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The Journal of Neuroscience, December 15, 2000, 20(24):9059-9070
Origin Sites of Calcium Release and Calcium Oscillations in Frog
Sympathetic Neurons
Stefan I.
McDonough,
Zoltán
Cseresnyés, and
Martin F.
Schneider
Department of Biochemistry and Molecular Biology, University of
Maryland Medical School, Baltimore, Maryland 21201
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ABSTRACT |
In many neurons, Ca2+ signaling depends on
efflux of Ca2+ from intracellular stores into the
cytoplasm via caffeine-sensitive ryanodine receptors (RyRs) of the
endoplasmic reticulum. We have used high-speed confocal microscopy to
image depolarization- and caffeine-evoked increases in cytoplasmic
Ca2+ levels in individual cultured frog sympathetic
neurons. Although caffeine-evoked Ca2+ wave fronts
propagated throughout the cell, in most cells the initial
Ca2+ release was from one or more discrete sites
that were several micrometers wide and located at the cell edge, even
in Ca2+-free external solution. During cell-wide
cytoplasmic [Ca2+] oscillations triggered by
continual caffeine application, the initial Ca2+
release that began each Ca2+ peak was from the same
subcellular site or sites. The Ca2+ wave fronts
propagated with constant amplitude; the spread was mostly via
calcium-induced calcium release. Propagation was faster around
the cell periphery than radially inward. Local Ca2+
levels within the cell body could increase or decrease independently of
neighboring regions, suggesting independent action of spatially separate Ca2+ stores. Confocal imaging of
fluorescent analogs of ryanodine and thapsigargin, and of MitoTracker,
showed potential structural correlates to the patterns of
Ca2+ release and propagation. High densities of RyRs
were found in a ring around the cell periphery, mitochondria in a
broader ring just inside the RyRs, and sarco-endoplasmic reticulum
Ca2+ ATPase pumps in hot spots at the cell edge.
Discrete sites at the cell edge primed to release
Ca2+ from intracellular stores might preferentially
convert Ca2+ influx through a local area of plasma
membrane into a cell-wide Ca2+ increase.
Key words:
ryanodine receptor; sympathetic neuron; caffeine; confocal microscopy; calcium; calcium wave; calcium oscillations; calcium-induced calcium release; subsurface cistern; fluo-4
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INTRODUCTION |
Cytoplasmic
Ca2+ levels in neurons govern many
signaling processes, including neurotransmitter secretion, regulation
of membrane excitability, and induction of gene expression (Kennedy,
1989 ; Clapham, 1995 ; Ghosh and Greenberg, 1995 ). Cytoplasmic
Ca2+ concentrations are increased by
influx of extracellular Ca2+ through
plasma membrane Ca2+ channels and by
release of Ca2+ from within intracellular
organelles, especially the endoplasmic reticulum (ER), that serve as
Ca2+ stores (Berridge, 1998 ). Although the
ER may be a continuous membrane system throughout the neuron (Berridge,
1998 ), different parts of the ER may act separately for purposes of
Ca2+ signaling (Golovina and Blaustein,
1997 ; Meldolesi and Pozzan, 1998 ). Two prominent pathways for release
of Ca2+ from within the ER into the
cytoplasm are via ryanodine receptors (RyRs) or inositol
1,4,5-trisphosphate receptors (InsP3Rs) located on the ER membrane. Both molecules are
Ca2+ channels that are themselves gated by
cytoplasmic Ca2+; RyRs are also opened
pharmacologically by millimolar concentrations of caffeine (Rousseau et
al., 1988 ; McPherson et al., 1991 ). Local Ca2+ release can induce
Ca2+ release from neighboring sites,
amplifying the initial release into Ca2+
wave fronts.
Oscillations of cytoplasmic Ca2+ levels
are a striking form of signaling in which RyRs or
InsP3Rs govern repetitive release from
intracellular Ca2+ stores in response to a
constant external stimulus. Such oscillations occur with distinct
frequencies and shapes and have been observed in many kinds of
excitable and nonexcitable cells (Tsien and Tsien, 1990 ; Fewtrell,
1993 ). Oscillations evoke secretion in hepatocytes, pancreatic acinar
cells, and gonadotrophs (Tepikin and Petersen, 1992 ; Hille et al.,
1994 ). The precise oscillation frequency has been shown to control
specific patterns of gene expression (Dolmetsch et al., 1998 ; Li et
al., 1998 ), the activation of
Ca2+-sensitive enzymes (De Koninck and
Schulman, 1998 ), and the speed and direction of neuronal
migration (Gu and Spitzer, 1995 ; Komuro and Rakic, 1996 ; Flint et al.,
1999 ; Gomez and Spitzer, 1999 ). An especially well studied model system
of neuronal Ca2+ oscillation occurs in
cultured sympathetic ganglion neurons from grass frog or bullfrog that
are exposed continually to caffeine or to caffeine plus depolarization
(Kuba and Nishi, 1976 ; Smith et al., 1983 ; Lipscombe et al.,
1988a ,b ; Friel and Tsien, 1992b ; Friel, 1995 ; Cseresnyés et al.,
1999 ). The physiological trigger for
[Ca2+] oscillations may be repetitive
fast spiking (Peng, 1996 ). Most information about these oscillations
has come from whole-cell fluorescence or patch-clamp recordings in
which any subcellular spatial information is necessarily lost. Local
Ca2+ regulation, however, occurs in
neuronal dendrites (Finch and Augustine, 1998 ; Takechi et al., 1998 ;
Koizumi et al., 1999a ), contributes to the functions of some secretory
cells (Pozzan et al., 1994 ; Thomas et al., 1996 ; Tse et al., 1997 ), and
governs the direction of growth cone extension (Hong et al., 2000 ;
Zheng, 2000 ). Local Ca2+ signaling within
the soma could be equally important. Here we find evidence for local
release and nonuniform propagation of Ca2+
in these neurons.
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MATERIALS AND METHODS |
Cell culture. Cultured sympathetic neurons were
prepared as previously described (Cseresnyés et al., 1997 ).
Briefly, frogs (Rana pipiens) were packed in ice for 20-30
min, decapitated, and pithed, according to guidelines issued by the
Institutional Animal Care and Use Committee, University of Maryland
(Baltimore, MD). Sympathetic ganglion chains from three frogs were
removed into ice-cold Ringer's solution containing (in
mM): 128 NaCl, 2 KCl, 10 glucose, 10 HEPES, pH
adjusted to 7.3 with NaOH, with 0 added
Ca2+, manually desheathed, and
enzymatically digested with 3 mg/ml collagenase for 20-40 min and then
with 2 mg/ml trypsin for 7-9 min. After washing, individual cells were
released from the ganglia by gentle trituration with a polished Pasteur
pipette and plated onto cover glasses (VWR no. 1) coated with
poly-L-lysine. Cells were maintained in culture
for 2-5 d in a 50:50 mixture of Liebovitz's L-15 medium (Life
Technologies, Gaithersburg, MD) with 0.1% phenol red and Ringer's
solution [2 mM Ca2+
Ringer's supplemented with 25 µg/ml ascorbic acid, 2.5 µg/ml glutathione, 0.25 µg/ml 6,7-dimethyl-5,6,7,8-tetrahydropterine (DMPH), and 0.5 µl/ml gentamicin, pH 7.3].
Imaging. Cells were washed with 2 mM
Ca2+ Ringer's and loaded with 2 µM fluo-4-AM (Molecular Probes, Eugene, OR) at
room temperature for 20-25 min. Endogenous esterases converted
nonfluorescent fluo-4-AM into fluorescent fluo-4. Culture dishes were
placed on the stage of an inverted microscope (Nikon Diaphot 300) and
imaged with a Nikon RCM-8000 real-time confocal microscope (Tsien and
Bacskai, 1995 ). The focus was set at the widest area of the cell, which was at or near the vertical center. Cells were continuously superfused with a 2 mM Ca2+ or 0 Ca2+ Ringer's bath solution flowing at
~5 ml/min, and caffeine or high-K+
Ringer's solution was microperfused onto an individual cell through a
quartz perfusion head (internal diameter, 100 µm; Adams and List
Associates, Westbury, NY). The internal diameter of the microperfusion pipette was approximately double the diameter of the widest part of the
cell, making local caffeine gradients unlikely. The microperfusion pipette was always positioned just above the focal plane of the recorded cell image and to the left of the cell, ~50 µm away. Epifluorescent excitation for fluo-4 was with the 488 nm line of an
argon-ion laser (Coherent, Santa Clara, CA), and emission was collected
at > 510 nm. Fluo-4 fluorescence before caffeine application
was mostly uniform, but often brighter in the center of the cell.
Before dye loading, autofluorescence was visible in some cells as
bright spots, especially in the cell center. Addition to the bath of
0.005% saponin in 0 Ca2+ Ringer's with
10 mM added EGTA rapidly quenched an average of 86% of the whole-cell confocal fluorescence after fluo-4 loading (n = 4), indicating a predominantly cytoplasmic
localization of the dye. The in vitro
KD of fluo-4 for
Ca2+ is 345 nM
(Molecular Probes). Whole-cell peak Ca2+
signals measured previously with fura-2 were ~1
µM for the first and <350
nM for subsequent
Ca2+ peaks within a caffeine-evoked
oscillation cycle (Cseresnyés et al., 1999 ), so the fluo-4 was
unlikely to be saturated.
For measurements of the direct effects of caffeine on indo-1
fluorescence (Muschol et al., 1999 ), neurons were loaded with 15-20
µM indo-1-AM (Molecular Probes) for 20-25 min at room
temperature. Cells were pretreated with 2 µM thapsigargin
(TG) (Sigma, St. Louis, MO) for at least 2 min to fully release
Ca2+ from intracellular stores and
eliminate any rise in Ca2+ on caffeine
application (Cseresnyés et al., 1999 ). Excitation was at 351 nm
(argon-ion laser), and emission was collected at 360 nm < < 440 nm. Ca2+-dependent
emission from indo-1 would increase emission intensity at these
wavelengths, whereas the thapsigargin-treated cells responded to
caffeine with a decrease in emission intensity, verifying that a direct
caffeine-dye interaction, not a Ca2+-dye
interaction, caused the change in fluorescence. The
Ca2+-independent emission obviated the
need to quantify the de-esterification of indo-1-AM.
Cells were imaged with a 60× NA 1.2 water-immersion objective lens
(Nikon, with correction collar to compensate for the thickness of the
coverslip) to image the middle of the cell without the refractive index
mismatch of an oil-immersion lens. The spatial resolution was estimated
by imaging a single, 100 nm fluorescent bead in water. In the focal
plane, the fluorescence intensity in the x and y
directions was fit by a Gaussian function with full width at
half-maximum (FWHM) of 0.3-0.4 µm. Axial (z) resolution for the confocal pinhole setting used, determined by collecting the
total emission from the bead while incrementing the z
position, was fit by a Gaussian function with FWHM of 1.5-2 µm. A
few cells were imaged with a Nikon 40× NA 1.15 water-immersion lens.
Emission values were digitized with an eight-bit converter. Data were
collected at video rate with a two-frame average for an effective 15 Hz sampling rate (66 msec/frame). Images were analyzed with software custom-written in the IDL programming language (Research Systems, Boulder, CO). The whole-cell confocal fluorescence time courses are the
average of unsubtracted pixel values within either the entire cell or
the area indicated, except as noted. All displayed images were
background-subtracted, with an average of four or five consecutive
image frames acquired before changes in fluorescence. Pixels for which
the averaged background image was larger than the displayed image were
set to zero. Where noted, images were smoothed in space and time with a
3 × 3 × 3 kernel. Smoothing was used in cells in which the
subtracted signal was too dim to be apparent in still-frame images.
Smoothing distorted the precise site of initiation, but made the
propagation of the wave front much clearer. Grayscale shading for each
pixel was set according to the look-up table bar in each figure. In the
text, positions at the cell edge are sometimes referred to with
"o'clock" terminology, with the position in the cell referred to
by the corresponding hour hand of a clock oriented with 12 at the top.
Staining. RyRs were stained with either Bodipy FL-X
ryanodine (green emission) or TR-X ryanodine (red emission) (Molecular Probes). Green emissions were recorded from 515 to 560 nm, and red
emissions were recorded from 580 to 630 nm, as determined by the
spectra of the excitation and emission dichroic. Cells were loaded at
room temperature with 250 nM dye in Ringer's
solution + 10 mM caffeine to promote
high-affinity ryanodine binding to an open state of the RyR. The
solution was changed to dye-free Ringer's before excitation with the
488 nm line of the argon-ion laser or with the 568 nm line of the
krypton-argon laser, respectively, for the green or red emission
fluorophores. The typical pattern of RyR staining around the
circumference of the cell appeared after ~2 min of dye incubation.
Incubation of up to 8 min resulted in brighter emission at the
circumference but no increase in brightness in the interior of the
cell. Mitochondria were stained with 250 nM
MitoTracker Green FM (Molecular Probes) for 30 min at room temperature;
the dye was washed off before imaging. For cells that were costained
with MitoTracker green and TR-X red ryanodine and dually imaged, some
emission from the green MitoTracker was recorded in the red channel.
For cells stained only with MitoTracker green, the ratio of intensity
in red divided by intensity in green for the brightest parts of the
image was 0.11. Each red image taken after staining with both red
ryanodine and MitoTracker green was corrected for green bleed-through
by subtracting pixel by pixel with 0.11× the corresponding
pixel value from the corresponding green image. There was no
bleed-through of red ryanodine into the green emission channel. To
stain for sarco-endoplasmic reticulum calcium ATPase (SERCA) pumps,
cells were loaded with 1 µM Bodipy thapsigargin
(Molecular Probes) in Ringer's solution at room temperature for 1 min,
a concentration and exposure time sufficient to release Ca2+ from within stores and to suppress
the response to 10 mM caffeine (Cseresnyés
et al., 1997 ). After washout of TG from the bathing medium, imaging
revealed discrete hot spots of fluorescence at the edges of the cell.
Hot spots first appeared ~30 sec after addition of labeled TG, and
the pattern was unchanged after 3 min.
Movies. Image series for selected figures (see Figs.
1, 3, 4, 7) were written as movies in Moving Picture Experts Group
(MPEG) format with IDL software and are available as
supplemental information for this paper. (Please see
http://www.jneurosci.org.) Movies can be viewed with Windows Media
Player (Microsoft, free software download available at
www.microsoft.com/windows/windowsmedia/en/download/default.asp; operating system requirements listed at
www.microsoft.com/windows/mediaplayer/en/download/sysreq.asp), or with
other software capable of playback of MPEG files at 30 frames
per second. Because images were recorded at 15 Hz, although movie
playback is at 30 Hz, movies were written with a copy of each frame
interleaved between each frame and the subsequent frame, so the movie
gives a real-time image of Ca2+ spread
within the cell. For the movie of Figure 7, the interoscillation period
of unchanging fluorescence was cut out to conserve computer memory, and
each Ca2+ peak was background-subtracted,
with an average of five frames taken before the
Ca2+ rise that began each individual peak.
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RESULTS |
Initiation of Ca2+ release from the
cell periphery
Cell depolarization by microperfusion of a 50 mM
K+, 2 mM
Ca2+ Ringer's solution onto a neuron
evoked a fluorescence increase (Fig.
1A, left),
presumably initiated by entry of extracellular Ca2+ into the cytoplasm through
voltage-gated Ca2+ channels of the plasma
membrane. In the confocal section, this depolarization-evoked
fluorescence began as a uniform ring around the cell periphery, as
expected for a uniform distribution of voltage-gated
Ca2+ channels (Lipscombe et al., 1988a ;
Hernandez-Cruz et al., 1990 ), and then spread gradually inward (Fig.
1B, image series 1). Peak fluorescence was
attained after the images shown in this series and was uniform across
the cell, except for a higher emission intensity from the nucleus
(Hernandez-Cruz et al., 1990 ; Perez-Terzic et al., 1997 ). Instead of a
higher nuclear Ca2+ concentration, this is
likely to reflect a different solvation environment for the fluo-4 dye
in nuclear and non-nuclear compartments (Perez-Terzic et al.,
1997 ). Fluorescence decayed to baseline levels after returning
the cell to Ca2+-free Ringer's solution.
Full Ca2+ removal was confirmed by the
lack of fluorescence increase evoked by microperfusion of 50 mM K+, 0 Ca2+ Ringer's (Fig. 1A,
center).

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Figure 1.
Caffeine evokes release of Ca2+
from a discrete site at the cell edge. For this cell, the continuously
flowing bath solution was frog Ringer's solution without added
Ca2+. A, Time course of confocal
fluorescence averaged from within the entire cell in response to
microperfusion of Ringer's solution containing 50 mM
K+ and 2 mM Ca2+
(left, trace 1); 50 mM
K+ and zero added Ca2+
(middle); and 2 mM K+, 0 Ca2+ with 10 mM caffeine
(right, trace 2). There is a 2 min
interval between the left and middle
panels, sufficient time for recovery of responsiveness to
high-K+ stimulation (Friel and Tsien, 1992a ), and a
1 min interval between the middle and right
panels. B, Image series 1 and
2 are consecutive images taken from the areas under
traces 1 and 2 in A,
marked with the horizontal bars. The
arrow in image series 2 indicates the
site of fluorescence initiation. Pixel values from 0 to 80 were
assigned brightness according to the grayscale look-up
bar. Scale bar, image series 1, 10 µm.
C, Time course of the fluorescence in small subcellular
areas during depolarization and caffeine application.
Left, Map of the cell showing the
subcellular areas from which the fluorescence signal in
A was further analyzed. Right, Time
course of the change in fluorescence (arbitrary units) within the
subarea of the corresponding color at the onset of fluorescence of
traces 1 (50K) and 2 (caffeine).
Open circles, shown only for the black subarea, indicate
the sampling interval of 66 msec. Each tick on the
x-axis is 1 sec. Scale bar, 10 µm. Please see
associated movie of the responses to 50 mM
K+ and to caffeine (B) in the
electronic version of this paper.
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Cytoplasmic Ca2+ levels were also
increased by evoking release of Ca2+ from
intracellular stores. Efflux via RyRs was evoked pharmacologically by
microperfusion of 10 mM caffeine. In this cell, application of caffeine in Ca2+-free Ringer's
solution evoked a fluorescence increase (Fig. 1A, right), consistent with whole-cell studies showing that
extracellular Ca2+ is not required for the
release of Ca2+ from intracellular stores
(Neering and McBurney, 1984 ; Lipscombe et al., 1988a ; Thayer et al.,
1988 ; Friel and Tsien, 1992a ; Cseresnyés et al., 1997 , 1999 ).
Cytoplasmic Ca2+ is a physiological ligand
for RyRs. Caffeine increases RyR Ca2+
sensitivity, possibly analogous to the effects of cyclic ADP-ribose or
other modulatory pathways (Rousseau et al., 1988 ; Sitsapesan and
Williams, 1990 ; McPherson et al., 1991 ; Hua et al., 1994 ; Empson and
Galione, 1997 ), thereby allowing the Ca2+
release at resting Ca2+ levels observed
here. Ca2+ stores governed by
InsP3 receptors, if present at all in these amphibian neurons, are labile and quite small compared with the stores
governed by RyRs (Pfaffinger et al., 1988 ; Friel and Tsien, 1992a ) (but
see Kirkwood et al., 1991 ). We cannot, however, exclude the possibility
that the Ca2+ signal includes some
component of Ca2+ release through
InsP3Rs.
The caffeine-evoked increase in
Ca2+-dependent fluorescence began at a
single discrete site on the right edge of the cell, presumably at the
low side of any caffeine gradients attributable to microperfusion from
the left (Fig. 1B, image series 2). From
the site of release, the Ca2+ spread
around the cell periphery, faster in the counterclockwise than the
clockwise direction, followed by radial spread into the center (Fig.
1B, image series 2, C,
right). Ca2+ reached different
sites around the cell edge with a delay, but without decrement of the
amplitude (Fig. 1C). The rise of fluorescence at each
peripheral location was rapid, going from baseline to a near-maximal
change in two or three images (66 msec/image). From the difference in
the time to half-maximal fluorescence at the release initiation site
(black), at the cell periphery opposite the origin
(orange), and at the cell center (light blue),
the one-dimensional speed of Ca2+
propagation with caffeine can be estimated as 130 µm/sec clockwise and 230 µm/sec counterclockwise around the cell periphery, and 40 µm/sec radially inward. Because free
Ca2+ would be expected to diffuse
decrementally in all directions from a single release site, much of the
Ca2+ propagation must have been caused by
a process other than passive diffusion. This process was likely
regenerative calcium-induced calcium release (CICR) among RyRs
distributed through the cell. In eight neurons, with caffeine, the
circumferential propagation speed averaged 204 ± 39 µm/sec, and
radial propagation averaged 49 ± 6 µm/sec
(p < 0.012; unpaired t test).
Assuming minimal anisotropies in the diffusion path for
Ca2+ in the cytoplasm, the slower radial
propagation implies a greater propensity for CICR around the periphery
than toward the center of the cell. In the cell of Figure 1, the speed
of inward propagation during depolarization without caffeine
(image series 1) was 20 µm/sec. This is only an upper
bound on the rate of Ca2+ diffusion
because Ca2+ elevation during
depolarization evokes a degree of CICR even in the absence of caffeine
(Friel and Tsien, 1992a ; Hua et al., 1993 , 1994 ; Llano et al., 1994 ;
Shmigol et al., 1995 ; Peng, 1996 ; Usachev and Thayer, 1997 ). In
the same eight neurons, inward radial propagation speed in response to
high-K+ depolarization was 26.9 ± 6.2 µm/sec, whereas inward radial propagation in the same cells
during subsequent exposure to 10 mM caffeine, after return to baseline fluorescence in Ringer's solution, measured as 49.0 ± 6.9 µm/sec (p < 0.02). The
ratio of speed in caffeine to speed in
high-K+ was 2.5 ± 0.5.
The caffeine dependence of propagation speed was tested by evoking
Ca2+ release first with 5 mM
and then, after washout, with 20 mM caffeine. In three of
three cells, Ca2+ release originated at
the same peripheral site with 20 mM as with 5 mM; in one of the three cells, release was also seen from a
second site. The one-dimensional peripheral propagation speed evoked by
5 and 20 mM caffeine applied to each of the former two cells increased from ~90 to ~430 µm/sec and from ~100 to ~350 µm/sec. Because the concentration and mobility of dye and of
endogenous buffers was the same for both applications of caffeine, the
increase in speed can be attributed to an increased fraction of CICR.
Spread of intracellular caffeine
At a given intracellular location, the local cytoplasmic
concentrations of caffeine and fluo-4, as well as
Ca2+, influence the observed fluorescence
signal. The proportion of a given area that is occupied by cellular
organelles, and thus effectively inaccessible to the dye, would also
affect emission intensity. Detection of fluorescence itself confirms
the presence of fluo-4 in a given area, whereas the homogenous increase
of cytoplasmic fluorescence during peak responses to caffeine (Figs. 1,
3, 7, 9) provides some evidence against gross inequalities in fluo-4
distribution among different regions of the cytoplasm at this
resolution. Because caffeine must diffuse across the plasma membrane
and through the intracellular milieu to act on RyRs of the ER membrane,
the recorded fluorescence could reflect regional differences in
caffeine, not Ca2+. To monitor
intracellular caffeine levels during external application of caffeine,
fluorescence of cells loaded with the dye indo-1 was measured in
response to extracellular microperfusion of 10 mM caffeine.
Cells were pretreated with thapsigargin to eliminate Ca2+-dependent fluorescence (see Materials
and Methods). Caffeine reduced the intracellular indo-1 fluorescence
emission intensity at 360 nm < < 440 nm, wavelengths at
which Ca2+ binding increases indo-1
emission intensity. Thus we attributed the decrease in emission to a
direct caffeine-dye interaction (Muschol et al., 1999 ) and used it to
measure the penetration of caffeine within the cell. Figure
2 shows the magnitude and time course of
indo-1 fluorescence averaged over the entire outline of a cell image
and from within each of five numbered, arbitrarily chosen subareas.
Each panel shows on the same scale the change in fluorescence from the
correspondingly numbered subarea (noisy solid line) and from the entire
cell (less noisy line) in response to the same caffeine application.
The total amplitude decrease was the same for all subareas. The time to
50% decay was shortest at the left side of the cell, closest to the
caffeine application, and slowest in the middle (Fig. 2, legend), but
the greatest difference in time between any two subareas was 290 msec.
In results pooled from the two left and two right subareas of three
cells, the 50% decay time was reached more quickly than the whole-cell
average, by 159 ± 84 msec at the left side and by 29 ± 34 msec at the right side (mean ± SD; n = 6). The
decay time at the center of the cell (subarea 1) was 92 ± 8 msec
slower than the whole-cell time course (mean ± SD;
n = 3). We conclude that caffeine permeates the
membrane rapidly in these cells and equilibrates with only minor
differences among different regions of the cell. This further
implies that the local signaling events that were observed reflected
elevations of intracellular Ca2+, and not
caffeine. In a different cell, release of
Ca2+ from a discrete site at the cell edge
was observed ~20 min after bath application of caffeine (data not
shown), obviously well after equilibration of intracellular
caffeine.

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Figure 2.
Time course of caffeine spread within a cell. The
decrease in indo-1 emission intensity on caffeine application was used
to detect the time course of caffeine within a thapsigargin-treated
cell (see Materials and Methods). Top left,
Outline of a cell and of five arbitrarily chosen
subareas within the cell. Arrows to the
left of the cell outline show the
direction of external caffeine microperfusion. In each numbered
panel, the fractional change in average fluorescence within the
correspondingly numbered subarea (noisy
trace) is plotted together with the fractional change in
fluorescence averaged from within the entire cell (less noisy
trace, mostly superimposed on the subarea fluorescence).
Each tick on the x-axis represents 2 sec. The decay for
each subarea was fit well by a single Boltzmann function. The 50%
decay time for each subarea minus the 50% decay time for the whole
cell average was as follows: area 1, +82 msec; area 2, 198 msec; area
3, 208 msec; area 4, 47 msec; area 5, 55 msec.
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Sites of preferential Ca2+ release
Propagation of elevated Ca2+ via
regenerative CICR suggests that many sites throughout the cell are
capable of releasing Ca2+. Caffeine was
applied multiple times to a single cell to test whether the site of
initial release was random, or whether it might reflect functional
differences among RyRs (Fig. 3). In
response to each caffeine application, fluorescence increased first at a discrete site in the distal part of a growth cone and propagated from
there into the cell body. Because the base of the growth cone was in
the same focal plane as the cell body, for this cell the actual initial
Ca2+ increase in the cell body occurred
unambiguously within the recorded confocal section. Although
Ca2+ increases were eventually recorded
from the entire intracellular area, significant nonuniformities in
fluorescence initiation and spread occurred well after the ~0.5 sec
required for caffeine to reach all points within the cell, providing
evidence for functional differences among stores. Before the increase
from the growth cone had extended over the entire perimeter of the
cell, another localized increase in fluorescence was observed at
arbitrarily labeled site "a " at the right edge of the
cell (blue box), opposite the direction of caffeine
microperfusion, without Ca2+ increases in
the intervening regions (Fig. 3C). In addition, whereas
Ca2+ spread smoothly from the base of the
growth cone symmetrically in the clockwise and counterclockwise
directions during the first caffeine application,
Ca2+ spread much more slowly after
subsequent caffeine applications, especially in the radial and
clockwise directions. These same patterns of initiation and
propagation were recorded for each of five separate caffeine
applications to the cell (Fig. 3), further supporting the idea that the
site (or sites) where release initiates is not random, but rather an
intrinsic Ca2+ release property of the
site itself.

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Figure 3.
Origin and spread of intracellular
Ca2+ in response to successive applications of
caffeine. A, Time course of average fluorescence within
the entire cell in response to five successive applications of 10 mM caffeine. Record is discontinuous between caffeine
applications; fluorescence returned to baseline in the interpeak
intervals. B, Consecutive confocal images corresponding
to the indicated intervals (A, bars) during the upstroke
of each of the first three peaks in the whole-cell confocal
fluorescence time course. The grayscale look-up bar
represents pixel values from 0 to 80. Arrow in each
image series indicates the point of first increase in fluorescence on
stimulation with caffeine. Scale bar, 10 µm. C,
Left, Outline of the cell, with labeled
arbitrary subareas marked with boxes, and arbitrary
spatial reference points a and b.
Right, Time course of fluorescence during the first
three caffeine applications within the subarea defined by the
correspondingly colored box. Each tick on the
y-axis represents 10 arbitrary fluorescence units
calculated from background-subtracted images (note different scale for
different caffeine applications). Please see associated movie of the
first three caffeine applications to this cell (B, 1-3)
in the electronic version of this paper.
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Caffeine was applied to a total of 67 cells in either
Ca2+-free or 2 Ca2+ Ringer's solution. In 47 cells, the
increase in fluorescence began at one or more discrete sites, always at
the edge of the cell. Conceivably, a tonic influx of external
Ca2+ might have resulted in a higher
cytoplasmic Ca2+ concentration near the
plasma membrane, and consequently in easier CICR at the cell edges, but
the lack of a requirement for Ca2+ influx
for caffeine-evoked Ca2+ release argues
against this (Fig. 1) (Neering and McBurney, 1984 ; Lipscombe et
al., 1988a ; Thayer et al., 1988 ; Friel and Tsien, 1992a ;
Cseresnyés et al., 1997 , 1999 ). The initial
Ca2+ release was at the left side of the
cell in 32 of 47 cells, presumably reflecting a transiently higher
caffeine concentration closer to the microperfusion pipette (Fig. 2).
Increase initiated at the right side of the cell (Fig. 1), opposite to
the direction of caffeine application, in 5 of 47 cells. (In
seven cells, release initiated from both the left and right sides of
the cell, and in three cells release initiated from the top or bottom
of the imaged plane of the cell.) This suggests differences in caffeine sensitivity among different release sites (see Discussion).
In 20 of 67 cells, caffeine caused a fluorescence increase that
occurred with a diffuse pattern, arising either simultaneously across
the entire cell, or from diffuse bands extending more than one-fourth
of the way around the cell perimeter (data not shown). In these cells,
the actual Ca2+ release could have
occurred simultaneously throughout the cell, as recorded, or could have
propagated from a single release site outside the focal plane to appear
as a more uniform rise of Ca2+ in the
recorded plane. Because release from discrete sites in a
three-dimensional cell would sometimes be expected to appear in
two-dimensional confocal recordings as a diffuse rise, we prefer the
explanation that actual Ca2+ release was
always from a discrete site, rather than invoking different release
mechanisms among neurons of the same type. This interpretation is
supported by a recording of three consecutive caffeine applications to
the same cell made with the focal plane set to the center of the cell
(z = 0), to 8 µm above the center (z = +8), and to 8 µm below the center (z = 8). With
the focus at z = 0, the
Ca2+ release initiated from a broad band
covering the top half of the image; at z = +8, release
initiated from a small site several micrometers wide at ~11 o'clock
on the cell edge; and at z = 8, release initiated
evenly over the entire confocal image (data not shown). The patterns
observed at each focal plane are consistent with initiation of
Ca2+ release from a discrete site at
z = +8 on each caffeine application. Assuming that
successive caffeine applications evoked
Ca2+ release from the same site each time,
as in the cell of Figure 3, this suggests that the diffuse patterns of
Ca2+ release recorded from 20 cells were
caused by propagation from a discrete release site that was out of focus.
Sites of Ca2+ release during oscillations in
intracellular Ca2+ levels
To determine whether discrete sites of release were maintained
during oscillations in cytoplasmic Ca2+
levels (Lipscombe et al., 1988a ,b ; Friel and Tsien, 1992b ; Friel, 1995 ;
Cseresnyés et al., 1999 ), oscillations were evoked by steady microperfusion of 10 mM caffeine in 2 mM
K+, 2 mM
Ca2+ Ringer's solution. The amplitude of
each peak decreased during the oscillation train. This decrease was
also seen in whole-cell recordings exhibiting decreasing oscillations
monitored with the ratiometric Ca2+
indicator fura-2 (Cseresnyés et al., 1999 ), so the records here may reflect actual decreases in Ca2+
levels rather than photobleaching of the fluo-4. Because caffeine was
applied continuously to evoke oscillations, patterns of
Ca2+ release after the first
Ca2+ peak occurred in the presence of a
uniform intracellular caffeine concentration. Figure
4 displays images from a cell that
responded to continual caffeine application with a cycle of eight
oscillation peaks (A). For the first peak,
fluorescence increase was first observed over an area ~2 × 2 µm at ~11 o'clock (B, image series 1,
frame 3, arrow) and spread from there.
Fluorescence increased two frames (132 msec) later at a second site, at
~2 o'clock (B, image series 1, frame
5, arrow). For each of the seven subsequent Ca2+ peaks in the oscillation cycle,
fluorescence increased at that same 2 o'clock site before increasing
in the rest of the cell (Fig. 4B, image series
2, 3; C; movie). Fluorescence at the release site increased and then stayed constant during the rising phase of the
whole-cell fluorescence (Fig. 4C), suggesting that
Ca2+ release was completed at the
initiation site as the wave front propagated. Release did not initiate
again from the first (11 o'clock) site, suggesting that release at
that site reflected proximity to the direction of caffeine application.
Thus, the timing of a cell-wide Ca2+
increase during Ca2+ oscillations was
determined by Ca2+ release at a single
site. These neurons appear to have an "oscillator" site at the cell
edge from which release initiates, as reported for
InsP3-evoked Ca2+
oscillations in some nonexcitable cells (Rooney et al., 1990 ; Pozzan et
al., 1994 ). In all neurons recorded, each rise in
Ca2+ at the oscillator site was followed
by extension of a Ca2+ wave front farther
into the cell. Mitochondrial Ca2+ stores
do not initiate Ca2+ oscillations in these
neurons (Friel, 1995 ), suggesting that the observed oscillator sites
reflected Ca2+ release from ER, rather
than mitochondrial stores. The wave front propagated first around the
cell edges and then radially inward for each peak in the oscillation.
For this cell, final fluorescence in any oscillation was as bright in
the center of the cell as at the periphery. Considering the combined
second, third, and fourth oscillation peaks from each of five cells,
the ratio of radial to circumferential propagation speed was 0.18 ± 0.05 (n = 15; mean ± SEM). For six oscillation
peaks, radial propagation failed entirely (speed = 0); excluding
those, the ratio of radial to circumferential propagation speed was
0.29 ± 0.05 (n = 9). Thus, on average, the
circumferential propagation speed was more than threefold greater than
the radial propagation speed, measured with a uniform intracellular
caffeine concentration. The off-rate of
Ca2+ from fluo-4 [measured for fluo-3 as
424 sec 1 by Lattanzio and Bartschat
(1991) , and 175 sec 1 by Escobar et al.
(1997) ] is likely to be too rapid for any anisotropies in the fluo-4
diffusion pathway to have delayed the radial spread of
Ca2+ to this extent.

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Figure 4.
Patterns of Ca2+ during
caffeine-evoked oscillations. A, Time course of
whole-cell confocal fluorescence in response to continual
microperfusion of 10 mM caffeine. B,
Consecutive confocal images corresponding to the indicated intervals
(A, bars) during the upstroke of each of the first three
peaks in the oscillation cycle. Arrows show initiation
sites of Ca2+ release. Scale bar, 10 µm.
C, Time course of fluorescence at the onset of each
oscillation peak for the whole cell (solid line) and for
the marked subcellular area (dashed line). The interpeak
regions of unchanging fluorescence have been removed to display the
upstroke of each oscillation peak at an expanded time scale; the decay
of fluorescence after each peak is not shown. The y-axis
represents the change in fluorescence with time; minimum fluorescence
values for the unsubtracted whole-cell (12.5) and origin site (10.2)
time courses are subtracted from the displayed time courses. Please see
associated movie displaying the oscillation series in real time in the
electronic version of this paper.
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Molecular correlates of initiation and propagation
Functional measurements presented above show that when discrete
sites of Ca2+ release are observed, they
are always at the cell edges, and that the
Ca2+ wave front propagates faster around
the circumference of the cell than radially inward. To explore a
possible organellar or molecular basis for these observations, living
neurons were stained with fluorescent analogs of ryanodine and
thapsigargin and with MitoTracker to detect intracellular distributions
of RyRs, SERCA pumps, and mitochondria. Figure
5 shows images from the same cell simultaneously labeled with green-emitting MitoTracker (Fig.
5A) and with red-emitting ryanodine (Fig. 5B),
recorded at two different emission wavelengths (see Materials and
Methods). Images of all neurons (Table 1)
taken with labeled ryanodine showed a bright ring around the cell
circumference (Fig. 5B), independent of the length of time
of dye incubation (n = 5). Mitochondria similarly exhibited a ring of brighter fluorescence within all cells (Fig. 5A; n = 7), a wider ring that extended to
the inner margin of the bright ring observed with labeled ryanodine.
Neither marker stained the nucleus (Fig. 5, dark crescent at
top). Autofluorescence was always negligible compared with
fluorescence because of staining for RyRs or mitochondria. Apparently,
the density of RyRs is heavier in the circumference of the cell than in
the interior, and the vast majority of mitochondria are localized in an
inner ring just inside the RyRs. These distributions held when the
entire cell was imaged with a series of confocal sections taken at
incremented focus settings (data not shown). The presence of RyRs at
the cell edge suggests an obvious molecular basis for the initiation of caffeine-evoked Ca2+ release at the cell
edge. Possibly RyRs are only available on the cell edge, or those at
the cell edge have greater sensitivity to caffeine. However, the
non-zero inward radial spread of Ca2+ (via
CICR) suggests functional RyRs throughout the cell. More likely, the
higher RyR density at the edge of the cell increases the likelihood
that a unitary Ca2+ release event through
an RyR at the cell edge will induce Ca2+
release from neighboring RyRs, and so initiate a regenerative wave
front. The distributions of both RyRs and mitochondria might also
explain the slower radial propagation of
Ca2+ wave fronts. A regenerative
Ca2+ wave front would be expected to
travel faster along a path of higher RyR density because
Ca2+ released from one RyR or RyR cluster
has a shorter distance to diffuse to and activate neighboring clusters
than when RyRs are less dense. In addition, mitochondria in these
neurons serve as active Ca2+ stores (Friel
and Tsien, 1994 ; Pivovarova et al., 1999 ); uptake of
Ca2+ into mitochondrial stores would be
expected to buffer the speed of radial, but not circumferential,
Ca2+ propagation.

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Figure 5.
Localization of ryanodine receptors and
mitochondria. Representative cell exposed to both MitoTracker and to a
fluorescent analog of ryanodine. A, Green
emission, corresponding to mitochondria. B,
Red emission, corresponding to ryanodine. Images were
corrected for a small bleed-through of the green
emission into the red channel as described in
Materials and Methods.
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Table 1.
Summary of calcium release and propagation properties for
all cells analyzed and the number of cells from which staining
measurements were made
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Although RyRs were located at the cell perimeter, staining with labeled
ryanodine did not reveal clusters of RyRs that might correspond to the
sites that repeatedly initiated Ca2+
release. Staining with labeled thapsigargin, however, provided a
possible molecular correlate. Thapsigargin binds to (and inhibits the
function of) SERCA pumps, a major mechanism for reuptake of cytoplasmic
Ca2+ into intracellular stores in these
neurons (Cseresnyés et al., 1997 ). Living neurons exposed to a
brief pulse of labeled TG followed by washout of TG showed hot spots at
the cell edges (Fig.
6A,C,E,F), corresponding to spots with a higher density of SERCA pumps. Longer exposures to labeled TG increased emission intensity at the hot spots,
but not at other intracellular areas. Such focal peripheral fluorescence was seen in 11 of 14 cells stained with the fluorescent TG. Autofluorescence was significant compared with TG staining in some
cells (Fig. 6D) but not in others (Fig.
6B). However, the autofluorescence always consisted
of discrete spots in the interior of the cell, clearly different from
the peripheral focal fluorescence seen after staining with fluorescent
TG. The position of the autofluorescent spots changed with time in
these unfixed cells, possibly reflecting movement of intracellular
organelles, thus precluding the ability to correct for autofluorescence
by subtracting the background image. Assuming that the TG-labeled pumps
in the hot spots are functional, a higher density of SERCA pumps might
be expected to result in locally higher
Ca2+ concentrations within the adjoining
intracellular stores for the condition of steady-state pump leak
balance. Higher levels of stored Ca2+ are
known to make RyRs more likely to open in response to a given level of
cytoplasmic Ca2+ (Gyorke and Gyorke, 1998 ;
Koizumi et al., 1999b ). We speculate that a high density of SERCA pumps
results in locally high Ca2+ levels within
the stores, which in turn makes the apposed RyRs more likely to open in
response to caffeine application.

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Figure 6.
Localization of SERCA pumps. Confocal images of
cells exposed briefly to a fluorescent analog of TG (see
Materials and Methods). Pixel values were fit to a linear grayscale.
A, Cell after TG staining. Scaling factor was chosen to
highlight contrast through the entire cell. The arrow
points to an area of especially intense staining that was far offscale
after scaling. Thus, the picture understates the contrast between this
hot spot and the rest of the cell. B, Background
fluorescence of the same cell as A, with the same
scaling. The image was taken before exposure to TG.
C, A different cell after TG exposure. D,
Background fluorescence of the same cell as C, with the
same scaling. The image was taken before exposure to TG.
E, F, two additional cells,
images taken after TG exposure.
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Multiple release initiation sites during
Ca2+ oscillations
In 7 of the 14 cells that oscillated in response to steady
caffeine application, release for each peak after the first initiated from a single site, as in Figure 4. For three cells, the
Ca2+ rise was homogenous over the entire
confocal section, without detectable spatial anisotropy (data not
shown). In four cells, however, oscillation peaks originated from more
than one discrete site; release of Ca2+
was observed from four separate release sites for the cell displayed in
Figure 7 (see Fig. 7, movie).
This cell responded to steady caffeine application with 28 fluorescence
peaks (Fig. 7A). In this cell, the oscillation peaks
initiated from multiple sites simultaneously or from different single
sites, all located at the cell edge. Image series (Fig. 7B)
and fluorescence amplitudes from within four arbitrarily located sites
(Fig. 7C,a-d) for five oscillation peaks with different
patterns of release initiation are shown. The first peak in the
oscillation originated only from a band at the left edge (Fig.
7B, image series 1). For most oscillation peaks,
Ca2+ rose at the different sites within a
few frames of each other or simultaneously, as in the fourth peak
(image series 4). Late in the oscillation cycle,
however, Ca2+ levels at the different
sites increased with time lags of up to 2 sec, reflecting release
initiation from different points. The first
Ca2+ increase (Fig. 7) was near area
c for peak 23, near area d for peak 26, near area
b for peak 27 (image series 23, 26,
and 27), and near area a for peak 28 (see
movie). Ca2+ never increased
first near the 12 o'clock position in this cell, although fluorescence
clearly spread to and through this area without discontinuity for each
peak in the oscillation cycle. Either several different sites along the
cell edge can act as an oscillator site to initiate cell-wide
Ca2+ release, or
Ca2+ propagation from a single,
out-of-focus release site explains the different patterns. Such
propagation would have to be different enough for different peaks
within the oscillation cycle to appear in the recorded optical section,
sometimes as simultaneous release from sites
a-d, and sometimes as release from just one of
each of the four sites in turn.

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Figure 7.
Ca2+ oscillations from a cell
with multiple initiation sites of release. Top, Time
course of fluorescence averaged from within the whole cell confocal
plane in response to continual microperfusion of 10 mM
caffeine. Oscillation peaks 1, 4, 23, 26, and
27 are labeled to correspond to the image series below.
B, Consecutive confocal images from the upstroke of
oscillation peaks 1, 4,
23, 26, and 27. Scale bar,
10 µm. In each peak, fluorescence spread from the initiation site
over the entire cell; the final stages of spread are not shown to
conserve space. Arrows indicate sites of release
initiation for each displayed oscillation peak. The look-up
bar represents pixel values from 0 to 70 for oscillation
peaks 1 and 4, and 0 to 50 for
oscillation peaks 23, 26, and 27.
Image series 23, 26, and 27, where the
fluorescence signal was much dimmer, are smoothed for clarity.
Image series 1 and 4 are unsmoothed.
C, Time course of fluorescence within subareas at the
four different release initiation sites. Left,
Outline of the cell, with boxes a, b, c,
and d arbitrarily placed to reflect the different
initiation sites of Ca2+ release.
Right, Time course of average pixel values within the
boxes of corresponding color for oscillation
peaks 4, 23, 26, and 27. Each tick on the
x-axis represents 0.5 sec; each tick on
the y-axis represents an increase of 2 arbitrary
fluorescence units measured from background-subtracted images (note
different scale for different peaks). Please see associated movie of
the smoothed compacted record of the entire oscillation series, with
the inter-oscillation times cut out to conserve memory, in the
electronic version of this paper.
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It is easy to imagine how regular discharge of a single release
initiation site could produce a regular overall oscillation frequency.
Interestingly, however, in the four cells in which different
oscillation peaks originated from different release initiation sites
(Fig. 7), the oscillation frequency was also regular, with only a
monotonic decline in frequency with time (Cseresnyés et al.,
1999 ). It might have been expected that stochastic release from several
active initiation sites would sometimes produce an overall oscillation
record with irregular interpeak intervals. Moreover, cells with more
functional release initiation sites might oscillate at a higher overall
frequency. Figure 8 shows oscillation
frequency as a function of the number of separate initiation sites for
each oscillating cell with a discrete initiation site of
Ca2+ release. Oscillation frequencies were
comparable with those evoked in intact nerve terminals by 20 Hz firing
(Peng, 1996 ). No correlation was evident between oscillation frequency
and the number of initiation sites. One interpretation is that a wave
front extending throughout the cell via CICR discharges the
Ca2+ stores at all possible release
initiation sites, thereby eliminating the possibility of independent
initiation of two oscillation peaks in close succession from different
release initiation sites.

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Figure 8.
Oscillation frequency as a function of the number
of oscillation initiation sites for each cell. Each point is from a
separate cell. Because the oscillation frequency decreased gradually
during a cycle, frequencies shown are approximate; frequency was
calculated as the number of peaks in the oscillation cycle divided by
the time from the onset of the first peak to the maximum of the last
peak. A site was counted as an initiation site if fluorescence arising
from that site triggered the spread of fluorescence for at least one
peak within the oscillation cycle. For defining the number of
initiation sites per cell, the first peak of the oscillation cycle was
excluded because caffeine likely had not yet reached a uniform
intracellular concentration. The three oscillating cells in which
fluorescence increased without an obvious site of origin are not
included in the graph; these cells oscillated with an average frequency
of 0.27 Hz. No correlation was evident when oscillation frequency was
calculated from only the first five oscillation peaks for each cell,
instead of from the entire oscillation cycle.
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Propagation of the Ca2+ wave front
Spread of the fluorescence wave front was observed to fail not
only in certain intracellular directions, as in Figure 3, but also
across the entire cell. Failures occurring within an oscillating cell
were the most informative because wave fronts that extended successfully throughout the same cell confirmed the presence of dye and
active Ca2+ stores. Such a cell is shown
in Figure 9. For this cell, each oscillation peak after the first originated from a site at ~4 o'clock on the cell edge (Fig. 9C, arrows). From
this site, fluorescence spread over the entire cell for peaks 1-5, 7, and 9 within the oscillation cycle, but failed to extend fully into the
left side of the cell for peaks 6, 8, and 10. The propagation failure
is reflected in the smaller signal for these peaks in the whole cell confocal record (Fig. 9A). Such failures probably underlie
the "small oscillations," that were frequently observed, especially late in an oscillation cycle, in whole-cell studies of caffeine-induced Ca2+ oscillations in these neurons
(Cseresnyés et al., 1999 ). Thus, propagation failure is likely
quite common.

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Figure 9.
Failures of Ca2+ propagation.
A, Time course of average fluorescence from within the
entire cell in response to continual microperfusion of 10 mM caffeine. The jump in baseline fluorescence before the
sixth peak in the oscillation cycle is attributable to
the lowering of the neutral density filter (increased excitation
intensity). The filter was also lowered at the upstroke of the
seventh peak. B, Time course of average
unsubtracted fluorescence within the subcellular areas enclosed by the
left (dotted line) and
right (solid line)
rectangles during the seventh,
eighth, and ninth peaks in the
oscillation cycle. Background and peak fluorescence were slightly
higher in the left rectangle. C,
Consecutive images corresponding to the indicated intervals
(A, bars) of oscillation peaks
2 (top) and 8
(bottom). Arrows mark initiation sites of
fluorescence for each oscillation peak. Scale bar, 10 µm. Because the
images were faint, especially for oscillation
peak 8, images were further scaled after background
subtraction. Pixel values from 0 to 50 were linearly rebinned to fill
the entire eight-bit 0-255 range, and the array was then smoothed.
Color-coding for image series 2 and 8 is
marked by the bar at the end of each image
series.
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Figure 9B shows quantitatively the fluorescence spread over
two arbitrarily defined rectangular areas of this cell for the seventh,
eighth, and ninth oscillation peaks. For the seventh and ninth
oscillation peaks, fluorescence increased first within the right
rectangle (solid line), close to the 4 o'clock
initiation site, then slightly later in the left rectangle
(dashed line). For the eighth peak, however, fluorescence
increased in the right rectangle but stayed at baseline
levels in the left rectangle. Consecutive confocal images from the
eighth oscillation peak illustrate the failure of the wave front to
extend from the initiation site into the left side of the
cell (Fig. 9C). Oscillation peak 6 spread over perhaps
three-fourths of the cell, whereas peaks 8 and 10 propagated
only approximately halfway. The continuous decline in fluorescence
between oscillation peaks in Figs. 7, 9, and 10 probably indicates
continuous photo bleaching of the fluo-4 in these cells during the
prolonged recording time. What caused the propagation failures observed
here? After oscillation peaks 5, 7, and 9, Ca2+ decreased simultaneously in the left
and right sides of the cell. This suggests that the stores on the left
side had indeed reloaded Ca2+ that was
then available for release during peaks 6, 8, and 10. A failure of
stores to release accumulated Ca2+ likely
caused the wave to stop, although other modulations are possible.
Failure of RyRs to open could have been caused by insufficient levels
of either cytoplasmic or lumenal Ca2+
(Gyorke and Gyorke, 1998 ; Koizumi et al., 1999b ).
The observed propagation of the Ca2+ wave
front represents the sum of contributions from passive diffusion of
free Ca2+, diffusion of
Ca2+ complexed with fluo-4 or endogenous
buffers, and propagation attributable to CICR. Presumably caffeine
selectively increases the amount of spread attributable to CICR.
Although pharmacological interventions that inhibit CICR would also
inhibit the initial Ca2+ release, several
points argue that the spread of Ca2+ wave
fronts in the presence of caffeine was almost wholly attributable to
CICR. The propagation failures illustrated in Figure 9, in which the
Ca2+ wave front was stationary for ~1
sec in an area that contained dye and active stores, suggest a minimal
role for diffusion (see also Fig. 10).
Moreover, we observed Ca2+ increases with
similar rise time and peak amplitude at various distances from the
point of initial release (Figs. 1C, 3C,
7C). Passive diffusion would have resulted in increasingly
delayed and decremental increases in free
Ca2+ with increasing distance from the
Ca2+ source.

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Figure 10.
Locally elevated Ca2+ levels
during interpeak periods of an oscillation cycle. A,
Average pixel fluorescence within areas of the cell indicated by
solid and dotted lines
(left) is plotted as a function of time
(right) in response to continual application of 10 mM caffeine. The dotted line corresponds to
the fluorescence of the subarea; the solid line
corresponds to the fluorescence of the rest of the cell. The first 6 of
12 oscillation peaks are displayed. The time course was made from
background-subtracted images. Numbered points indicate
the times of the corresponding confocal image series in
B. B, Consecutive images recorded from
the three points in the time course marked with the corresponding
number onset of the first oscillation peak (1), and the
troughs between the first and second peaks (2), and
third and fourth peaks (3). Pixel values from 0 to 80 for each image
series are grayscale-coded according to the look-up bar
after image series 2. Image series 2 and
3 are smoothed; image series 1 is not
smoothed. Arrows in series 1 at 10, 7, and 2 o'clock mark points at which fluorescence rose without a wave
first propagating to the site. Arrow in image
series 2 indicates a persistent area of locally high
fluorescence. Scale bar, 10 µm.
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Decay of Ca2+ levels
For most cells, the decay of fluorescence after either
depolarization or caffeine application was uniform across the cell (see
movies). Nuclear fluorescence decayed with the same time course as cytoplasmic fluorescence, measured for the cell in Figure 4
(data not shown). Subcellular areas of nonuniform
Ca2+ decay were also recorded, however,
within an oscillating cell (Fig. 10). Average whole-cell confocal
fluorescence was plotted from two areas: a small subarea at the bottom
of the cell (Fig. 10A, dotted line) and
the rest of the cell (solid line). Steady caffeine
application evoked an initial fluorescence increase that decayed to
approximately baseline levels over most of the cell (solid
line). Fluorescence in the subarea, however, decreased more
slowly, held steady for ~1 sec, and then rose again during the second
peak of the oscillation cycle. This persistent fluorescence again
underscores the limited diffusibility of
Ca2+ within these cells; whether the same
Ca2+ ions remained steady in the subarea,
or whether Ca2+ ions were being removed
from and released into this area at the same rate, the elevated
Ca2+ in the subarea did not diffuse into
neighboring areas (Fig. 10B, arrow,
compare image series 2 and 3). After the second
peak in the oscillation cycle, fluorescence decayed within the subarea more slowly than in the rest of the cell, and a still smaller part of
the marked subarea did not return to baseline levels. After each
subsequent oscillation peak, fluorescence within the subarea returned
fully to baseline in register with the rest of the cell, showing that
the persistent fluorescence after the first two peaks was not caused by
a locally high dye concentration.
The subarea of decreased uptake in this cell occurred at one of two
functional release initiation sites. Release sites at 7 and 2 o'clock
are visible in the first oscillation peak as areas of discrete
fluorescence that arose independently of the wave front spreading from
the left side of the cell (Fig. 10B, image series 1, third and fifth frames,
arrows). This cell responded to continual caffeine
application with an oscillation cycle of 12 peaks. After the first
peak, 5 of the 11 subsequent peaks initiated from the 7 o'clock site,
including the second and third peaks. The local area where
Ca2+ did not decay fully after the first
and second peaks in the oscillation cycle was also the site of
initiation of the subsequent (second and third) peaks in the
oscillation cycle, suggesting that continual release from
Ca2+ stores contributed to the persistent
local Ca2+ elevation. Again, this
indicates that intracellular Ca2+ stores
in different areas of the cell receiving the same stimulus need not
necessarily act in concert.
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DISCUSSION |
Data presented here indicate that, although
Ca2+ release from intracellular stores
took place throughout these neurons, discrete sites at the cell edge
were preferentially primed to release Ca2+
throughout a cycle of Ca2+ oscillations.
The corresponding patterns of Ca2+ release
sites and of RyRs and SERCA pumps suggest a structural basis for the
initiation and propagation of Ca2+.
Discrete sites initiate Ca2+ release
The spatially smallest caffeine-evoked
Ca2+ increases detected here, at the start
of the Ca2+ wave fronts (compare Fig.
4), were a few micrometers wide, consistent with the size of
elementary Ca2+ release events in other
cells (Cheng et al., 1993 ; Bootman and Berridge, 1995 ; Tsugorka et al.,
1995 ; Koizumi et al., 1999a ; Lacampagne et al., 1999 ). We infer that
Ca2+ wave fronts that were recorded here
began by release through RyRs, analogous to a spark, that was
then amplified via CICR.
Local Ca2+ signaling has not been obvious
in imaging of Ca2+ oscillations in other
neurons. In developing cortical (Flint et al., 1999 ) and cerebellar
granule (Komuro and Rakic, 1996 ) neurons, the
Ca2+ rise was uniform or somewhat larger
in the cell center than at the edges. The simultaneous rise of
Ca2+ over the entire cell body was also
seen in pioneering studies in frog sympathetic neurons of
Ca2+ oscillations evoked by depolarization
plus caffeine (Lipscombe et al., 1988a ). These oscillations occur at
~10-fold lower frequency than oscillations evoked by caffeine alone
(Lipscombe et al., 1988a ; Friel and Tsien, 1992b ), so the mechanism of
initial release could easily be different from that studied here.
Uniform Ca2+ release across the cell body
might reflect the presence or absence of organellar structures or the
lack of variation in Ca2+ or caffeine
sensitivity among RyRs. Confocal recordings from other neuronal types
should indicate whether release from subareas at the cell edge is a
more general mechanism for initiation of Ca2+ wave fronts in neurons.
How did release always initiate from the cell periphery, even with the
uniform intracellular caffeine concentration (Fig. 2) present during
oscillations? Staining experiments (Fig. 5) suggest that only at the
cell periphery is the density of RyRs high enough for release of
sufficient Ca2+ to activate neighboring
RyRs and initiate a regenerative Ca2+ wave
front. Bullfrog sympathetic neurons have high levels of caffeine-sensitive Ca2+ stores close to
the plasma membrane within sub-surface cisterns (SSCs) of the ER
network (Fujimoto et al., 1980 ). The discrete spots of high SERCA pump
density at the cell periphery (Fig. 6) suggest a possible mechanism for
the formation of these high [Ca2+]
deposits, although we do not know whether the SERCA pump hot spots
correspond to SSCs. Clearly, however, these neurons have distinct
sites, just under the plasma membrane, of preferential release of
Ca2+, of high SERCA pump density, and of
high Ca2+ storage levels (Fujimoto
et al., 1980 ). This implies functional specialization of different
regions apposed to the plasma membrane. It is tempting to speculate
that caffeine-evoked intracellular Ca2+
release is initiated via RyRs from SSCs directly underneath the cell
membrane that have been filled with Ca2+
by locally high levels of SERCA pumps. Many types of neurons have SSCs
(Rosenbluth, 1962 ; Watanabe and Burnstock, 1976 ; Henkart et al., 1978 ;
Berridge, 1998 ) or clusters of RyRs or InsP3Rs
similar to these neurons. In cerebellar neurons, for example, a high
density of InsP3Rs is found in the membranes of
ER cisternal stacks (Satoh et al., 1990 ; Takei et al., 1992 ), and
junctions analogous to the muscle triad have been viewed between
cisternal and plasma membranes in several types of neuron (Henkart et
al., 1976 , Henkart, 1980 ). Ca2+ release
channels seem to be commonly apposed to subareas of the ER; further
work is required to show functional roles for these subareas during
Ca2+ release or oscillations.
If RyRs at the release initiation sites recorded here were indeed
apposed to higher lumenal Ca2+ levels than
others, these RyRs might be gated by lower levels of cytoplasmic
Ca2+, analogous to RyRs in bilayers and
PC12 cells (Gyorke and Gyorke, 1998 ; Koizumi et al., 1999b ), and
thereby initiate the Ca2+ wave front. Some
evidence for differences in sensitivity among RyRs to caffeine (and to
Ca2+) (Rousseau et al., 1988 ; Sitsapesan
and Williams, 1990 ) in these neurons is found in the location of the
initial Ca2+ rise. On the first caffeine
application, RyRs on the right side of the cell responded first in a
few cells (5 of 47; Table 1), even though the right side of the cell
had a lower caffeine concentration (Fig. 2). This suggests differences
in caffeine sensitivity among different release sites; otherwise
initial release would always have been from the left.
Ca2+ stores with different agonist
sensitivities have also been proposed for
InsP3-sensitive stores in nonexcitable cells
(Parker and Yao, 1991 ; Kasai et al., 1993 ; Thorn et al., 1993 ; Bootman
et al., 1994 ), and among RyRs in chromaffin cells (Cheek et al., 1994 ). Higher sensitivity to Ca2+ or caffeine, or
greater capacity of RyRs in our cells, however, could itself be a
by-product of modification of RyRs or other molecules by
phosphorylation, calmodulin, cyclic ADP-ribose, or other
Ca2+-activated signaling pathways. The
location of each Ca2+ release initiation
site at the cell edge also suggests modification by molecules of the
plasma membrane.
Propagation of the Ca2+ wave front
Based on the rise time of fluorescence in subareas at the cell
periphery, Ca2+ release began and ended
within 200 msec, faster than the wave front extended over the entire
cell (Figs. 1C, 3C, 4C,
7C). However, based on the low
Ca2+ diffusibility observed in many cells
(Figs. 3, 9, 10), passive Ca2+ spread in
these neurons appears to be quite low. This suggests that
Ca2+ wave front propagation in these
neurons is best viewed as a sequential series of fast
Ca2+ release events at neighboring sites.
Higher RyR density at the cell periphery may account for faster
circumferential than radial propagation. Although the CICR mechanism
itself requires microdiffusion of Ca2+ for
release from one RyR site to activate release at adjacent RyRs,
elevated Ca2+ levels that were not part of
a propagating wave front (Figs. 9, 10) appeared effectively immobile.
Because, in most cases, and always on initial caffeine application,
Ca2+ propagated without obvious
discontinuity, the RyRs that form Ca2+
release sites may form an almost continuous distribution. Because Ca2+ wave fronts initiate at the same site
(or sites) for each peak in an oscillation cycle, propagation failures
could result in consistent activation of
Ca2+ signaling pathways in only certain
subcellular areas.
Physiological implications
In other cell types, locally nonuniform
Ca2+ levels during
InsP3-dependent Ca2+
oscillations may contribute to exocytosis and fluid secretion or
reflect the sites of hormonal stimulation (Kasai and Augustine, 1990 ;
Rooney et al., 1990 ; Nathanson et al., 1992 ; Toescu et al., 1992 ; Hille
et al., 1994 ; Tse et al., 1997 ). What might be a corresponding functional role for the patterns of Ca2+
release via RyRs described here? Frog neurons receive synapses on the
cell body (Adams et al., 1986 ); a release initiation site adjacent to
the plasma membrane is ideally situated to amplify Ca2+ influx through the plasma membrane
into a propagating Ca2+ wave front. Such
amplification would turn a local Ca2+
increase into a Ca2+ increase as far as
the Ca2+ wave front propagated. We further
speculate that modulation of Ca2+ influx
across the plasma membrane, or of RyR Ca2+
sensitivity, at just the release initiation site could be a method for
local modulation to affect cell-wide Ca2+
levels. Although Ca2+ influx without
additional RyR agonists induces CICR in these and other neurons (Friel
and Tsien, 1992a ; Hua et al., 1993 , 1994 ; Llano et al., 1994 ; Shmigol
et al., 1995 ; Peng, 1996 ; Usachev and Thayer, 1997 ) (but see Cohen et
al., 1997 ), CICR is more likely when RyRs have been sensitized to
cytoplasmic Ca2+. A physiological analog
of caffeine is not firmly established, although increased levels of
cyclic ADP-ribose or activity of kinases or calmodulin have been
proposed to play this role (Hua et al., 1994 ; Lee et al., 1994 ).
Weakening of cytoplasmic Ca2+ buffering
might be even more effective than sensitization of the RyRs for
triggering CICR. In several cell types, only ~1% of cytoplasmic
Ca2+ is free (Hille et al., 1994 ); even a
modest decrease in cytoplasmic buffering efficacy could dramatically
increase the free Ca2+ available to
initiate CICR.
In conclusion, high-speed imaging has revealed a potential organellar
basis for subcellular Ca2+ signaling and
Ca2+ wave front propagation in these
neurons. It will be interesting to see whether similar mechanisms
initiate or mediate Ca2+ oscillations
during neuronal migration or other physiological processes.
 |
FOOTNOTES |
Received March 16, 2000; revised Sept. 1, 2000; accepted Sept. 11, 2000.
This work was supported by National Institutes of Health (NIH) Grant
RO1 NS33578 to M.F.S. and by NIH individual National Research
Service Award NS10689 to S.I.M. We thank Dr. Christopher W. Ward for
programming advice and helpful discussions.
Correspondence should be addressed to Dr. Martin Schneider, Department
of Biochemistry and Molecular Biology, University of Maryland Medical
School, 108 N. Greene Street, Baltimore, MD 21201. E-mail:
mschneid{at}umaryland.edu.
Dr. McDonough's present address: Marine Biological Laboratory, 7 MBL
Street, Woods Hole, MA 02543.
 |
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M. Patterson, J. Sneyd, and D. D. Friel
Depolarization-induced Calcium Responses in Sympathetic Neurons: Relative Contributions from Ca2+ Entry, Extrusion, ER/Mitochondrial Ca2+ Uptake and Release, and Ca2+ Buffering
J. Gen. Physiol.,
January 1, 2007;
129(1):
29 - 56.
[Abstract]
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M. D. Bootman, D. R. Higazi, S. Coombes, and H. L. Roderick
Calcium signalling during excitation-contraction coupling in mammalian atrial myocytes.
J. Cell Sci.,
October 1, 2006;
119(Pt 19):
3915 - 3925.
[Abstract]
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[PDF]
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K. Ouyang, H. Zheng, X. Qin, C. Zhang, D. Yang, X. Wang, C. Wu, Z. Zhou, and H. Cheng
Ca2+ sparks and secretion in dorsal root ganglion neurons
PNAS,
August 23, 2005;
102(34):
12259 - 12264.
[Abstract]
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A. Verkhratsky
Physiology and Pathophysiology of the Calcium Store in the Endoplasmic Reticulum of Neurons
Physiol Rev,
January 1, 2005;
85(1):
201 - 279.
[Abstract]
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[PDF]
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R. Nitsch, E. E. Pohl, A. Smorodchenko, C. Infante-Duarte, O. Aktas, and F. Zipp
Direct Impact of T Cells on Neurons Revealed by Two-Photon Microscopy in Living Brain Tissue
J. Neurosci.,
March 10, 2004;
24(10):
2458 - 2464.
[Abstract]
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N Wanaverbecq, S J Marsh, M Al-Qatari, and D A Brown
The plasma membrane calcium-ATPase as a major mechanism for intracellular calcium regulation in neurones from the rat superior cervical ganglion
J. Physiol.,
July 1, 2003;
550(1):
83 - 101.
[Abstract]
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D. Rossi, I. Simeoni, M. Micheli, M. Bootman, P. Lipp, P. D. Allen, and V. Sorrentino
RyR1 and RyR3 isoforms provide distinct intracellular Ca2+ signals in HEK 293 cells
J. Cell Sci.,
June 15, 2002;
115(12):
2497 - 2504.
[Abstract]
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J. Hongpaisan, N. B. Pivovarova, S. L. Colegrove, R. D. Leapman, D. D. Friel, and S. B. Andrews
Multiple Modes of Calcium-Induced Calcium Release in Sympathetic Neurons II: A [Ca2+]i- and Location-Dependent Transition from Endoplasmic Reticulum Ca Accumulation to Net Ca Release
J. Gen. Physiol.,
July 1, 2001;
118(1):
101 - 112.
[Abstract]
[Full Text]
[PDF]
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J. S. Marchant, V. Ramos, and I. Parker
Structural and functional relationships between Ca2+ puffs and mitochondria in Xenopus oocytes
Am J Physiol Cell Physiol,
June 1, 2002;
282(6):
C1374 - C1386.
[Abstract]
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