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The Journal of Neuroscience, July 1, 1999, 19(13):5205-5212
Calcium-Activated Potassium Conductances Contribute to Action
Potential Repolarization at the Soma But Not the Dendrites of
Hippocampal CA1 Pyramidal Neurons
Nicholas P.
Poolos and
Daniel
Johnston
Division of Neuroscience, Baylor College of Medicine, Houston,
Texas 77030
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ABSTRACT |
Evidence is accumulating that voltage-gated channels are
distributed nonuniformly throughout neurons and that this nonuniformity underlies regional differences in excitability within the single neuron. Previous reports have shown that Ca2+,
Na+, A-type K+, and
hyperpolarization-activated, mixed cation conductances have varying
distributions in hippocampal CA1 pyramidal neurons, with significantly
different densities in the apical dendrites compared with the soma.
Another important channel mediates the large-conductance Ca2+-activated K+ current
(IC), which is responsible in part for
repolarization of the action potential (AP) and generation of the
afterhyperpolarization that follows the AP recorded at the soma. We
have investigated whether this current is activated by APs retrogradely
propagating in the dendrites of hippocampal pyramidal neurons using
whole-cell dendritic patch-clamp recording techniques. We found no
IC activation by back-propagating APs in
distal dendritic recordings. Dendritic APs activated
IC only in the proximal dendrites, and
this activation decayed within the first 100-150 µm of distance from
the soma. The decay of IC in the proximal
dendrites occurred despite AP amplitude, plus presumably AP-induced
Ca2+ influx, that was comparable with that at the
soma. Thus we conclude that IC activation
by action potentials is nonuniform in the hippocampal pyramidal neuron,
which may represent a further example of regional differences in
neuronal excitability that are determined by the nonuniform
distribution of voltage-gated channels in dendrites.
Key words:
dendrites; hippocampus; calcium-activated potassium
conductances; back-propagation; action potentials; patch clamp; calcium
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INTRODUCTION |
Recent advances in recording
techniques have shown that voltage-gated channels are distributed
nonuniformly throughout the hippocampal pyramidal neuron; these include
Ca2+ channels (Elliott et al., 1995 ; Magee and
Johnston, 1995a ) and Na+ channels, which have a
relatively constant density throughout the cell but differ in their
inactivation properties between the soma and dendrites (Colbert et al.,
1997 ; Mickus et al., 1999 ). The distributions of the transient A-type
K+ current and the hyperpolarization-activated
cation current (Ih) both show dramatic
nonuniformity, increasing in density with distance in the apical
dendrites (Hoffman et al., 1997 ; Magee, 1998 ). The differential
distribution of these voltage-gated channels between soma and dendrites
yields significant differences in excitability between these two
regions. For example, the increased A-current density causes the
dendrites to be relatively less excitable than the soma, such that with
increasing distance from the soma, dendritic action potential (AP)
amplitude progressively decreases, and the threshold for AP initiation
increases (Hoffman et al., 1997 ).
Less is known about the distribution of
Ca2+-activated K+ channels in
neurons, in particular the current generated by the large-conductance Ca2+-activated K+ channel or
BK channel. This current (here abbreviated
IC) has been studied with somatic
recordings at the hippocampal pyramidal neuron, as well as in many
other neurons (for review, see Sah, 1996 ; Vergara et al., 1998 ). The BK
channels that underlie IC generate a high
single-channel conductance for K+, are both voltage-
and Ca2+-sensitive, rapidly open with
[Ca2+]i rises in the range of 1-10
µM, and are blocked by charybdotoxin (CTX) and
submillimolar concentrations of tetraethylammonium (TEA) (Barrett et
al., 1982 ; Blatz and Magleby, 1984 ). IC
activation occurs with Ca2+ influx induced by APs
and contributes to the rapid repolarization of the AP and subsequent
fast afterhyperpolarization (AHP) (Lancaster and Adams, 1986 ; Storm,
1987 ). This current is distinct from that generated by
small-conductance Ca2+-activated
K+ channels (SK), which are Ca2+-
but not voltage-sensitive, activate slowly in response to submicromolar rises in [Ca2+]i, show varying
sensitivity to apamin, and generate the slow AHP after a train of APs
(Lancaster and Zucker, 1994 ; Sah, 1996 ; Vergara et al., 1998 ).
Although the role of IC in repolarizing
the AP is well documented for APs initiated at the soma of hippocampal
pyramidal neurons, it is unknown whether this current is present in the
dendrites and whether it contributes to the repolarization of the
dendritic AP. Since the initial descriptions of retrograde AP
propagation in the dendrites (or "back-propagation"), it has been
appreciated that dendritic APs differ from somatic APs in that the
amplitude of dendritic APs is variable, diminishing with distance from
the soma, they lack an afterhyperpolarizing phase, and their
repolarization is slower (Andreasen and Lambert, 1995 ; Spruston et al.,
1995 ; Colbert et al., 1997 ). We therefore questioned whether
IC is activated by APs back-propagating in
the dendrites as it is by APs at the soma. Because we were interested
in assessing this functional role of IC,
we used whole-cell patch-clamp recordings in the dendrites of
hippocampal CA1 pyramidal neurons to measure
IC activation by back-propagating action potentials.
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MATERIALS AND METHODS |
Hippocampal slices were prepared from 6- to 10-week-old
male Sprague Dawley rats. Animals were anesthetized with a lethal dose
of a combination of ketamine, xylazine, and acepromazine injected
intraperitoneally. After being deeply anesthetized, the animal was
perfused intracardially with ice-cold modified artificial CSF
containing (in mM): 110 choline chloride, 2.5 KCl, 1.25 NaH2PO4, 0.5 CaCl2, 7 MgCl2, 7 dextrose, 3 pyruvic acid, and 1.3 ascorbic acid. The brain was then removed, and 400-µm-thick slices were prepared using a vibratome (Lancer). Hippocampal slices were stored until use in a holding chamber containing external recording solution at room temperature.
Recordings from hippocampal pyramidal neurons were obtained from slices
maintained in a submerged chamber at 30-32°C. The external recording
solution contained (in mM): 125 NaCl, 2.5 KCl, 1.25 NaH2PO4, 2 CaCl2, 2 MgCl2, and 10 dextrose, bubbled continuously with
95% O2/5% CO2; pH was adjusted
to 7.4 with NaOH. The internal recording pipette solution contained (in
mM): 120 KMeSO4, 20 KCl, 10 HEPES,
2 MgCl2, 4 Na2-ATP, 0.3 Tris; pH was
adjusted to 7.3 with KOH.
Whole-cell patch-clamp recordings were made from hippocampal CA1
pyramidal neuron somata and dendrites that were visualized using
infrared differential interference contrast microscopy (IR-DIC; Zeiss
Axioskop). Pipettes were fabricated with a Flaming-Brown puller
(Sutter Instruments) using borosilicate glass (Fisher Scientific, Houston, TX) and had DC resistances of ~10 M . Whole-cell
recordings were obtained with a bridge-mode amplifier (Dagan BVC-700),
digitized at 10 kHz (IOTech), and stored with custom data acquisition
software. Whole-cell series resistance was 10-25 M for somatic
recordings and 15-50 M for dendritic recordings. Recordings without
stable series resistance were discarded. Antidromic action potentials were elicited by constant-current pulses (WPI) delivered by a tungsten
electrode (AM Systems) placed in the alveus. Recordings are shown with
stimulus artifacts truncated for clarity. In some cases, action
potentials were elicited by brief depolarizing current pulses delivered
through the somatic recording pipette. All drugs were bath-applied.
CNQX (10 µM; Research Biochemicals, Natick, MA) and
bicuculline methiodide (25 µM; Sigma, St. Louis, MO) were routinely added to the external solution to block postsynaptic potentials. Charybdotoxin (Alomone Laboratories) was prepared and
applied in a solution of 0.01% bovine serum albumin (Sigma) to prevent
nonspecific binding of the toxin to tubing. Application of bovine serum
albumin-containing solution alone had no apparent effect on action
potential firing (data not shown).
Changes in somatic action potential repolarization were quantified by
measuring the linear slope of repolarization (volts per second) at two
time points on the repolarizing phase of the AP: one at 80% of peak AP
amplitude (measured peak to baseline) and the other at 20% of peak
amplitude. This method allowed measurement of the rate of AP
repolarization over a reasonably linear segment of the waveform, as was
used by Storm (1987) . Dendritic APs were measured similarly except that
the second point was taken at 30% of peak amplitude; because dendritic
APs have a slower, more exponential late phase in repolarization,
measuring between the 80 and 30% points captured a more linear segment
of repolarization. In experiments (see Fig. 6) in which the
change in repolarization was compared in the soma and at varying
distances along the dendrites, the repolarization slope in both soma
and dendrites was measured at the 80-30% points for consistency.
Changes in repolarization are shown as the percent decrease in
repolarization; that is, slower repolarization is represented by a
positive number. Data are reported as mean ± SEM.
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RESULTS |
Dendritic action potentials lack a fast afterhyperpolarization
Whole-cell patch-clamp recordings were obtained from visualized
CA1 hippocampal pyramidal neurons either at the soma or in the apical
dendrites at distances up to 200 µm from the soma (Fig. 1A). Antidromic
activation of single APs or trains of APs by alvear stimulation
resulted in an AP that was recorded at the soma [but presumably
initiated at the axon initial segment or first node of Ranvier (see
Colbert and Johnston, 1996 )] and then propagated retrogradely
(back-propagated) into the apical dendrites (Spruston et al., 1995 ).
Action potentials recorded in the dendrites differed from their somatic
counterparts in several ways (Fig.
1B,C). First, the amplitude of
single dendritic APs declined with distance from the soma beyond ~70
µm, such that at the mean distal dendritic recording location
(174 ± 5 µm; n = 9), their amplitude was
57.5 ± 2.7 mV, compared with 98.4 ± 1.1 mV
(n = 8) at the soma. Second, during a train of APs, the
amplitude of dendritic APs declined continually during the course of
the train, whereas the amplitude of somatic APs remained constant.
Finally, single dendritic APs had a significantly slower repolarization
than did somatic APs and lacked the fast afterhyperpolarizing phase
present in somatic APs. These observations were consistent with
previous reports on dendritic AP characteristics (Andreasen and
Lambert, 1995 ; Colbert et al., 1997 ).

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Figure 1.
Back-propagating APs recorded in the apical
dendrites lack a fast AHP. A, Hippocampal CA1
pyramidal neurons were visualized using IR-DIC optics. The large
arrow points to cell soma; the small arrow
points to the apical dendrite ~150 µm from the soma, where a patch
pipette can be faintly seen. B, Top,
Back-propagating dendritic action potentials (trace
shown) differ from somatic action potentials in their smaller
amplitude, slower repolarization, and lack of a fast AHP.
Bottom, When APs were repetitively stimulated, dendritic
APs decremented in amplitude over the course of the train.
C, Top, Somatic action potentials showed
much faster repolarization and a fast AHP (arrowhead)
after the AP. Bottom, When repetitively stimulated,
somatic APs had a nearly constant amplitude. Synaptic blocks were
omitted in this experiment.
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Repolarization of action potentials in distal dendrites is
not affected by Ca2+ channel blockade
Although dendritic action potentials clearly lacked a fast AHP, it
was not clear whether Ca2+-activated
K+ currents contributed to dendritic AP
repolarization without producing an overt AHP. To study this question,
we elicited single antidromic APs in control solution and in solution
with 100-200 µM Cd2+ added. With
action potentials recorded at the soma, the blockade of
Ca2+ channels with Cd2+ caused
slowing of repolarization and blockade of the fast AHP (Fig.
2A,B).
Similar results were also obtained with solutions containing 0 Ca2+ and 6 mM Mg2+
(data not shown). When this effect was quantified by measuring the
decrease in the rate of repolarization (as described in Materials and
Methods), the blockade of Ca2+ channels caused a
34.7 ± 4.7% (n = 8) decrease in repolarization rate. This result was consistent with the previous work of Storm (1987) , who found that a decrease of 38 ± 6.3% in repolarization rate appeared to represent the effect of maximal blockade of
IC on AP repolarization at the soma.

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Figure 2.
Repolarization of action potentials in the distal
dendrites is not affected by Ca2+ channel blockade.
A, Top, Action potentials recorded at the
soma are shown under control and 100 µM
Cd2+ conditions. Right, Superimposed
APs show that Ca2+ channel blockade significantly
slowed AP repolarization and blocked the fast AHP
(arrow). Bottom, Repolarization of
dendritic APs was not significantly affected by Ca2+
channel blockade. B, The same responses presented in
A (right) are shown at a longer time
scale to show block of the fast AHP (arrow) at the soma
by 100 µM Cd2+. C,
Summary of data shows the average decrease in AP repolarization
(repol.) slope between control and
Ca2+ channel blockade conditions (grouped data from
100-200 µM Cd2+ and from 0 Ca2+ and 6 mM Mg2+
solutions; n = 8 for soma, n = 9 for dendrite).
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In contrast, the repolarization of dendritic action potentials obtained
>150 µm from the soma was not affected by the blockade of
Ca2+ channels with Cd2+ (Fig.
2A,B). This lack of effect was
evident despite prolonged solution superfusion times (up to 30 min) and
was similarly observed with 0 Ca2+ and 6 mM Mg2+ solutions. Quantification of the
effect of Ca2+ channel blockade on distal dendritic
AP repolarization showed a 1.3 ± 5.5% (n = 9)
slowing of action potential repolarization (i.e., a small increase in
repolarization rate that was not significantly different from 0).
Comparison of the effects of Ca2+ channel blockade
on AP repolarization at the soma and distal dendrites (Fig.
2C) showed this effect was significantly different between
the two groups (p < 0.0005). This result shows
that for the distal dendrites, Ca2+-activated
conductances do not contribute to action potential repolarization as
they do at the soma. In dendritic recordings obtained in the proximal
dendrites at distances <150 µm from the soma,
Ca2+ channel blockade had an effect on AP
repolarization that was intermediate between that at the soma and in
the distal dendrites. The results obtained in the proximal dendrites
are further discussed below.
Blockade of Ca2+-activated K+
channels does not affect repolarization of dendritic action
potentials
To determine whether IC contributes
to AP repolarization in the dendrites, we applied blockers of this
current and elicited back-propagating APs. As shown in Figure
3A, bath application of
CTX (30 nM), a potent blocker of BK channels at
nanomolar concentrations (Miller et al., 1985 ), caused significant
broadening of the somatic action potential. This effect was fairly
rapid in onset (4-5 min after initiation of perfusion) but had a slow
and incomplete reversal after washing in control saline (data not
shown). Application of CTX caused a 37.1 ± 3.7%
(n = 3) decrease in the repolarization slope of somatic
APs, similar in magnitude to the slowing caused by
Ca2+ channel blockade. The AP broadening that
occurred in CTX differed from that with Ca2+ channel
blockers in that CTX caused broadening that began at an earlier point
on the repolarizing waveform. This difference may stem either from the
possible presence of other voltage-gated non-Ca2+-dependent K+ channels
that are sensitive to CTX [such as Kv1.3 (Kaczorowski et al., 1996 )]
or from the contribution of inward Ca2+ currents to
the AP waveform, which would be blocked by Cd2+ but
unaffected by CTX.

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Figure 3.
Blockade of Ca2+-activated
K+ currents does not affect repolarization of
dendritic action potentials. A, Top,
Action potentials recorded at the soma showed slowing of repolarization
and blockade of the fast AHP (arrow) by CTX, an
inhibitor of large-conductance Ca2+-activated
K+ conductances. Bottom,
Repolarization of dendritic action potentials was not affected by CTX.
B, TEA, in low concentrations, blocks
IC to the exclusion of most other
K+ channels. Application of TEA (1 mM)
slowed AP repolarization at the soma (top), while having
a minimal effect on dendritic APs (bottom).
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In contrast, application of CTX caused no significant change in the AP
waveform recorded in the dendrites (Fig. 3A), despite perfusion times up to 25-30 min. CTX caused a 1.36 ± 10.1%
(n = 3) decrease in repolarization rate, which was
significantly different from the repolarization slowing at the soma
caused by CTX (p < 0.01). This result, obtained
with a high-affinity blocker of IC, is a
specific demonstration that IC makes
little contribution to the repolarization of dendritic action
potentials. Similar effects were obtained with perfusion of TEA
at concentrations (0.5-1 mM) that primarily affect
IC (Storm, 1987 ; Rudy, 1988 ). As shown in
Figure 3B, TEA caused somatic AP broadening (29.4 ± 4.7%; n = 3) that was similar in appearance to that of
CTX. No significant effect was seen when TEA was applied during
dendritic recordings (0.22 ± 4.4%; n = 4;
p < .005), further demonstrating that
IC makes little or no contribution to AP
repolarization in the distal dendrites.
Repetitive firing does not cause activation of dendritic
IC
Because it was apparent that single back-propagating dendritic APs
did not cause activation of IC, we
questioned whether this might be a result of insufficient
Ca2+ influx during a single dendritic AP. Previous
work using imaging of intracellular Ca2+
concentration ([Ca2+]i) had
demonstrated that repetitive firing of back-propagating APs led to
increases in [Ca2+]i in CA1 pyramidal
neuron dendrites that progressively increased with the number of APs
for brief trains of stimuli (Jaffe et al., 1992 ; Callaway and Ross,
1995 ). Thus, we investigated whether repetitive firing of
back-propagating APs could lead to activation of dendritic
IC.
Trains of five back-propagating APs were elicited by antidromic
stimulation at 20 Hz under control and Ca2+ channel
blockade conditions (Fig. 4). Somewhat
surprisingly, there was little change in the somatic AP broadening by
Ca2+ channel blockers when compared at the beginning
and end of the train. In the example shown in Figure
4A, application of 200 µM Cd2+ caused a fairly constant slowing of
repolarization for all APs in the train, with a 39.9% slowing of the
first AP and a 41.1% slowing of the last AP in the train. This
suggests that activation of IC at the soma
is nearly maximal with a single action potential.

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Figure 4.
Repetitive firing does not cause activation of
dendritic IC. A,
Top, Short trains of antidromic action potentials were
elicited in control and Cd2+ solutions.
Bottom, Comparison of superimposed APs in control and
Cd2+ solutions from the beginning
(left) and end (right) of the train shows
that Ca2+ channel blockade had a similar effect on
AP repolarization (arrow) at the beginning and end of
the train. This suggests that IC
activation was nearly maximal with the first AP. B, A
similar comparison of dendritic APs shows that
IC was minimally activated at both the
beginning (bottom left) and end (bottom
right) of the train of APs.
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When the effect of Ca2+ channel blockade was studied
during repetitive firing of dendritic APs, it was found that
Ca2+ channel blockers continued to have no effect on
AP repolarization despite repetitive firing. As shown in Figure
4B, comparison of APs elicited at the beginning and
end of a 20 Hz train of stimuli shows that Ca2+
channel blockade has little or no effect on AP repolarization throughout the train. Thus, despite presumably rising levels of dendritic [Ca2+]i during repetitive
firing, there is no evidence of dendritic IC activation by back-propagating action potentials.
Activation of IC diminishes in the
proximal dendrites
One factor that could underlie the absence of
IC activation by action potentials in the
distal dendrites might be the diminished amplitude of back-propagating
APs with increasing dendritic distance. Because the activation of
IC is both voltage- and
Ca2+-dependent, decreased peak AP amplitude would
decrease IC activation both because of the
decreased peak depolarization and because of decreased
Ca2+ influx through intrinsic voltage-gated
Ca2+ conductances. To investigate this possibility,
we studied the relation of IC activation
and AP amplitude in the proximal dendrites where AP amplitude
starts to decline from its value at the soma.
Dendritic recordings were obtained in the proximal dendrites at
distances between 25 and 150 µm, and the effect of
Ca2+ channel blockade with 200 µM
Cd2+ on AP repolarization was measured. Recordings
from several distances are shown in Figure
5. Comparing the effects at the soma and
at increasing distances in the proximal dendrites, it appears that the
effect of Cd2+ on AP repolarization is maximal at
the soma and then progressively declines with distance in the proximal
dendrites. A plot of the decrease in AP repolarization slope in
Cd2+ versus dendritic distance (Fig.
6A) shows that the
effect of Ca2+ channel blockade decreases
continuously with distance, with the decrease in repolarization
equaling one-half of the somatic value at a distance of ~70 µm from
the soma.

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Figure 5.
Activation of IC
diminishes in the proximal dendrites. A, Action
potentials recorded at the soma showed a marked slowing of
repolarization in 200 µM Cd2+
(arrow). B-D, Action potentials recorded
in the proximal dendrites at progressively greater distances from the
soma showed a gradual decrease in the activation of
IC (arrows).
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Figure 6.
The decrease in dendritic
IC activation does not depend on action
potential amplitude. A, A plot of the decrease in action
potential repolarization rate with Ca2+ channel
blockade versus distance in the dendrites from the soma. In this case,
the repolarization rate at both the soma and dendrites was computed as
the slope of AP repolarization measured between 80 and 30% of action
potential amplitude. Each point represents a single experiment, with
the values at the soma (dendritic distance = 0) and at 174 µm
(mean distal dendritic recording location) representing the mean values
of experiments at that location (n = 8 at the soma;
n = 9 in the distal dendrites). Note that
IC activation decreased continuously from
its value at the soma with increasing dendritic distance.
B, The decrease in repolarization slope
(squares) and AP amplitude (triangles)
normalized to these values at the soma and plotted versus dendritic
distance. [The SEM of the mean AP amplitude (ampl.) in
the distal dendrites was less than the symbol size.] In
the proximal dendrites up to ~70 µm, AP amplitude was nearly
invariant, whereas the activation of IC
declined. Thus, the diminishing activation of
IC in the dendrites was not a function of
decreasing AP amplitude.
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When the amplitude of the back-propagating AP was normalized to its
value at the soma and plotted versus dendritic distance (Fig.
6B), it can be seen that AP amplitude in the
dendrites remains similar to its value in the soma (~100 mV) for the
first ~70 µm of the proximal dendrites and then begins to decline
such that at 175 µm, AP amplitude is ~0.6 of its value at the soma
(or ~60 mV). Comparison of the normalized decrease in AP
repolarization with AP amplitude shows that in the first 70 µm of the
proximal dendrites, the AP repolarization change progressively
diminished while AP amplitude remained nearly constant. For example, at
70 µm, AP amplitude is similar to the somatic value, whereas the change in repolarization is approximately one-half its value at the
soma. Thus, the decrease in IC activation
in the dendrites appears unrelated to AP amplitude. It is likely that
other factors account for the decline of dendritic
IC activation, such as a decreased density
of Ca2+-activated K+ channels in
the dendrites or a similar decrease in the density of dendritic
voltage-gated Ca2+ channels activated by
back-propagating APs.
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DISCUSSION |
In this study we have investigated action potential repolarization
in the distal dendrites of CA1 hippocampal pyramidal neurons and have
found that, unlike APs at the soma, dendritic APs fail to activate
large-conductance Ca2+-activated
K+ current. This lack of
IC activation in the distal dendrites was demonstrated by the failure of both Ca2+ channel
blockade and IC blockers to affect AP
repolarization in the distal dendrites at concentrations that
completely blocked IC at the soma.
Repetitive firing of APs likewise failed to activate dendritic
IC. Investigation of AP repolarization in
the proximal dendrites showed that IC
activation by single APs progressively diminished within the proximal
dendrites and disappeared at a distance of 100-150 µm from the soma.
Thus, the activation of IC by action
potentials appears to be nonuniform within the CA1 pyramidal neuron,
diminishing with distance in the apical dendrites. Because this current
is responsible in part for the rapid repolarization of the somatic AP
and the fast AHP that follows the AP, its lack of activation in
the distal dendrites results in dendritic action potentials that
repolarize significantly more slowly than somatic APs and show no fast AHP.
Because IC activation is both voltage- and
Ca2+-dependent, the progressive loss of
IC activation with distance in the
dendrites could have several explanations: decreasing AP amplitude,
diminished Ca2+ influx triggered by back-propagating
APs, or a lack of IC itself in the
dendrites. Dendritic AP amplitude decrements with distance from the
soma and could affect IC activation both
by decreased membrane depolarization and by decreased
Ca2+ influx through intrinsic
Ca2+ conductances driven by the depolarization. This
is unlikely to explain the results for two reasons. First,
IC activation began to decline in the
proximal dendrites where AP amplitude was equal to that of the soma
(~100 mV); for example, at 70 µm from the soma, AP amplitude is
still ~100 mV, but IC activation had
declined to approximately one-half the somatic value. Second,
Ca2+-imaging experiments have shown that increases
in [Ca2+]i induced by back-propagating
APs are actually larger in the proximal dendrites than in the soma
(reaching a peak at ~100 µm from the soma) and thus would have been
expected to cause maximal activation of IC
(Jaffe et al., 1992 ; Callaway and Ross, 1995 ).
It is possible that IC activation depends
on Ca2+ influx through a specific
Ca2+ channel subtype that is nonuniformly
distributed throughout the pyramidal neuron. Marrion and Tavalin (1998)
have reported that BK channels in excised membrane patches from
hippocampal pyramidal neuron somata are selectively activated by N-type
Ca2+ channels and not by L- or P/Q-type channels.
N-type channels have been found in significant density at the soma but
occur at a much lower density in CA1 pyramidal neuron dendrites (Magee and Johnston, 1995a ); thus, it is possible that insufficient
Ca2+ influx is mediated by these channels to
activate dendritic IC. This assumes that
BK channels in the dendrites have the same predilection for
Ca2+ influx through N-type Ca2+
channels as do somatic channels and cannot be activated by
Ca2+ influx through other channel subtypes.
An additional possible explanation for the lack of activation of
dendritic IC depends on the distribution
of the underlying conductance itself. The most straightforward
hypothesis is that BK channels are primarily confined to the soma or to
the soma and proximal dendrites. This would be in agreement with the
findings of Knaus et al. (1996) who described the distribution of
slo (the BK channel gene) mRNA and protein in the
hippocampus as confined primarily to the pyramidal cell layer and to
mossy and perforant path fibers. Furthermore, slo has been
found to undergo alternative splicing to yield numerous isoforms with
wide variation in their Ca2+ sensitivity
(Tseng-Crank et al., 1994 ), so dendritic BK channels might exist as
isoforms that are markedly less sensitive to Ca2+
than is their somatic counterpart and thus are not activated by
dendritic APs.
Other than the present study, there are little previous data that
describe the activation of IC in
dendrites. One study using blind intradendritic recordings of presumed
pyramidal dendrites found that AP repolarization was sensitive to
prolonged application of Co2+ in some recordings,
although it was not reported at what dendritic distance this
observation occurred (Andreasen and Lambert, 1995 ). Sah and Bekkers
(1996) examined decay time constants of IPSCs to infer that slow AHP
currents mediated by SK channels were distributed on the proximal
dendrites, but this study did not investigate the currents underlying
the fast AHP. Previous cell-attached recordings in CA1 pyramidal neuron
dendrites have noted the infrequent appearance of BK-like channel
openings, usually under circumstances of poor cell health (D. Hoffman,
personal communication). This last finding would support the
presence of BK channels in dendrites, although at an unknown density
and of unknown biophysical properties.
The lack of dendritic IC activation has a
significant effect on the shape of the back-propagating dendritic
action potential, causing it to repolarize more slowly. This change in
AP shape likely affects dendritic integrative properties. For example, slower dendritic AP repolarization will cause greater inactivation of
both dendritic Na+ and A-type K+
currents, which may limit the ability of the dendrites to follow fast
repetitive firing at the soma. Broad dendritic APs will also have an
increased unblocking effect on the voltage-dependent conductance of
NMDA receptors, which can lead to increased Ca2+
influx during paired back-propagating APs and synaptic stimuli (Magee
and Johnston, 1997 ; Koester and Sakmann, 1998 ; Schiller et al., 1998 ).
Furthermore, the lack of IC may explain in
part the lowered dendritic threshold for Ca2+
spiking, because these regenerative responses are mediated by high-threshold Ca2+ channels that are usually
activated on the repolarizing phase of preceding dendritic
Na+ APs (Andreasen and Lambert, 1995 ; Magee and
Johnston, 1995b ). Conversely, the localization of BK channels
predominantly to the soma and axon terminals, as shown by anatomic data
(Knaus et al., 1996 ), suggests that IC is
most important for regulating the shape of orthodromically propagating
action potentials, especially at the axon terminal, where AP width can
have significant effects on neurotransmitter release.
Although the relative lack of IC
activation significantly affects dendritic AP shape, it is clearly not
the only factor. Dendritic AP back-propagation is also affected by the
progressive increase in A-current with dendritic distance, which
decreases AP amplitude and raises the threshold for dendritic AP
initiation (Hoffman et al., 1997 ). Under conditions of
IC blockade or both
IC and A-current blockade (Hoffman et al.,
1997 ), dendritic APs still repolarize significantly more slowly in the
dendrites than in the soma. This would suggest a relative lack of some
other conductance, most likely a rapidly activating delayed rectifier;
one possibility would be K+ channels containing the
subunit encoded by Kv2.1, which have been found to be a significant
component of the delayed-rectifier K+ current in
hippocampal neurons and appear to be confined to the soma and proximal
dendrites (Murakoshi and Trimmer, 1999 ). This possibility, along with
the present finding of a relative lack of dendritic
IC activation, joins accumulating evidence
that voltage-gated ion channels are distributed nonuniformly within the
hippocampal pyramidal neuron and that this regional nonuniformity
shapes the signal-processing capabilities of the neuron.
 |
FOOTNOTES |
Received March 4, 1999; revised April 8, 1999; accepted April 12, 1999.
This work was supported by the National Institute of Neurological
Disorders and Stroke (NINDS) Grant NS01981 to N.P.P., a grant from the
Epilepsy Foundation of America to N.P.P., the National Institute of
Mental Health Grant MH48432 to D.J., NINDS Grant NS37444 to D.J., and
grants from the Human Frontiers Science Project and the Hankamer
Foundation to D.J.
Correspondence should be addressed to Dr. Daniel Johnston, Division of
Neuroscience S-603, Baylor College of Medicine, Houston, TX 77030.
 |
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