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J Neurophysiol (April 1, 2003). 10.1152/jn.00709.2002
Submitted on Submitted 20 August 2002; accepted in final form 30 November 2002
1Department of Bioengineering, University of Toledo, Toledo, Ohio 43606-3390; and 2Department of Otolaryngology/Head and Neck Surgery, University of North Carolina, Chapel Hill, North Carolina 27599-7070
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ABSTRACT |
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Molitor, Scott C. and Paul B. Manis. Dendritic Ca2+ Transients Evoked by Action Potentials in Rat Dorsal Cochlear Nucleus Pyramidal and Cartwheel Neurons. J. Neurophysiol. 89: 2225-2237, 2003. Simultaneous fluorescence imaging and electrophysiologic recordings were used to investigate the Ca2+ influx initiated by action potentials (APs) into dorsal cochlear nucleus (DCN) pyramidal cell (PC) and cartwheel cell (CWC) dendrites. Local application of Cd2+ blocked Ca2+ transients in PC and CWC dendrites, demonstrating that the Ca2+ influx was initiated by dendritic Ca2+ channels. In PCs, TTX eliminated the dendritic Ca2+ transients when APs were completely blocked. However, the Ca2+ influx could be partially recovered during an incomplete block of APs or when a large depolarization was substituted for the blocked APs. In CWCs, dendritic Ca2+ transients evoked by individual APs, or simple spikes, were blocked by TTX and could be recovered during an incomplete block of APs or by a large depolarization. In contrast, dendritic Ca2+ transients evoked by complex spikes, a burst of APs superimposed on a slow depolarization, were not blocked by TTX, despite eliminating the APs superimposed on the slow depolarization. These results suggest two different mechanisms for the retrograde activation of dendritic Ca2+ channels: the first requires fast Na+ channel-mediated APs or a large somatic depolarization, whereas the second is independent of Na+ channel activation, requiring only the slow depolarization underlying complex spikes.
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INTRODUCTION |
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The classical view of
synaptic integration is that action potentials (APs) are generated by
the soma and axon in response to the passive summation of synaptic
inputs within the dendritic arbor (Coombs et al. 1957
;
Fatt 1957
). However, intradendritic recordings from
mammalian neurons showed that dendrites are not necessarily passive
structures (Llinás and Sugimori 1980
; Wong et al. 1979
). Although it was originally postulated that
dendritic voltage-gated conductances are only involved in the
anterograde propagation of synaptic responses toward the soma
(Llinás and Nicholson 1971
), somatic and axonal
APs can propagate retrogradely and evoke active dendritic responses.
The imaging of ion-sensitive fluorescence indicators has shown that APs
evoke a Ca2+ influx through dendritic
Ca2+ channels in cortical (Markram et al.
1995
; Schiller et al. 1995
) and hippocampal
(Jaffe et al. 1992
; Spruston et al. 1995
)
pyramidal neurons, in thalamocortical relay neurons (Zhou et al.
1997
), in olfactory bulb mitral cells (Charpak et al.
2001
; Margrie et al. 2001
), and in spinal
motoneurons (Larkum et al. 1996
).
Dendritic Ca2+ channels may play an important
role in the integration of synaptic inputs. Because of the importance
of Ca2+ as a second messenger (Tsien and
Tsien 1990
) and because of its limited mobility in cytoplasm
(Albritton et al. 1992
), dendritic Ca2+ channels may also provide an important
source of Ca2+ at or near synapses. This
dendritic Ca2+ influx may produce changes in
synaptic efficacy when the retrograde propagation of somatic APs into
the dendrites is paired with afferent inputs (Bell et al.
1997
; Linden 1999
; Magee and Johnston
1997
; Markram et al. 1997
). In addition, the
activation of dendritic Ca2+ channels by
propagating APs can alter the electrophysiologic response properties of
neurons. Ca2+ channel-mediated burst discharges
in hippocampal CA1 and CA3 pyramidal neurons can be induced under
conditions that block dendritic voltage-gated K+
channels (Golding et al. 1999
; Magee and Carruth
1999
), and simultaneous back-propagating APs and dendritic
depolarization can also evoke complex spike discharges in neocortical
pyramidal neurons (Schwindt and Crill 1999
;
Williams and Stuart 1999
).
Dendritic Ca2+ channels may contribute to
information processing in at least two neuronal populations within the
dorsal cochlear nuclei (DCN). Pyramidal cells (PCs, also known as
fusiform cells) receive excitatory afferent input from two spatially
and functionally segregated sources. The basal dendrites receive
excitatory input from auditory nerve fibers (ANFs) ascending from the
cochlea (Hirsch and Oertel 1988b
; Kane
1974
; Manis and Brownell 1983
; Ryugo and May 1993
), whereas the apical dendrites receive excitation from parallel fibers (PFs) originating from granule cells scattered throughout the cochlear nucleus (Manis 1989
; Osen
and Mugnaini 1981
). The activation of dendritic
Ca2+ channels by somatic APs could serve to
modulate synaptic efficacy in response to synchronously active ANF and
PF inputs. Cartwheel cells (CWCs) can be identified by their
characteristic burst discharges or complex spikes (Manis et al.
1994
; Zhang and Oertel 1993
) that consist of
fast Na+ channel-mediated APs superimposed on a
slow Ca2+ channel-mediated depolarization
(Agar et al. 1996
; Golding and Oertel
1997
). However, complex spiking units also respond with simple
spikes or a combination of complex and simple spikes in a variety of
preparations (Davis and Young 1997
; Ding et al.
1999
; Golding and Oertel 1996
; Manis et
al. 1994
; Parham and Kim 1995
; Waller and
Godfrey 1994
; Zhang and Oertel 1993
). These
distinct electrophysiologic responses could result from differences in the pattern of dendritic Ca2+ channel activation
initiated by Na+-channel mediated APs.
The experiments in the present study combine whole cell recordings with
the imaging of the fluorescent Ca2+ indicator
fluo-3 to investigate whether APs evoked by somatic current injection
evoke a Ca2+ influx into the dendrites of PCs and
CWCs. The properties of Ca2+ channels have been
investigated in acutely dissociated DCN neurons (Harasztosi et
al. 1999
; Molitor and Manis 1999
); however, no information about dendritic Ca2+ channels could
be obtained from this preparation. In the present study, recordings
from a brain stem slice preparation show that APs evoke a
Ca2+ influx into the apical and basal dendrites
of PCs and into the dendrites of CWCs. Na+
channel-mediated APs are required to evoke a Ca2+
influx into the dendrites of PCs and simple spiking CWCs, whereas the
activation of Na+ channels is not required to
evoke a Ca2+ influx into the dendrites of complex
spiking CWCs. The activation of dendritic Ca2+
channels by APs may play a significant role in shaping the output of
the DCN, both by contributing to the integration of spatially and
functionally segregated afferent inputs in PCs and by shaping the
electrophysiologic responses of CWCs.
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METHODS |
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Preparation of slices
Rat pups (age P10-P18) were anesthetized with ketamine (44 mg/kg) and decapitated, and the brain stem was quickly removed and
placed into an oxygenated HEPES-buffered dissection solution at 30°C
containing (in mM) 138 NaCl, 5 KCl, 1.25 KH2PO4, 10 glucose, 0.2 CaCl2, 4 MgSO4, and 10 HEPES, pH 7.35 with 5 M NaOH. Using an oscillating tissue slicer, the
cochlear nuclei were cut into 250-µm-thick slices in the transtrial
plane, perpendicular to the parallel fibers, and were placed into an
incubation chamber containing an artificial cerebrospinal fluid (ACSF;
see composition in the following text) maintained at 34°C. Slices
remained in incubation for
1 h before being transferred to the
recording chamber. In the recording chamber, slices were superfused
with the ACSF (2-4 ml/min) and were maintained at 33°C throughout
all recordings. The ACSF solution contained (in mM) 130 NaCl, 3 KCl, 1.25 KH2PO4, 20 NaHCO3, 10 glucose, 2.5 CaCl2, and 1.3 MgSO4 and was continuously perfused with 95% O2-5%
CO2 to maintain a pH near 7.4. During some
experiments, the voltage-gated Na+ channel
antagonist TTX was diluted from a concentrated stock solution and added
to the ACSF. TTX was purchased from Molecular Probes (Eugene, OR);
remaining chemicals were purchased from Sigma-Aldrich (St. Louis, MO).
Electrophysiologic recordings
Whole cell recording techniques (Edwards et al.
1989
; Hamill et al. 1981
) were used to provide
depolarizing stimuli, to record electrophysiologic responses, and to
provide a rapid means of loading individual cells with a fluorescent
indicator while minimizing background fluorescence. Individual cells
near the slice surface were visualized with infrared video microscopy
(MacVicar 1984
) on a fixed-stage upright microscope
(Axioskop FS, Carl Zeiss) with a 40×, 0.75 NA water-immersion
objective. Whole cell recordings were obtained using either a List
EPC-7 amplifier in current-clamp mode or an Axoprobe 1A current-clamp
amplifier, filtered at 3 kHz and digitized at 10 kHz with a 12-bit A/D
converter (Digidata 1200, Axon Instruments). Although it is known that
voltage-clamp amplifiers such as the List EPC-7 can distort the
measured AP waveform in current-clamp mode (Magistretti et al.
1998
), no significant differences were observed between the
AP-evoked Ca2+ influx in recordings obtained with
either amplifier. Recording pipettes were pulled with a horizontal
puller (BB-CH-PC, Mecanex) from borosilicate glass capillaries (KG-33
glass, Garner Glass), fire-polished, and coated with silicone elastomer
(Sylgard; Dow Corning). Pipette resistances ranged from 3 to 8 M
with a pipette solution containing (in mM) 110 K gluconate, 20 KCl, 4 NaCl, 4 MgATP, 10 HEPES, 10 phosphocreatine, 0.3 GTP, 0.2 EGTA, and 0.2 fluo-3 (pentapotassium salt, Molecular Probes), pH 7.20 with 5 M KOH.
Although EGTA could reduce fluorescence signals by reducing the
available free Ca2+ for binding to fluo-3, we
found that the addition of a low concentration of EGTA to the pipette
solution improved the detection of fluorescence signals by reducing
background and resting fluorescence levels and improved the long-term
stability of electrophysiologic recordings. Small amounts of
hyperpolarizing holding current (typically <300 pA for pyramidal cells
and <200 pA for cartwheel cells) were sometimes applied to prevent
spontaneous APs. Bridge balance errors were corrected on-line for
recordings made with the Axoprobe 1A and off-line for recordings made
with the List EPC-7. Capacitive transients were blanked and a measured
junction potential of 12 mV between the pipette solution and the ACSF
was subtracted from the voltage traces.
In some experiments, local application of TTX and
CdCl2 via pressure pipette was employed to
ascertain the conductance types contributing to the dendritic
Ca2+ influx. TTX and CdCl2
were diluted from concentrated stock solutions into a HEPES-buffered
solution containing (in mM) 138 NaCl, 5 KCl, 10 glucose, 2.5 CaCl2, 1.3 MgCl2, and 10 HEPES, pH 7.35 with 5 M NaOH. The concentration of TTX (10 µM) and
CdCl2 (1 mM) in the pressure pipette was 10-fold
the desired final concentration at the site of application. Pressure
pipette solutions were 0.2 µm filtered and centrifuged at 12,000 rpm
for 5 min to prevent clogging of tips with any insoluble material that
may be present. Pressure pipettes were similar to the recording
pipettes, although the pressure pipettes generally had smaller tips
(resistances 5-10 M
) than the recording pipettes to limit the
mixing of the ACSF with the pipette contents and to limit the spread of
the ejected bolus. Under visual control, pressure pipettes were
typically placed within 10 µm of the target dendritic process. For
each stimulus trial during which a pressure application was given, two
or three 10-ms pulses of 3-5 PSI were delivered at 50 Hz by opening a solenoid valve driven by a TTL circuit. Pressure pulses were
timed so that the first pulse was delivered prior to the onset of the
electrophysiologic stimulus, and the remaining pulses were delivered
during the stimulus train. No discernible effects were observed on
electrophysiologic or fluorescence recordings from three cells during
pressure application of the HEPES-buffered pressure pipette solution
without TTX or CdCl2 (not shown).
Image acquisition
A shuttered mercury arc lamp (HBO 100 W, Carl Zeiss) was used with a 450- to 490-nm band-pass excitation filter to excite dye fluorescence; emissions were filtered with a 520-nm long-pass filter. The resulting images were collected with an integrating CCD camera (model 4982, Cohu). Individual video frames were acquired every 33 ms and were digitized with a 10-bit frame grabber (Image Lightning 2000, Axon Instruments) controlled by Axon Imaging Workbench (version 2.0-2.1) in the nonratiometric imaging mode. Digitized images are 640 × 480 pixels, which corresponds to an imaged area of 150 × 115 µm. Both PCs and CWCs possess extensive dendritic arbors; however, the use of a fixed-stage microscope prevented the movement of the objective relative to a cell once recordings began, so the results are limited to the most proximal processes of these neurons. Electrophysiologic stimuli were generated and recordings were obtained by a separate computer that was synchronized to the imaging computer by a common trigger signal. The onset of any electrophysiologic stimuli was delayed by 100 ms relative to the onset of image acquisition to allow for the acquisition of three resting fluorescence images for direct comparison with fluorescence levels during presentation of electrophysiologic stimuli. Repetitive stimuli were presented 10 s apart to allow for a complete return of intracellular Ca2+ to resting levels.
After the termination of electrophysiologic recordings, the recording
pipette was withdrawn and a series of integrated (2-8 video frames)
fluorescence images were obtained from different regions, and focal
depths to reconstruct the morphology of the neuron from which
recordings had been obtained. Montages of these fluorescence images
were assembled to simultaneously display all visible anatomic features.
PCs were identified as large (long axis of the soma >25 µm) bipolar
neurons with extensively branched apical dendrites extending into the
superficial DCN and less-extensively branched basal dendrites extending
into deeper layers (Blackstad et al. 1984
). CWCs were
identified as medium-sized (long axis of soma 15-20 µm) multipolar
neurons with ovoid cell bodies and spiny dendrites typically limited to
the superficial DCN (Wouterlood and Mugnaini 1984
). The
spines characteristic of CWC (and to a lesser extent, PC) dendrites
were not always visible due to light scatter through the 250-µm-thick
tissue sections. Therefore dendritic branching patterns were examined
to further distinguish CWCs from other DCN neurons. CWC dendrites
typically branch at wider angles, resulting in distal processes that
sometimes curve around or toward the soma (Wouterlood and
Mugnaini 1984
), whereas the dendrites of other neurons in the
superficial DCN, such as stellate cells, branch at smaller angles,
resulting in dendritic processes that radiate outward from the soma.
Image analysis
Fluorescence images are shown as
F/F,
which is the fractional change in fluorescence elicited by a stimulus
relative to the resting fluorescence. Estimates of the calcium
concentration can be computed from
F/F if
accurate measurements of the dye Kd
and the resting calcium levels are known (Lev-Ram et al.
1992
). Because these parameters have not been measured in our
preparation, values are only reported as fractional changes in
fluorescence. Given the properties of the fluorescence indicator being
used in these experiments, positive
F/F values
indicate an increase in free Ca2+ concentration.
Raw fluorescence images were background subtracted and filtered prior
to constructing
F/F images. Typically, the majority of pixels in a given image measured only background
fluorescence, so background subtraction was performed by subtracting
the median of a pixel intensity histogram for each image. After
background subtraction, a 3 × 3 filter was used to smooth pixel
intensities throughout each image (pixel weights were 4/9 in the
center, 1/9 on the sides, and 1/36 on the corners).
F/F images were then obtained by subtracting
the resting fluorescence image obtained immediately before the stimulus
presentation from a fluorescence image obtained at the end of the
stimulus presentation and normalizing this difference by the resting
fluorescence image.
One difficulty with the calculation of
F/F
images is the high level of background fluorescence in a slice
preparation (Sandler and Barbara 1999
). In these
experiments, many dendritic processes at rest were not visible above
background and only became visible after a fluorescence increase
resulting from a Ca2+ influx. Normalizing
fluorescence changes by resting fluorescence values that are not
significantly above background levels produces erroneously large
F/F values. To prevent these errors, the value of the background fluorescence was added back to the resting
fluorescence image prior to normalizing:
F/F = (Fstim - Frest)/(Frest + Fbackground). Although this results
in an underestimation of the true
F/F value, it does not alter our interpretation of these data, since the focus of
this study was to compare relative changes in
Ca2+ levels rather than absolute measures of
Ca2+ concentration.
Quantitative comparisons of fluorescence changes were obtained using
fluorescence profiles. Profiles are curves that follow a visible
dendrite along its length; the
F/F value for
each pixel that falls along the curve is plotted as a function of path
distance from the curve origin, which is typically located where the
dendrite originates from the soma. Despite filtering, there was
significant variation between neighboring pixels, which produced noisy
fluorescence profiles. To reduce this noise, profile data were smoothed
by averaging
F/F values from small regions
(~1 µm2) centered on each pixel along the
profile rather than using
F/F values from
individual pixels. Profile data were subsequently averaged across
stimulus repetitions; gray shaded regions are used to represent the
mean ± SE on graphs presenting profile averages. In some
instances (Figs. 3 and 4), fluorescence profiles were normalized to
compare the spatial distribution of Ca2+
transients evoked under different conditions. Rather than normalizing amplitudes at a fixed point along the profile, scaling factors were
calculated to minimize the mean square distance between profiles.
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RESULTS |
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Ca2+ transients in pyramidal cell dendrites
The ability of subthreshold and suprathreshold stimuli to evoke a Ca2+ influx into the soma and proximal dendrites of PCs was initially examined. PCs were presented with a 100-Hz train of 4-ms current pulses; the magnitude of these pulses was adjusted to produce subthreshold (Fig. 1A, left) and suprathreshold (Fig. 1A, middle and right) responses. A subthreshold depolarization alone is not sufficient to elicit a widespread Ca2+ influx; little or no fluorescence increase was evoked in the absence of APs (Fig. 1, B, left, and C, blue lines). Somatic APs produced fluorescence increases throughout the soma and proximal dendrites of PCs, indicating increased somatic and dendritic Ca2+ levels. A single AP can elicit a widespread dendritic Ca2+ influx; detectable fluorescence increases evoked by an individual AP were observed throughout most visible regions (Fig. 1, B, middle, and C, green lines). A substantial fluorescence increase in the soma and all visible dendrites was evoked by multiple APs in rapid succession (Fig. 1, B, right, and C, red lines).
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These results demonstrate that the fluorescence increase occurs in both
the proximal apical (Fig. 1, B, upper processes, and C, right) and basal (Fig. 1, B, lower
right process, C, left) dendrites of this PC.
Although the magnitude of fluorescence changes is greater in the apical
dendrite relative to the basal dendrite (Fig. 1C), this does
not necessarily indicate a larger Ca2+ influx
into the apical dendrite. Regions where the largest fluorescence changes were observed are usually the same areas where the resting fluorescence was higher compared with neighboring regions. This asymmetric distribution of resting dye fluorescence represents areas of
dye accumulation, compartments with decreased surface to volume ratios,
or processes closer to the slice surface, which reduces the amount of
overlying tissue that can scatter the emitted fluorescence. Normalizing
fluorescence changes by the resting fluorescence should account for a
nonuniform resting fluorescence, but our calculations of
F/F include the background fluorescence (see
METHODS), which reduces the relative magnitudes of spatial differences in the resting fluorescence values. While we can conclude that APs evoke a Ca2+ influx into the apical and
basal dendrites of PCs, we cannot make any conclusions about the
relative magnitudes of the Ca2+ changes across
different regions of an individual cell.
The involvement of dendritic Ca2+ channels in
producing the dendritic Ca2+ influx was
investigated with the Ca2+ channel antagonist
Cd2+. The fluorescence increase in an apical PC
dendrite elicited by a train of APs was reduced locally by the first of
two consecutive applications of 1 mM CdCl2 via a
pressure pipette (Fig. 2B). No reduction in the AP-evoked fluorescence increase was observed in a
basal dendrite farthest from the location of the pressure pipette (Fig.
2E). Cd2+ also reduced the
fluorescence of a background region near the pressure pipette in both
trials (Fig. 2C), which presumably results from the binding
of Cd2+ to residual dye in the extracellular
space that accumulated when the pipette approached the cell with
positive pressure prior to seal formation. Similar to
fluo-3/Mn2+ and fluo-3/Zn2+
complexes (Kao et al. 1989
), the fluorescence of a
fluo-3/Cd2+ complex may be substantially less
than that of a fluo-3/Ca2+ complex, resulting in
an apparent fluorescence reduction when Cd2+ is
added to the extracellular environment. Due to light scattering within
the tissue section, the background and dendritic fluorescence cannot be
independently measured, so that a reduction in background fluorescence
could contribute to an apparent reduction in dendritic fluorescence and
vice versa. However, the reduction of fluorescence along the apical
dendritic process is more extensive during the first
Cd2+ application (Fig. 2D, blue line
and arrows) when compared with the corresponding reduction in
background fluorescence (Fig. 2C, blue line and arrows). In
addition, a second Cd2+ application 10 s
after the first produced a widespread depression in fluorescence levels
along the entire apical dendrite (Fig. 2D, red line) that
was not observed in the corresponding background fluorescence profile
(Fig. 2C, red line). Across seven PCs, the dendritic
fluorescence reduction around the pressure pipette extended 28.2 ± 3.7 µm during the first and 42.6 ± 6.5 µm during the
second of two consecutive Cd2+ applications as
measured by the extent of a fluorescence reduction >3 SE from the
control fluorescence profile around the pressure pipette. In contrast,
the background fluorescence reduction only extended 14.7 ± 2.0 and 18.9 ± 2.9 µm during the same sequence of local
Cd2+ application. Thus a reduction of
extracellular dye fluorescence by Cd2+ cannot
account fully for the overall fluorescence decrease, indicating that a
reduction of Ca2+ influx through dendritic
Ca2+ channels blocked by
Cd2+ also contributes to the fluorescence
decrease.
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A reduction of the AP-mediated Ca2+ influx by
Cd2+ suggests that APs initiate a
Ca2+ influx through dendritic voltage-gated
Ca2+ channels. The results of Fig. 2 and similar
results from six other PCs do not imply that a
Ca2+ influx through Ca2+
channels is solely responsible for the increase in intracellular Ca2+ levels. It is possible that other sources
contribute to the rise in intracellular Ca2+
levels, such as Ca2+-induced
Ca2+ release (Llano et al. 1994
;
Sandler and Barbara 1999
). It has been shown that the
majority of the Ca2+ influx into acutely isolated
PC cell bodies can be attributed to Ca2+ channels
(Rusznak et al. 2000
), although we did not attempt to resolve the relative contributions of separate sources of the dendritic
Ca2+ influx in the present study. However, it is
clear that dendritic Ca2+ channels initiate the
Ca2+ influx; additional sources may contribute to
the overall Ca2+ influx once the initial influx
through Ca2+ channels occurs.
It is possible that APs trigger a large somatic
Ca2+ increase that diffuses into dendritic
processes, accounting for the majority of the observed fluorescence
increases. This is not likely due to the limited diffusion of cytosolic
Ca2+ within neurons (Albritton et al.
1992
). In addition, a localized reduction of
Ca2+ influx due to the application of
Cd2+ via a pressure pipette also suggests that
the diffusion of somatic Ca2+ is not responsible
for the observed dendritic Ca2+ influx. However,
if the diffusion of a somatic Ca2+ influx was
responsible for the dendritic extent of the fluorescence increase, a
larger somatic Ca2+ influx should produce an
increased spread of fluorescence, as opposed to a spatially uniform
increase with little or no spatial spread. Increasing the number of APs
does not produce a more distal spread of fluorescence; instead, larger
fluorescence increases were seen in regions that had detectable
F/F values elicited by a single AP (Fig.
3B - D,
). This uniform
increase can be also be observed by directly comparing the fluorescence
profiles elicited by one to four APs normalized to the magnitude of the fluorescence profile elicited by eight APs (Fig. 3, B-D,
- - - and
). In this cell and in nine other PCs, the normalized
fluorescence magnitudes share a similar profile regardless of the
number of APs, suggesting that the dendritic Ca2+
increase results from a Ca2+ influx that is local
to the region of the observed fluorescence increase rather than a
diffusion of a somatic Ca2+ influx.
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Although the increase in fluorescence changes resulting from additional
APs is spatially uniform, the distribution of an AP-mediated Ca2+ influx along a dendritic process may not be
spatially homogeneous. Peaks in the fluorescence profiles were observed
(Fig. 3, B-D), which may indicate localized regions of high
Ca2+ influx, or "hot spots." Despite examples
to the contrary, a correlation between fluorescence peaks and dendritic
branch points appeared to be the case in many PC dendrites, similar to
what had been proposed to occur in the dendrites of cerebellar Purkinje
neurons (Llinás and Nicholson 1971
). However, most
hot spots observed here also correspond to regions where the resting
fluorescence was higher than in neighboring regions, potentially
representing areas of dye accumulation or compartments with lower
surface-to-volume ratios. In addition, continuous dendritic segments
sometimes did not reside within a single focal plane, contributing to
the appearance of nonuniform fluorescence changes. Therefore we cannot
necessarily conclude that nonuniform fluorescence changes correspond to
a nonuniform Ca2+ influx along the length of a
dendritic process.
The time course of fluorescence changes also supports the idea that the
increase in dendritic Ca2+ is due to local
Ca2+ sources rather than the diffusion of
Ca2+ from the soma or other cellular compartment.
If the diffusion of somatic Ca2+ was the source
of dendritic Ca2+ influx, the time course of
distal fluorescence transients would be delayed and or prolonged
relative to the time course of proximal fluorescence transients.
However, the decay of distal fluorescence transients (Fig. 3,
E-H,
) appears to occur at the same rate or faster than
the decay of proximal fluorescence transients (Fig. 3, E-H,
). The larger fluorescence magnitudes observed when more APs were
elicited (Fig. 3, B-D) reflects an accumulation of
Ca2+ bound to the fluorophore rather than an
increase in Ca2+ diffusion. The image acquisition
rate (30 Hz) is too slow to resolve the fluorescence increases that
occur with each individual AP. However, the high
Ca2+ binding affinity of the dye
(Kd = 400 nM) (Minta et al.
1989
) and the dye concentration used in these experiments (200 µM) should result in a slow off-rate of Ca2+
bound to the dye (Helmchen et al. 1996
) as observed by
the slow fluorescence decay following a train of APs (Fig. 3,
E-H). This slow off-rate produces an accumulation of
dye-bound Ca2+ when APs are elicited in rapid
succession, effectively integrating the Ca2+
influx across all APs within the train. This integration of
Ca2+ influx can be observed in the rising phase
of the fluorescence transients, which continue to increase until the
train of APs that initiate the influx has been terminated (Fig. 3,
E-H). Although it cannot be determined how the magnitude of
the Ca2+ influx varies among individual APs, it
does appear that each additional AP elicits additional
Ca2+ influx when presented in rapid succession.
Contribution of Na+ channels to dendritic Ca2+ transients
The Ca2+ channels that initiate the dendritic Ca2+ influx can also actively propagate a somatic depolarization throughout the dendritic arbor. Other voltage-gated conductances, such as Na+ channels, may also be present in the dendrites and contribute to the spread of a dendritic depolarization. One possibility is that dendritic Na+ channels are responsible for conducting the propagating depolarization into the dendrites, whereas Ca2+ channels respond to this depolarization with a Ca2+ influx but contribute little to the active propagation of APs into the dendritic arbor. To investigate this possibility, the effects of blocking Na+ channels on the dendritic Ca2+ influx were subsequently investigated.
If dendritic Na+ channels contribute to the
spread of a somatic depolarization into the dendritic arbor, a local
block of Na+ channels could prevent the
depolarization from propagating past the site of
Na+ channel block, thereby reducing the
Ca2+ influx at and distal to that region. Local
application of 10 µM TTX slightly reduced the dendritic
Ca2+ influx elicited by a train of somatic APs at
but not distal to the site of TTX application in an apical PC dendrite
(Fig. 4C). One interpretation
of this result is that the TTX applied via pressure pipette did not
reach its target; however, three lines of evidence refute this
interpretation. First, application of Cd2+ via
pressure pipette using similar positioning and pressure pulses resulted
in a localized reduction in the Ca2+ influx (Fig.
2). Second, the raw fluorescence images show that the apical dendrite
moved slightly in response to the bolus ejected from the pressure
pipette (not shown); these raw fluorescence images were reconstructed
to align the apical dendrite to its original location prior to the
calculation of the
F/F images. Third, a
subsequent application of TTX 10 s later blocked all but one AP
(Fig. 4B, bottom), reducing the
Ca2+ influx into the apical dendrite (Fig.
4D,
). A comparison of the fluorescence profile evoked
during the second TTX application normalized to the fluorescence
profile evoked under control conditions (Fig. 4D, - - -
and
) shows that Ca2+ transients were still
observed throughout the visible apical dendrite despite a block of
Na+ channels whose spatial extent was large
enough to affect AP initiation. Similar results were obtained from six
other PCs in which the first TTX application did not eliminate APs and
in which the pressure pipette was confirmed to be unclogged after
recordings had been terminated. Therefore blocking dendritic
Na+ channels does not attenuate the dendritic
Ca2+ influx if the extent of the
Na+ channel block does not alter the generation
of APs evoked by somatic depolarization.
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A dendritic Ca2+ influx can still be observed
when APs are blocked during a block of Na+
channels throughout the entire cell. The Ca2+
influx elicited by a train of somatic APs (Fig.
5C,
) was reduced by the
addition of 1 µM TTX to the bathing medium (Fig. 5C,
), which prevented the cell from spiking in response to depolarizing current injection (Fig. 5B, bottom). Unlike
subthreshold responses (Fig. 1), a measurable fluorescence increase
remains in the presence of TTX. This presumably is due to the larger
depolarizing stimulus used to evoke APs under control conditions
compared with the smaller depolarizing stimulus needed to maintain the
cell at subthreshold levels. However, these results did vary, and other
PCs showed a more complete block of the original
Ca2+ influx by TTX (e.g., Figs. 6 and 7). The
variable amount of Ca2+ influx blocked by TTX
likely reflects differences in the stimulus levels used to evoke APs
across the different cells. In nine PCs, TTX blocked 76.8-96.9% of
the AP-evoked fluorescence increase; in seven of these cells, reduced
or attenuated APs were observed as TTX washed into the superfusate
(Fig. 5B, middle), and these attenuated APs were
sufficient to evoke widespread Ca2+ influx (Fig.
5C, - - -). The profiles of fluorescence changes evoked by
reduced numbers of APs in the presence of TTX closely approximated
profiles evoked by similar numbers of APs under control conditions (not
shown), suggesting that a dendritic Ca2+ influx
can be evoked independent of Na+ channel
activation.
|
If a block of Na+ channels does not eliminate the
dendritic Ca2+ influx, then it may also be
possible to fully recover the dendritic Ca2+
influx in the absence of any Na+ channel
activation. The Ca2+ influx elicited by a train
of somatic APs (Fig. 6C,
shaded area) was eliminated by the addition of 1 µM TTX to the
bathing medium (Fig. 6C,
), which prevented to cell from
spiking in response to depolarizing current injection (Fig.
6B, bottom left). Somatic current pulses of large
amplitude and duration elicited an AP that was smaller and broader
(Fig. 6B, bottom right) than the original APs
evoked prior to the exposure to TTX (Fig. 6B, top left). These broad APs were likely to be
Ca2+ channel-mediated events that can be evoked
in PCs during Na+ channel blockade (Hirsch
and Oertel 1988a
). When these Ca2+
channel-mediated APs were evoked, a substantial
Ca2+ influx was observed (Fig. 6C, top
dashed line) that was similar to the magnitude of the
Ca2+ influx evoked by Na+
channel-mediated APs. In seven PCs tested, 14.8-93.4% of the fluorescence increase blocked by TTX was recovered with increased somatic current injection. However, these fluorescence changes are
dependent on the magnitude of the somatic depolarization rather than
the number of Ca2+-mediated APs: a much smaller
fluorescence increase is observed (Fig. 6C, bottom dashed
line) when evoked by a smaller somatic depolarization that is still
sufficient to evoke a Ca2+-mediated AP. Therefore
a complete block of Na+ channels does not
preclude a dendritic Ca2+ influx, if a sufficient
somatic depolarization is provided in the absence of APs.
|
When Na+ channels are blocked, a local block of
Ca2+ channels by Cd2+
produces a region of membrane that is devoid of any depolarizing active
conductances, which could prevent the propagation of a Ca2+ spike distal to this region. To test this
hypothesis, the effects of applying Cd2+ via a
pressure pipette were examined while Na+ channels
were blocked by TTX. The Ca2+ influx elicited by
a train of APs (Fig. 7C,
)
was reduced (Fig. 7C,
) when the APs were blocked by the
addition of 1 µM TTX to the bathing medium (Fig. 7B,
middle). A partial recovery of the original fluorescence
increase was obtained (Fig. 7C, - - -) by increasing the
amplitude and duration of somatic current pulses that elicited small
Ca2+ spikes (Fig. 7B,
bottom). A local block of Ca2+
channels via a pressure application of Cd2+
produced a local reduction in the partially recovered fluorescence increase at but not distal to the region of Ca2+
channel block (Fig. 7D,
) without having any discernible
effects on the magnitude of the small Ca2+ spikes
(not shown). The results from this and a 2nd PC show that a local block
of dendritic Ca2+ channels in the absence of any
Na+ channel activation does not prevent the
propagation of Ca2+ channel-mediated APs,
suggesting that any attenuation occurring over a small region of
passive membrane is not sufficient to terminate the spread of a
dendritic depolarization.
|
Ca2+ transients in cartwheel cell dendrites
Unlike PCs, CWCs can respond to a suprathreshold stimulus with a
complex spike, a burst of fast APs superimposed on a slow depolarization (Manis et al. 1994
; Zhang and
Oertel 1993
) that is mediated by Ca2+
channels (Golding and Oertel 1997
). These different
electrophysiologic responses may reflect different patterns of
dendritic Ca2+ channel activation. Complex spikes
evoked by small somatic current pulses (Fig.
8B, top left)
elicited a large dendritic Ca2+ influx (Fig.
8C,
) in two visible dendrites of a CWC. Addition of 1 µM TTX to the bathing medium blocked the fast APs but did not block
the slow underlying depolarization (Fig. 8B, top
right) or the dendritic Ca2+ influx (Fig.
8C,
). In this CWC, blocking Na+
channels with TTX increased the duration of the slow depolarization (Fig. 8B, top right). It is not clear why this
occurred; one possibility is a reduction in the activation of
K+ channels that normally contribute to the
repolarization of fast Na+-mediated APs. A
prolonged slow depolarization could augment the dendritic
Ca2+ influx that would otherwise be reduced in
the absence of Na+ channel activation. Although
not conclusive, the time course of fluorescence changes suggests that
the prolonged slow depolarization extends the duration of the
fluorescence changes instead of increasing their amplitudes (Fig.
8B, bottom right). In addition, a dendritic Ca2+ influx was observed in other CWCs in which
TTX did not produce a similar increase in the duration of the slow
depolarization in other CWCs (Fig. 9).
Therefore a dendritic Ca2+ influx into CWC
dendrites evoked by a complex spike can occur in the absence of
Na+ channel activation.
|
|
Unlike PCs, little or no increase in the amplitude and duration of somatic current injection was required to elicit a Ca2+ influx into the dendrites of complex spiking CWCs in the presence of TTX. In five complex spiking CWCs tested, a dendritic Ca2+ influx could be elicited in the presence of TTX that was comparable in magnitude (110.0 ± 5.6%, range 95.0-121.5%) to the dendritic Ca2+ influx elicited under control conditions. In one of these cells, blocking Na+ channels with TTX produced a variable threshold for evoking the slow depolarization underlying the original complex spike (Fig. 9C), which allowed for a direct comparison of the Ca2+ influx evoked in the presence and absence of this slow depolarization (Fig. 9D). The large depolarization that is directly elicited by the depolarizing current (Fig. 9C) is an artifact due to an increase in access resistance, and the results of Fig. 9D clearly indicate that this depolarization is not responsible for the Ca2+ influx observed during TTX application. It is possible that this increase in access resistance contributed to a variable threshold for evoking the slow depolarization underlying complex spikes. However, in two other CWCs, blocking Na+ channels with TTX required a small increase (<200 pA) in the amplitude of the 4-ms somatic current pulse to recover the slow depolarization and the dendritic Ca2+ transients. This is in contrast to the results of similar experiments performed on PCs, in which large increases in the amplitude and/or duration of somatic current pulses were required to recover fluorescence increases in the presence of TTX (Figs. 6 and 7). Therefore the slow depolarization underlying complex spikes can occur in the absence of Na+ channel activation and is responsible for initiating a large Ca2+ influx into CWC dendrites.
In addition to complex spikes, CWCs can also respond with individual
fast APs (simple spikes) followed by a characteristic afterdepolarization in response to depolarizing somatic current injection (Manis et al. 1994
; Zhang and Oertel
1993
). The mode of CWC spiking has a dramatic effect on the
properties of the AP-mediated Ca2+ influx. Simple
spikes (Fig. 10B,
left) were blocked by the addition of 1 µM TTX to the
bathing medium (Fig. 10B, right). Similar to PCs,
blocking somatic APs with TTX blocked the dendritic
Ca2+ influx (Fig. 10C, solid line),
and a partial release of the Na+ channel block
during the washout of TTX sufficient to evoke one to three attenuated
APs resulted in a partial recovery of the fluorescence increase (Fig.
10C, dashed lines). In six simple spiking CWCs tested, TTX
blocked 66.6-92.2% of the fluorescence increase elicited under
control conditions. In three of these cells, a large increase in the
amplitude and duration of the somatic current injection was used to
evoke a small Ca2+ channel-mediated AP to recover
the fluorescence increase blocked by TTX. These results varied: in two
cells, 75% of the original fluorescence increase was recovered; in the
third cell, a large fluorescence increase was observed whose magnitude
was 250% of that obtained under control conditions. Although a
Ca2+ influx that was larger in TTX than under
control conditions was never observed in PC dendrites, these results
suggest that the Ca2+ influx into simple-spiking
CWC dendrites is more similar to the Ca2+ influx
into PC dendrites than to the Ca2+ influx into
complex-spiking CWC dendrites.
|
As was the case in PCs, the AP-mediated Ca2+
influx into the dendrites of CWCs is initiated by dendritic
Ca2+ channels. Consecutive applications of 1 mM
CdCl2 via pressure pipette produced local
reductions in the dendritic Ca2+ influx (Fig.
11C,
and - - -)
relative to control levels (Fig. 11C,
). Similar to the
results presented from a PC (Fig. 2), the negative
F/F values in Fig. 11C may be
attributed a reduction of background fluorescence due to the reduced
fluorescence of the Cd2+/fluo-3 complex compared
with free fluo-3. However, no apparent reduction in the background
fluorescence was observed in this cell (not shown), although the
orientation of the pressure pipette along the axis of the dendrite may
have obscured any reduction in background fluorescence. These results
were obtained from a simple-spiking CWC: the duration of somatic
current pulses was increased to elicit a pair of APs, and no slow
depolarization underlying the APs characteristic of a complex spike was
observed (Fig. 11B). Similar results were obtained from
three other simple-spiking CWCs; fluorescence recordings during a
localized application of Cd2+ were not obtained
from any complex-spiking CWCs.
|
| |
DISCUSSION |
|---|
|
|
|---|
Ca2+ and Na+ channels in pyramidal cell dendrites
Ca2+ channels are present in the apical and
basal dendrites of PCs and initiate a Ca2+ influx
in response to APs evoked by somatic depolarization. One issue that
requires additional consideration is the extent to which the
Ca2+ influx is observed throughout PC dendrites.
The present results were limited to dendritic processes within 100 µm
of the soma, and PC dendrites can extend upward of 500 µm from the
cell body (Blackstad et al. 1984
). In some cases,
measurable Ca2+ transients could be observed
where dendrites exited the field of view (e.g., Figs. 4 and 5),
indicating that the depolarization continued to propagate toward distal
dendritic processes. In other cases, Ca2+
transients rapidly tapered off with increasing distance from the soma
(e.g., Fig. 2), even though distal processes were subsequently observed
during morphologic reconstruction (not shown). A number of factors
could prevent the observation of Ca2+ transients
in more distal processes, including variations in process depth
relative to the focal plane, or fluorescence intensities not
significantly above background levels due to small process volumes or
inadequate dye spread. Therefore it is reasonable to assume that the
dendritic Ca2+ influx evoked by APs extends into
dendritic processes beyond those visualized in the present study.
Dendritic Ca2+ channels can contribute to the
integration of spatially segregated ANF and PF inputs by modulating
synaptic responses in an activity-dependent fashion. Coincident
synaptic inputs and activation of dendritic conductances by APs produce
changes in synaptic efficacy (Bell et al. 1997
;
Magee and Johnston 1997
; Markram et al.
1997
). Activation of
N-methyl-D-aspartate receptors, which are
present at PF synapses in PCs (Bilak et al. 1996
;
Manis and Molitor 1996
), may contribute to this
modulation of postsynaptic responses by augmenting an AP-evoked
dendritic Ca2+ influx (Schiller et al.
1998
). Therefore, suprathreshold ANF-mediated inputs in the
basal dendrites of a PC could propagate to PF synapses in the apical
dendrites, altering the subsequent postsynaptic responses to
PF-mediated inputs that were coincidentally active. This modulation
could occur independently of coincident inputs: PCs exhibit high rates
of intrinsic spontaneous activity (Waller and Godfrey
1994
), which would generate a dendritic
Ca2+ influx and potentially lead to an ongoing
modulation of postsynaptic responses to excitatory inputs.
Although APs, presumably mediated by somatic and axonal
Na+ channels, initiate a
Ca2+ influx into PC dendrites, the results of the
present study suggest that dendritic Na+ channels
are not necessary for the retrograde activation of dendritic Ca2+ channels. Individual
Na+ channel-mediated APs evoke a
Ca2+ influx into the dendrites of hippocampal and
cortical PCs (Markram et al. 1995
; Spruston et
al. 1995
), which possess dendritic Na+
channels (Jaffe et al. 1992
; Stuart and Sakmann
1994
), but not into the dendrites of cerebellar Purkinje
neurons (Lev-Ram et al. 1992
; Ross and Werman
1987
), which lack a sufficient density of dendritic
Na+ channels (Stuart and Häusser
1994
). In the DCN, a Ca2+ influx into PC
dendrites could still be observed during the direct application of TTX
to dendritic processes at levels sufficient to partially block somatic
APs. Furthermore, dendritic Ca2+ transients could
be evoked when a large somatic depolarization was presented in the
complete absence of APs during TTX block. Again, these conclusions are
limited to observations made from proximal dendrites, and it is
possible that the contribution of dendritic Na+
channels is required for a depolarization to spread into distal processes.
Ca2+ Channels in CWC dendrites
One striking difference between CWCs in this study and
morphologically identified CWCs in previous studies (Ding et al.
1999
; Golding and Oertel 1996
, 1997
;
Manis et al. 1994
; Zhang and Oertel 1993
)
is the inability of some CWCs to respond with complex spikes to
depolarizing stimuli. Otherwise, this subpopulation of simple-spiking CWCs appears to be normal: fast Na+
channel-mediated APs were followed by an afterdepolarization (e.g.,
Fig. 10B) as observed in sharp-electrode recordings from CWCs in guinea pig DCN (Manis et al. 1994
). The most
obvious differences between the present and previous studies are the
use of different rodent species (rat vs. mouse, guinea pig, and
gerbil), the ages of the animals used, and the use of whole cell
recordings instead of sharp-electrode recordings. Bursting units were
observed in extracellular recordings from rat DCN (Waller and
Godfrey 1994
), so it is unlikely that the difference in CWC
responses can be attributed solely to the species used. The use of
whole cell recordings could prevent complex spikes by disrupting normal
Ca2+ buffering processes, leading to a
Ca2+-dependent activation of
K+ channels and/or a
Ca2+-dependent inactivation of
Ca2+ channels in some CWCs. Although not
representative of the responses typically observed in CWCs, the
presence of a simple-spiking CWC subpopulation provided an opportunity
to investigate the differences between the electrophysiologic
mechanisms underlying the generation of simple and complex spikes.
In contrast to PCs, the dependence of the dendritic Ca2+ influx on Na+ channel-mediated APs depends on the firing mode of CWCs. Although both simple and complex spikes evoke a Ca2+ influx, only complex spikes elicit a large dendritic Ca2+ influx that is not dependent on Na+ channel activation. The data in this study confirm the existence of Ca2+ channels in CWC dendrites; however, it is unclear from these data whether dendritic Ca2+ channels contribute to the slow depolarization observed in somatic recordings or if these channels only generate a Ca2+ influx in response to the slow depolarization initiated by more proximal Ca2+ channels. A correlation between the slow depolarization underlying complex spikes and a dendritic Ca2+ influx suggests that dendritic Ca2+ channels may contribute to the generation of complex spikes. However, repetitive simple spikes evoked similar dendritic Ca2+ transients with little or no evidence of the slow depolarization associated with complex spiking. In addition, blocking Na+ channels had little or no effect on the threshold for evoking the slow underlying depolarization as would be expected if this slow depolarization were generated by Ca2+ channels remote to the site of depolarizing current injection. Although further investigation is required, complex spikes are likely to be generated by a coordinated action of somatic and dendritic Ca2+ channels.
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ACKNOWLEDGMENTS |
|---|
This work was supported by National Institute on Deafness and Other Communication Disorders Grant R01 DC-00425 to P. B. Manis.
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FOOTNOTES |
|---|
Address for reprint requests: S. C. Molitor, Dept. of Bioengineering, University of Toledo, 5051 Nitschke Hall, Toledo, OH 43606-3390 (E-mail: smolitor{at}eng.utoledo.edu).
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REFERENCES |
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