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Vol. 13, Issue 4, 1263-1273, April 2002
and
*Division of Biology, School of Arts and Sciences,
University of Tokyo, Tokyo, 153-8902; and
Department of
Cell Biology, National Institute for Basic Biology, Okazaki, 444-8585, Japan
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ABSTRACT |
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It has been proposed that a localized calcium (Ca) signal at the growing end of the cleavage furrow triggers cleavage furrow formation in large eggs. We have examined the possible role of a Ca signal in cleavage furrow formation in the Xenopus laevis egg during the first cleavage. We were able to detect two kinds of Ca waves along the cleavage furrow. However, the Ca waves appeared after cleavage furrow formation in late stages of the first cleavage. In addition, cleavage was not affected by injection of dibromoBAPTA or EGTA into the eggs at a concentration sufficient to suppress the Ca waves. Furthermore, even smaller classes of Ca release such as Ca puffs and Ca blips do not occur at the growing end of the cleavage furrow. These observations demonstrate that localized Ca signals in the cleavage furrow are not involved in cytokinesis. The two Ca waves have unique characteristics. The first wave propagates only in the region of newly inserted membrane along the cleavage furrow. On the other hand, the second wave propagates along the border of new and old membranes, suggesting that this wave might be involved in adhesion between two blastomeres.
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INTRODUCTION |
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During cytokinesis of animal cells, the
contractile ring, a band consisting of bundles of F-actin and myosin,
is formed at the equator of the cell (Schroeder, 1975
; Mabuchi and
Okuno, 1977
). In large eggs that undergo unilateral cleavage, it has
been proposed that localized elevation of cytosolic free calcium (Ca)
ions ([Ca2+]i) at the growing end of the
cleavage furrow triggers cleavage furrow formation by the activation of
myosin ATPase activity through the myosin light-chain kinase (MLCK;
Fluck et al., 1991
; Miller et al., 1993
; Chang
and Meng, 1995
; Webb et al., 1998
), as in the case of smooth
muscle (Scholey et al., 1980
). However, data regarding the
relevance of Ca waves in cleavage furrow formation are contradictory or
incomplete. In fish eggs, it has been suggested that cleavage furrow
formation is accompanied by a localized Ca wave that propagates in the
subcortical layer along the growing end of the cleavage furrow (Fluck
et al., 1991
; Chang and Meng, 1995
; Webb et al.,
1998
). However, in these studies, the exact positions of the furrow
ends were not identified simultaneously with observation of Ca waves.
In Xenopus eggs, buffering the
[Ca2+]i with
1,2-bis(o-aminophenoxy)ethane-N,N,N',N'-tetraacetic
acid (BAPTA)-type Ca buffers has been shown to inhibit cleavage furrow formation and also destroy already formed contractile rings (Miller et al., 1993
). Although Ca signals during cleavage of
dividing cultured cells and sea urchin eggs have been reported
(Poenie et al., 1985
; Tombs and Borisy, 1989
; Kao
et al., 1990
; Groigno and Whitaker, 1998
), the functional
role of the signal has not been determined. Timings of the signal
appearances are varied during cleavage. They are not restricted to the
furrow formation period and sometimes occur even after cytokinesis
(Tombs and Borisy, 1989
). Thus, the involvement of Ca waves in
cytokinesis remains uncertain.
Another mechanism has been proposed to mediate signaling for cleavage
furrow formation. The small GTPase Rho has been shown to play a key
role in furrow signaling (Kishi et al., 1993
; Mabuchi et al., 1993
; Drechsel et al., 1996
). Moreover,
it has been suggested that the Rho and cdc42 pathway might regulate
myosin II ATPase activity through target proteins (Uehata et
al., 1997
; Kawano et al., 1999
). Such a mechanism for
cleavage furrow formation would not require Ca waves. Therefore, we
wanted to establish whether such a wave could be detected.
In previous experiments using Xenopus eggs, Muto and
colleagues (1996)
suggested that a Ca wave along the cleavage furrow initiates after cleavage furrow formation begins. However, in the
report, the fertilization membranes were not removed, and the eggs were
observed from the vegetal hemisphere. In this configuration, the
growing ends of the cleavage furrow are inside the cleft between the
two blastomeres and covered with the fertilization membrane, making
clear observation difficult. To overcome these disadvantages, we
removed the fertilization membrane and labeled the egg surface with
rhodamine-wheat germ agglutinin (WGA) to visualize the growing ends
of the early cleavage furrow (Noguchi and Mabuchi, 2001
). We imaged
wave type Ca signals with Calcium Green-1 dextran (CalG-dx) from the
animal hemisphere of the egg. In addition to the Ca wave, which is the
orchestrated Ca release from a global area of the cell (Marchant
et al., 1999
), smaller classes of Ca signal have been
described. These are Ca puffs, which are thought to be Ca release from
10-30 coordinately opened Ca channels, and Ca blips, which are Ca
released from single open Ca channels (Parker et al., 1996
;
Bootman et al., 1997
; Sun et al., 1998
; Marchant
et al., 1999
). These signals were also examined during
cleavage furrow formation. Furthermore, we manipulated
[Ca2+]i in the egg, and the effects on
cytokinesis were examined with simultaneous monitoring of
[Ca2+]i.
Our observation and characterization of Ca waves revealed that two waves have distinct characteristics that would provide a new insight for the mechanism of propagation of wave type Ca signal and its role in embryogenesis during cleavage stage.
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MATERIALS AND METHODS |
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Handling of Animals and Eggs
Females of albino Xenopus laevis were induced to
ovulate by injection of 400 U of human chorionic gonadotropin (Denka
Seiyaku, Tokyo, Japan) a day before use. The eggs were inseminated and cultured as described previously (Noguchi and Mabuchi, 2001
).
Preparation of Fluorescently Labeled Dextran
To prepare the volume indicator for dual imaging, 5-(and 6-)-carboxynaphthofluorescein succinimidyl ester (CNF; Molecular Probes, Inc., Eugene, OR) was conjugated to amino dextran of 10,000 MW (Molecular Probes, Inc.), for 1 h at room temperature in reaction buffer (10 mM HEPES, pH 7.5) at 9:1 molar ratio of dye and amino dextran. The reaction was stopped by addition of stop solution (50 mM Tris-HCl, 10 mM K-glutamate). Uncoupled dye was removed by centrifugation at 10,000 × g and Sephadex G-25 gel filtration.
Imaging for Ca Wave
The vitelline membrane of the fertilized egg was manually removed. The volume of injectant was determined by measuring the diameter of the droplets injected into a salad oil droplet. The fluorescent indicators were introduced within 30 min after fertilization. For imaging [Ca2+]i, 10 nl of a solution of 0.5 mM calcium Green 1-dextran 10,000 MW (CalG-dx; Molecular Probes, Inc.) and 0.5 mM rhodamine-dextran (Rhod-dx; Molecular Probes, Inc.) was injected. In case of simultaneous imaging of the cortex and [Ca2+]i, 10 nl of a solution of 0.33 mM CalG-dx and 0.67 mM CNF-dx were injected. Then, the cell surface was labeled with 2.5 µg/ml rhodamine-WGA (Vector Laboratories, Burlingame, CA) for 5 min, just before cleavage was initiated. This staining enabled us to monitor cleavage furrow progression without affecting furrow formation.
Time-lapse imaging of [Ca2+]i was carried
out under a confocal laser scanning microscope (LSM; Zeiss LSM510, Carl
Zeiss, Iena, Germany), equipped with a 5× Fluar lens (see
Figure 1). CalG-dx was excited at 488 nm using an Argon laser line, and
emitted fluorescence was collected through a 505-550 nm bandpass
filter. Rhodamine dye was excited at 543 nm using a He-Ne laser
line, and fluorescence was collected through a 560-615 nm bandpass
filter. CNF dye was excited at 633 nm using a He-Ne laser line, and the
fluorescence was collected through a 650 nm longpass filter. Each
fluorescent dye was excited sequentially. Before recording, detection
gains of the photomultipliers were set to make fluorescence
intensities of the images of CalG-dx and that of volume indicator
(Rhod-dx or CNF-dx) to be equal at the resting level. The data were
processed with LSM 510 software for further analysis. Increase of
fluorescent intensity is calculated as FCalG
Fvolume indicator (Rhod or CNF).
Microinjection of Ca Chelator during Ca Wave Imaging
Imaging of [Ca2+]i was started as described above and then paused right after the first cleavage was initiated. The LSM was switched to the bright field microscopy mode, and the Ca buffer was injected from the perpendicular position to the division plane. Then the LSM was switched back to the LSM mode, and the time-lapse recording was restarted. In the injection experiments, eggs from more than three individual female frogs were used.
Imaging of Ca Puffs and Ca Blips
Ten nanoliters of 2 mM Fluo-4 (Molecular Probes, Inc.) was
injected into an albino egg within 30 min after fertilization. The
growing ends of the cleavage furrow were visualized by
rhodamine-WGA staining as described above. The egg was settled in a
handmade chamber designed for scanning the subcortical layer of the
Xenopus egg and compressed by a coverslip in order to
flatten the cortex (see Figure 1). In this chamber cleavage occurred
normally. Images of the growing end of the cleavage furrow and the
[Ca2+]i were recorded sequentially using the
LSM equipped with a 63× Plan-apochromat oil immersion lens (Zeiss).
The subcortical layer a few micrometers deep from the cell surface was
scanned. The thickness of the optical section was set at 3 µm. To
investigate the Ca dynamics in Ca puffs and Ca blips, serial linescans
in a fixed line position were performed. In Figure 3, in order to examine dynamics of the Ca in Ca puffs and Ca blips, increase of
fluorescent intensity was calculated as Fincrease = F
Frest. Frest was recorded
in the same position of the egg just before the Ca puff or the Ca blip.
In Figure 4, increase of fluorescent intensity was calculated as
Fincrease = Fn
Fn
1. Fluo-4 was compartmentalized in
small vesicles in subcortical layer in the egg and made bright spots in
the image. The vesicles move slowly depending on the contraction of the
cleavage furrow. To minimize the noise, we subtracted the next frame.
Most of the signal from the vesicles are subtracted by the same
vesicle in the next frame. Although relatively large noise is left in
the images, the real events are distinguishable from noise because an
event is a spark in one frame that disappears in the next frame, but
the noise exists continuously and moves gradually. Therefore, real
events were defined as signals that appeared in a single frame and had
a diameter of >1.5 µm.
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RESULTS |
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Ca Waves Do Not Associate with the Growing End of the Cleavage Furrow
To detect any Ca signals that may propagate along the cleavage
furrow, the cleavage furrow was visualized by staining with a low
concentration of rhodamine-WGA. We have previously demonstrated that WGA-binding sites colocalize with F-actin and myosin in the furrow
region (Figure 1A; Noguchi and Mabuchi,
2001
). Figure 1 shows two types of Ca imaging system we used: one for
Ca waves and the other for Ca blips and Ca puffs. To detect changes of [Ca2+]i by possible Ca wave, we injected the
eggs with a Ca indicator CalG-dx. The cleavage furrow and
[Ca2+]i were simultaneously monitored from the
animal hemisphere of the egg, by time-lapse recording using an LSM
(Figure 1B). Recordings were begun 5-10 min before cleavage
initiation, and images were taken every 30 s for 20 min. This time
period is long enough to monitor the advancement of the cleavage furrow
from the animal pole to the vegetal hemisphere. However, no Ca wave was
observed at the growing end of the cleavage furrow in any of the 200 eggs examined (Figure 2). Our
inability to detect Ca waves at the cleavage furrow could not be
explained by insensitivity of the imaging system or other technical
problem, because this experimental system could properly detect other
wave-type Ca signals (see below). Therefore, we conclude that no Ca
wave accompanies cleavage furrow formation in Xenopus eggs.
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Neither Ca Puffs nor Ca Blips Occur at the Growing End of the Cleavage Furrow
It remained possible that Ca signals occurred but were much
smaller in size than could be detected using the system for wave type
Ca signal. Therefore, we next asked whether smaller Ca signals such as
Ca puffs and/or Ca blips might take place at the growing end of the
cleavage furrow. We used a highly sensitive fluorescent Ca indicator,
Fluo-4 (Haugland, 1999
; Thomas et al., 2000
), and the
subcortical layer of the egg was scanned at a high speed and at a
higher magnification (Figure 1C). To demonstrate that this system is
sensitive enough to detect these small Ca releases, Ca puffs and blips
were induced by injection of a poorly metabolizable derivative of
InsP3, 3FIP3 (D-myo-inositol
1,4,5-triphosphate, 3-deoxy-3-fluoro-, hexasodium salt; Calbiochem, San
Diego, CA), as described previously (Parker et al.,
1996
). The subcortical layer was subsequently scanned to reveal the Ca
dynamics (See MATERIALS AND METHODS). Serial line scans (3 ms/one line
scan; Figure 3) were performed to measure
the temporal change of fluorescent intensity and the diameter of
half-maximum intensity of the signal, respectively (Figure 3). This
revealed that there were two classes of Ca signals based on their
signal properties. The duration and the diameter of half-maximum
intensity of Ca puff were 150-500 ms and 4.3 ± 0.65 µm,
respectively, and those of Ca blips were <100 ms and 1.8 ± 0.45 µm, respectively. These data fit well with previously reported values
(Sun et al., 1998
). Therefore, this system is sensitive
enough to detect both Ca puffs and Ca blips. Using this system, we
performed scanning of the subcortical layer around the growing end of
the cleavage furrow. We imaged each growing end. Total time for 30 scans is 23.4 s at a rate of 0.78 s/frame. In this time period,
the cleavage furrow advances ~50 µm. Therefore, any localized and
concentrated Ca signal should be detected. We plotted the position of
Ca signals to reveal the distribution of Ca releasing site. At the
growing end of the cleavage furrow, almost no microspikes were detected
in any of the eggs examined. (0-3 signals/egg, n = 15; Figure
4). However, in all of these eggs,
numerous Ca blips and Ca puffs were seen after microinjection of 3FIP3
(30-60 signals/egg). This indicates that there was no Ca microspike
occurring at the growing end of the cleavage furrow. Moreover, the
plotting of Ca signal after 3FIP3 injection revealed that although Ca
releasing sites are present around the growing end of the cleavage
furrow, they are not noticeably concentrated there. Furthermore, there
was no Ca microspike in the region of the contractile ring itself (0-2
signals in 9 eggs examined; our unpublished data). Combined with the
results of the Ca wave imaging, we conclude that no localized Ca signal
accompanies the propagating furrow end during the first cleavage in
Xenopus eggs.
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A Ca Wave that Propagates within the New Membrane Region Is Detectable
Despite the fact that we did not detect a Ca wave at the growing
end of the cleavage furrow, we were able to detect other Ca waves using
the CalG-dx system (Figures 5 and
6). One type of Ca wave (wave 1) appeared
a few minutes after membrane insertion started in the furrow region,
namely, ~10 min after furrow emergence at the animal pole, and lasted
for 5 min. Wave 1 showed some remarkable characteristics. It traversed
only the region of newly inserted membranes but never propagated into
the old membrane region (Figure 5C). The timing of its initiation
corresponded to that of the furrow deepening. Therefore, wave 1 is
likely to be the counterpart of the furrow deepening wave that has been
observed in zebrafish eggs (Chang and Meng, 1995
; Webb et
al., 1998
). However, its duration was short (~5 min), it did not
propagate into the vegetal hemisphere, and it was not seen in the
contractile ring region (Figure 5B). These results strongly suggest
that wave 1 is involved neither in the cleavage furrow formation nor in
the contraction of the contractile ring. The speed of propagation of
wave 1 was 1.66 ± 0.46 µm/s (n = 9), as measured by
tracing the wave front. Thus, it is categorized as a slow Ca wave,
which has been reported in some cell types (Fluck et al.,
1991
; Muto et al., 1996
; Jaffé and Créton, 1998
;
Webb et al., 1998
).
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A Second Ca Wave Traverses along the Border of Old and New Membrane Region after Cytokinesis
A second Ca wave (wave 2) appeared after completion of the
first cleavage, that is, 20-25 min after cleavage initiated (Figure 6). Thus, the time of wave 2 indicates it cannot be involved in cytokinesis. Interestingly, wave 2 was distinct from wave 1. It began
mostly at the animal pole and traversed along the border of the old and
the new membrane regions. It did not propagate continuously but showed
a skipping and/or flickering manner of movement, but still moved only
along the border. Based on these features, it is likely that wave 2 corresponds to the Ca wave previously observed along the cleavage
furrow in Xenopus eggs (Muto et al., 1996
). The
speed of wave 2 was measured during periods when it propagated without
skipping. Its speed was 1.66 ± 0.45 µm/s (n = 12),
suggesting that it also belongs to the slow Ca wave class. The
characteristics and time periods of wave 1 and wave 2 are summarized in
Figure 7.
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Suppression of Both Wave 1 and Wave 2 by Ca Chelators Did Not Inhibit Cytokinesis
The two Ca waves that were detected along the cleavage
furrow are not likely to play a role in cytokinesis because of their distribution and the timing of their appearances. To further confirm that these two Ca waves are not involved in cytokinesis, we suppressed the waves by microinjecting two types of Ca chelators into dividing eggs. We monitored [Ca2+]i and the effects on
cytokinesis simultaneously (Figure 8).
The results are summarized in Table 1.
EGTA at an intracellular concentration of 0.9 mM effectively lowered
the [Ca2+]i and suppressed both waves 1 and 2 without affecting either the first or second cleavages. Injection of
dibromoBAPTA at the same concentration also clearly suppressed both
waves although the extent of decrease in the
[Ca2+]i was little lower than that of EGTA. The
first cleavage continued and was accomplished normally. These results
strongly suggest that the two Ca waves along the cleavage furrow are
not involved in cytokinesis. In dibromoBAPTA injected eggs, the second
cleavage occurred normally in the blastomere on the noninjected side,
while it was inhibited in the blastomere on the injected side. In the control, neither the Ca wave nor cytokinesis was inhibited.
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dibromoBAPTA Induces Aberrant and Irreversible Cortical Contraction of the Xenopus Egg
dibromoBAPTA was previously shown to inhibit furrow formation at
the growing end (Miller et al., 1993
). However, our data suggest that this effect is not due to change in
[Ca2+]i. To investigate this inhibitor, we
reexamined the effect of dibromoBAPTA on furrow formation. We injected
various concentrations of dibromoBAPTA near one growing end of a furrow
(Figure 9). On the side of the injection,
the furrow formation was clearly inhibited in a dose-dependent manner
as described previously, although it progressed normally at the other
end. Combined with the result shown in Figure 8, it seems that
dibromoBAPTA injection affected furrow formation only when it was
injected near the growing end. This is the case even if the
concentration is high enough for suppressing Ca waves (Figure 9).
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We found that aberrant cortical contraction was induced by injection of dibromoBAPTA, which led to deformation of the egg around the injection site (Figure 9, e-f'). Contraction was recognized at final concentrations from 0.45 to 3.6 mM. The deformation was irreversible for at least 6 h (n = 12 at 1.8 mM). It was also detected in the experiment shown in Figure 8. In contrast, EGTA did not show any effect on both the cortex and the furrow formation even when it was injected at concentrations up to 6.3 mM. These observations suggest that the effect of dibromoBAPTA on cleavage furrow progression is not due to its Ca-chelating ability.
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DISCUSSION |
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Ca Signal Is Not Involved in the Furrow Formation at the Growing End of the Cleavage Furrow
Recent studies have suggested that the Ca blip is the smallest
unit of Ca release in vivo (Parker et al., 1996
; Bootman
et al., 1997
; Sun et al., 1998
). We
demonstrated that our experimental system for Ca imaging is sensitive
enough for detecting Ca puffs and Ca blips and that these small Ca
signals do not accompany cleavage furrow formation. Furthermore,
suppression of the Ca waves along the cleavage furrow by lowering the
[Ca2+]i did not affect the progression of the
cleavage furrow. Therefore, at least in Xenopus eggs, a Ca
signal is not directly involved in the formation of the contractile
ring. There has been a speculation that free Ca ions might be relevant
to the contractile ring formation by the following mechanism: 1)
[Ca2+]i increases and Ca ions bind to
calmodulin, 2) Ca calmodulin activates myosin light-chain kinase, 3)
myosin light-chain kinase phosphorylates myosin regulatory light chain
at the activation sites, and 4) the phosphorylated myosin somehow
contributes to contractile ring formation (Matsumura et al.,
1998
). However, the present results indicate that in Xenopus
eggs, Ca increase does not occur during formation of the contractile
ring at the growing end of the cleavage furrow. Our results do not
exclude the possibility that the amount of phosphorylated myosin may
increase somewhere other than the cleavage furrow region by this
mechanism (Mabuchi and Takano-Ohmuro, 1990
; Satterwhite et
al., 1992
), because we could not see deep inside of the whole
Xenopus egg. Then the phosphorylated myosin could be
recruited to the cleavage furrow region. Alternatively, myosin might
already be phosphorylated before or during mitosis. However, double
staining with antibodies against phosphorylated myosin light chain and
myosin heavy chain in dividing cultured cells (Matsumura et
al., 1998
) has shown that phosphorylation and assembly of myosin
occur in close temporal proximity. In addition, biochemical experiments
have been shown that myosin II is kept in an inactive state during
mitosis and activated through phosphorylation after the end of mitosis
in Xenopus eggs and cultured cells (Satterwhite et
al., 1992
; Yamakita et al., 1994
). Because our
data suggest that Ca ions are not directly involved in the cleavage
signaling process, the alternate mechanism of myosin activation through
the low-molecular-weight GTPase Rho is more likely to be involved in
cleavage signaling (Kishi et al., 1993
; Mabuchi et
al., 1993
). The pathway containing rho does not utilize free Ca
ions as an activator.
Two Ca Waves along the Cleavage Furrow Are Not Involved in Cytokinesis
We also demonstrated that the two Ca waves detected along the
cleavage furrow during the first cleavage are not required for cytokinesis of Xenopus eggs by two observations: 1) the Ca
waves are not seen at the proper time and place. The observed waves were seen after formation and contraction of the contractile ring and
even after new membranes were added in the cleavage furrow. Moreover,
these waves were observed in a region of the egg spatially separated
from the contractile ring. 2) Suppressing the two Ca waves with an
appropriate concentration (0.9 mM) of dibromoBAPTA or EGTA did not
affect cleavage. In a previous report (Miller et al., 1993
),
it was shown that injection of dibromoBAPTA inhibits furrow formation
more effectively than EGTA. To account for the differences of their
inhibitory activities, a "shuttle buffer model" was proposed. In
this model, dibromoBAPTA, which has a Kd for Ca (0.15 µM) close to the
[Ca2+]i of a Xenopus egg (0.3 µM),
would bind to a Ca ion in an area of high
[Ca2+]i and then release it immediately after
diffusing to an area of low [Ca2+]i, becoming
active again. On the other hand, EGTA, which has a
Kd for Ca ion of 0.01 µM, would not
release the Ca ion once bound. Thus, dibromoBAPTA is proposed to lower
the [Ca2+]i more smoothly than does EGTA
(Speksnuder et al., 1989
; Miller et al., 1993
;
Webb et al., 1998
). However, our imaging data suggest that
this is not the case. In fact, EGTA suppressed the Ca waves more
effectively than dibromoBAPTA. In addition, it is reported in cultured
astrocytes that EGTA suppresses the wave type Ca signals more
effectively than dibromoBAPTA (Wang et al., 1997
). Moreover, the concentration required to suppress the Ca waves, which was 0.9 mM
when injected away from the furrow ends (position 1), was lower than
the concentration that inhibits cytokinesis, which was 1.8 mM when
injected at the same position (our unpublished data). This may support
the idea that the inhibitory activity of dibromoBAPTA on cytokinesis is
not due to suppression of the Ca signal itself.
Why Does dibromoBAPTA Inhibit Furrow Formation?
We found that there was no Ca signal at the growing end as mentioned above. In addition, suppression of Ca waves by injection of Ca buffers did not affect cytokinesis. Therefore, we reexamined the dose dependency of the inhibition of furrow formation by dibromoBAPTA. Furrow formation was inhibited in dose-dependent manner; however, it is most likely that this effect is a side effect of dibromoBAPTA based on two reasons: 1) We found that the cortical region where dibromoBAPTA was injected may be structurally damaged: aberrant cortical contraction was induced and the region was deformed. This may not be induced by reducing the [Ca2+]i near the injection site because EGTA did not show any such effect. This cortical damage did not seem to be reversible, because the second division in the blastomere in the side of injection did not take place (Table 1). In addition, we found that once the cortex was damaged and deformed, it did not recover for at least 6 h after injection. 2) The inhibition took place only if dibromoBAPTA was injected near the furrow end. dibromoBAPTA inhibited furrow formation at low concentration (0.23-0.9 mM) on the side of injection, and the furrow progressed normally at the other growing end (Figure 9). When 0.9 mM dibromoBAPTA was injected at position 1 away from both ends of the cleavage furrow, the Ca wave was suppressed completely, but the egg cleaved normally (Figure 8 and Table 1).
Therefore, even at low concentration, the cortical damage by dibromoBAPTA might inhibit furrow formation if dibromoBAPTA were injected near the growing end.
Mechanism and Role of Propagation of Wave 1 and Wave 2
We demonstrated that wave 1 and wave 2 are categorized as slow Ca
waves on the basis of the speed of propagation. Despite the fact that
the two waves are both slow Ca waves, these two waves were markedly
different from one another in location and character of propagation.
The mechanism of propagation of slow Ca waves has not yet been
determined, although it is suggested that IP3 is involved in Ca release
(Muto et al., 1996
; Webb et al., 1998
).
Wave 1 propagates only within the new membrane region. The reason for this is not clear. However, one hypothesis is that just after its formation, the new membrane is immature compared with the old membrane, and the content of phospholipids might be different between the two membranes. This is the first report that Ca waves selectively propagate in different areas of the cell because of differences in the membrane.
In contrast, wave 2 propagates along the border of the old and the new
membrane regions. It is known that tight junctions are formed between
the two blastomeres along this region after the first cleavage is
accomplished (Merzdorf et al., 1998
). Moreover, [Ca2+]i rises during tight junction
formation in tissue culture cells (Nigam et al., 1992
).
Therefore, wave 2 might be involved in tight junction formation between
the blastomeres to seal up the embryo body. Another interesting aspect
of this data is that along the border of the old and new membrane
region, several initiation sites of Ca waves are formed in a short
period at the end of the first cleavage. The distinct timing and
orientation of these waves lead us to speculate that slow Ca wave
propagation may involve distinct pathways for IP3 production in
particular positions of the cell.
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ACKNOWLEDGMENTS |
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We thank Dr. Andrew Miller for advice on this project and Dr. K. Miller, Dr. D. Frank, Dr. R. Hoppman, and Mr. A. Rogat for critical reading of the manuscript. This work was supported by research grants from the Ministry of Education, Culture, and Science in Japan (10213202 and 1249008). T.N. was supported by a predoctoral fellowship from the Japan Society for the Promotion of Science for Young (Doctoral) Scientists.
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FOOTNOTES |
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Corresponding author. E-mail address:
noguchi{at}biology2.wustl.edu.
DOI: 10.1091/mbc.01-10-0501.
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REFERENCES |
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