurons also by exposure to millimolar concentrations of 4-aminopyridine (4-AP), which blocks several K+
conductances (Magee and Carruth, 1999
). Unlike native bursting, 4-AP-induced bursts are suppressed by Ca2+
channel blockers, consistent with the view that they are generated by
dendritic Ca2+ spikes (Magee and Carruth,
1999
).
Two lines of evidence suggest that somatic bursting in low
[Ca2+]o is driven
by INaP. First, in most experiments
bursting was readily induced in nominally
Ca2+-free saline containing 2 mM Mn2+. Blocking
Ca2+ channels with
Mn2+ in addition to deleting
Ca2+ ensured that neither
Ca2+ currents nor
Na+ currents through
Ca2+ channels (Lux et al., 1990
) were
involved in bursting. Thus, the only slow inward current available in
this saline was INaP. Second,
intrinsic bursting induced by low
[Ca2+]o was
readily suppressed by TTX, phenytoin, and PDB. Although these drugs
interact with voltage-gated Na+ channels
in different ways (Catterall, 1999
), they share a common depressant
effect on INaP.
We have examined three hypotheses that explain why
INaP becomes more effective in
producing intrinsic bursting as
[Ca2+]o is
lowered: (1) suppression of opposing
Ca2+-activated
K+ currents, (2) upmodulation of
INaP itself, and (3) increase in electrotonic coupling through gap junctions. These hypotheses will be
assessed in the following sections.
Suppression of Ca2+-activated
K+ currents
In CA1 PCs, IC activates during
the action potential and contributes largely to the late phase of spike
repolarization (Storm, 1987
). Thus, the density of
IC influences the waveform of the spike ADP and may determine whether it will progress to a burst. We
compared the effects of three experimental manipulations that cause
IC suppression, namely, lowering
[Ca2+ ]o, blocking
Ca2+ currents with extracellular
Ni2+, and preventing intracellular
Ca2+ accumulation with BAPTA. As expected,
all of these manipulations reduced the
IC-dependent fast AHP. However, only
low [Ca2+ ]o
induced intrinsic bursting, indicating that reduction in
IC (or any other
Ca2+-activated current) by itself is not
sufficient to invoke this firing pattern in CA1 PCs. Rather, lowering
[Ca2+ ]o exerts
additional effects that are crucial for the induction of bursting.
Upmodulation of INaP
An attractive possibility is that low
[Ca2+ ]o
upmodulates INaP. We tested this possibility by
monitoring the effects of
Ca2+o removal on
TTX-sensitive plateau potentials and inward rectification that are
generated by INaP. Both the plateau
potentials and inward rectification were enhanced in this condition,
supporting the view that lowering [Ca2+
]o upmodulates
INaP.
In a previous study in supraoptic hypothalamic neurons, lowering
[Ca2+ ]o enhanced
INaP and the associated spontaneous
intrinsic bursting (Li and Hatton, 1996
). However, replacement of
Ca2+ with other divalent cations prevented
these effects, suggesting that they are caused by a net decrease in
extracellular divalent ion concentration (which would shift
INaP activation to more positive potentials by unscreening the external negative membrane surface potential) rather than by a specific decrease in
[Ca2+ ]o. In our
experiments, the concentrations of divalent cations were maintained
constant at 4 mM in all salines, and the
induction of intrinsic bursting occurred regardless of the species of
divalent cations used to replace
Ca2+o. These data
suggest that in CA1 PCs,
Ca2+o decreases
INaP by a mechanism that involves its
selective binding to membrane receptors. The receptors that bind
Ca2+o may be the
Na+ channels themselves (Armstrong and
Cota, 1991
) or G-protein-coupled Ca2+-sensing receptors (Yamaguchi et al.,
2000
), such as metabotropic glutamate receptors (Kubo et al., 1998
),
that may modulate INaP via second
messenger cascades. The latter mechanism is less likely, because 100 µM neomycin (n = 3) and 10 nM gadolinium (n = 3), which
activate Ca2+-sensing receptors (Xiong and
MacDonald, 1999
), failed to reverse the induction of intrinsic bursting
by low [Ca2+ ]o
(Su and Yaari, unpublished observations).
Increase in electrical coupling through gap junctions
We also examined whether augmentation of electrotonic coupling via
gap junctions contributes to the appearance of intrinsic bursting in
low [Ca2+]o. Both
experimental (Getting and Willows, 1974
) and theoretical (Sherman and
Rinzel, 1992
) data suggest that electrotonic coupling can cause neurons
to burst. Indeed, it was shown that raising extracellular pH enhances
both dye coupling (and by implication, electrotonic coupling) and
intrinsic bursting in CA1 PCs and that only PCs coupled to other
neurons display bursting behavior (Church and Baimbridge, 1991
).
Although we found significant dye coupling between CA1 PCs bathed in
low [Ca2+]o, we
could not substantiate a role for electrotonic coupling in the bursting
behavior. First, the incidence of dye coupling among bursters and
nonbursters was the same. Second, the gap junction blocker
doxyl-stearic acid did not affect intrinsic bursting. It should be
noted that both the overall incidence of dye coupling (21.4%)
and the size of a coupled aggregate (two to four cells) in
Ca2+-free saline were much lower than in
high pH saline (88% and two to nine cells, respectively)
(Church and Baimbridge, 1991
). Thus, if electrical coupling via gap
junctions and intrinsic bursting are causally associated, this
mechanism may be more important for intrinsic bursting in high
extracellular pH than in low
[Ca2+]o.
Functional implications
Despite the strict homeostatic control of
[Ca2+]o in the
brain, neuronal activity can cause substantial decreases in
[Ca2+]o (Heinemann
et al., 1977
). In hippocampal slices perfused with 2 mM
Ca2+ saline, repetitive orthodromic
activation of CA1 PCs at
frequencies (5-10 Hz) decreases
[Ca2+]o down to
1.4 mM (Benninger et al., 1980
). This decrease, in combination with an associated increase in
[K+]o (up to 12 mM), would convert many nonbursting PCs into intrinsic bursters. This may explain why
frequency orthodromic activation of
CA1 PCs also leads to the development of postsynaptic bursting (Thomas
et al., 1998
).
The induction of intrinsic bursting by activity-dependent decreases in
[Ca2+]o also may
be germane to the genesis of epileptic seizures. In vivo
recordings of
[Ca2+]o in
experimental models of epilepsy have shown dramatic decreases in
[Ca2+]o (down to
0.2 mM) during seizure activity (Pumain et al.,
1985
). These decreases would be expected to enhance intrinsic bursting, which in turn would contribute to the explosive development and spread
of seizure activity (Jensen and Yaari, 1997
). Consistent with this view
is the finding that lowering
[Ca2+]o to 0.2 mM or less induces spontaneous population bursts
in rat hippocampal slices despite the block of chemical synaptic transmission (Jefferys and Haas, 1982
; Taylor and Dudek, 1982
; Yaari et
al., 1983
).
 |
FOOTNOTES |
Received Aug. 1, 2000; revised March 26, 2001; accepted March 27, 2001.
This work was supported by the Bundesministerium für Bildung
Wissenschaft (BMBF), the Israel Ministry of Science (MOS), and the
Israel Science Foundation (ISF) administered by the Israel Academy of Sciences and Humanities. E.D.K. was supported by a fellowship from Teva Pharmaceuticals Inc.
Correspondence should be addressed to Dr. Yoel Yaari, Department of
Physiology, Hebrew University School of Medicine, P.O. Box 12272, Jerusalem 91121, Israel. E-mail:
yaari{at}md2.huji.ac.il.
 |
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