Abstract
Ca2+ waves and oscillation are key signalling elements during the fertilization process of animals, and are involved, for example, in egg activation. In the unique double fertilization process in flowering plants, both the egg cell and the neighbouring central cell fuse with a sperm cell each. Here we succeeded in imaging cytosolic Ca2+ in these two cells, and in the two synergid cells that accompany the gametes during semi-in vivo double fertilization. Following pollen tube discharge and plasmogamy, the egg and central cells displayed transient Ca2+ spikes, but not oscillations. Only the events in the egg cell correlated with the plasmogamy. In contrast, the synergid cells displayed Ca2+ oscillations on pollen tube arrival. The two synergid cells showed distinct Ca2+ dynamics depending on their respective roles in tube reception. These Ca2+ dynamics in the female gametophyte seem to represent highly specific signatures that coordinate successful double fertilization in the flowering plants.
Intracellular calcium waves are key signalling elements during the fertilization process of animals, involved in egg activation. Here the authors image calcium oscillations during the fertilization process in flowering plants, revealing specific signatures involved in the success of this process.
Ca2+ is important as an intracellular second messenger in the fertilization of many organisms1,2,3. In animals including mouse, xenopus, ascidian, starfish and sea urchin, various patterns of cytosolic Ca2+ waves and oscillations are involved in fertilization and the subsequent onset of embryogenesis3,4. In flowering plants, the egg is intimately associated with typically six to eight other haploid cells forming the female gametophyte. These include the central cell representing the second female gamete and two synergid cells that produce the signals, which guide the male gametophyte, or pollen tube, towards the ovule. The pollen tube delivers two non-motile sperm cells whose release occurs by bursting, which in turn is triggered when the tube interacts with the synergid cells5. The receptive synergid cell degenerates following this interaction, whereas the other synergid cell persists. After their ejection from the pollen tube, the two sperm cells stay immobile between the two female gametes for several minutes and subsequently fuse with the egg and central cells, respectively6. These two fusion events give rise to the embryo and to the endosperm, respectively, and the process is therefore termed double fertilization.
Since the entire fertilization process takes place within the ovule, characterization of Ca2+ dynamics in the egg cell in situ and in the accompanying gametophytic cells has been elusive in plants. Previously, in vitro fertilization of isolated egg cells7,8,9 has shown Ca2+ influx in the vicinity of the sperm entry site and waves of Ca2+ influx were observed to spread through the whole egg cell plasma membrane10,11. This Ca2+ influx may trigger egg activation, which includes cell wall formation and vacuole fragmentation12. The coordination of this process in vivo is likely to require intimate cell-to-cell communication between the gametophytic cells13. Assessing the complete picture of the signalling processes therefore requires the presence of the other gametophytic cells. Although Ca2+ imaging has been performed to monitor the interaction between the synergid cell and the pollen tube14, Ca2+ dynamics during the actual gamete fusion is unknown. Here, we show Ca2+ dynamics of the female gametophytic cells in semi-in vivo condition by using the Ca2+ probe Yellow Cameleon 3.60 (YC3.60) (ref. 15) and high-resolution microscopies. The egg cell revealed two Ca2+ spikes following pollen tube discharge and plasmogamy. The central cell displayed similar Ca2+ spikes with the first one occurring on pollen tube discharge but the second spike not always being correlated with the plasmogamy. The two synergid cells on the other hand displayed very different Ca2+ dynamics. Both synergid cells showed Ca2+ oscillations on pollen tube arrival. Ca2+ was higher in the receptive synergid, but oscillations were sustained in the persistent synergid after double fertilization. The data suggest that characteristic Ca2+ signalling in the principal female gametophytic cells is involved in successful double fertilization in plants.
Results
Two Ca2+ spikes in the egg cell during double fertilization
To monitor cytosolic Ca2+ dynamics in the egg cell of Arabidopsis thaliana, the Ca2+ probe Yellow Cameleon 3.60 (YC3.60) (ref. 15) was expressed under the egg cell-specific promoter DD45 (ref. 16). Ovules expressing this YC3.60 sensor were cultivated with pollen tubes for semi-in vivo double fertilization6,17. In this setup, the female gametophyte is intact and still surrounded by the ovule tissues. To visualize behaviour of sperm cells, their nuclei were labelled with the red fluorescent protein mRFP fused to the histone H3.3 variant HTR10 (ref. 6). We at first performed two-photon excitation imaging, which enabled us to simultaneously excite CFP and mRFP without any time lag using the 800 nm excitation wavelength18 and to obtain high-resolution imaging within the depths of the ovule6. On the basis of the movement of sperm cell nuclei, the timing of pollen tube discharge, egg cell fertilization and central cell fertilization were evaluated as previously reported6. The rapid movement of the sperm cell nuclei is indicative of pollen tube discharge. After a short period of immobility, the sperm cell nuclei resume movement towards the target female gamete cells representing fertilization (plasmogamy)6,19. We observed two transient peaks of the cytosolic Ca2+ concentration ([Ca2+]cyt) in the egg (Fig. 1b,c, Supplementary Movie 1, Supplementary Fig. 1a), which appeared correlated in time with pollen tube discharge and egg cell fertilization, respectively. There was no clear Ca2+ change detected in the egg at the timing of central cell fertilization (Fig. 1b,c).
For imaging at higher temporal resolution, Förster resonance energy transfer (FRET)/cyan fluorescent protein (CFP) ratio imaging of ovules was performed at one to four frames per min using a spinning-disk confocal microscope equipped with automatic filter changer and high sensitive electron multiplying-charge coupled device (EM-CCD) camera (Fig. 1d,e, Supplementary Fig. 1b). Consistent with the observations made by two-photon excitation imaging, monitoring [Ca2+]cyt of the egg cell in 15 s time-lapse intervals did not reveal an oscillatory pattern following fertilization as is typical for many animal gamete fusions, but instead two distinct, transient Ca2+ spikes were observed (Fig. 1d,e, Supplementary Movie 2). The data show that the first Ca2+ peak corresponded to pollen tube discharge, whereas the second coincided with egg cell fertilization (Fig. 1d,e). No noticeable Ca2+ elevation was detected in the egg cell at the time of central cell fertilization (Fig. 1e). The first peak in [Ca2+]cyt was of relatively short duration (2.8±1.0 min) and occurred simultaneously in the entire egg cell without apparent starting location. The second peak seemed to start at the chalazal end where the fusion with the sperm cell occurs and then spread over the entire cell (Fig. 1d), consistent with observations made during in vitro fertilization of the maize eggs10. Remarkably, the duration of the second peak (4.7±1.2 min), while longer than the first, was much shorter than the peak observed in the in vitro fertilization system using maize (several tens of min to more than 1 h10,20).
Previously, we have shown that the order of egg cell and central cell fertilization is arbitrary6. Therefore, to substantiate the temporal correlation between individual events, we quantitatively analysed Ca2+ dynamics in the egg cell using data from a total of 28 cases of pollen tube discharge, 24 cases of egg cell fertilization and 21 cases of central cell fertilization. The average time delay between pollen tube discharge and the first Ca2+ peak was 2.3±15 s (Fig. 1f), clearly confirming that this first Ca2+ peak corresponds to the timing of pollen tube discharge. The second Ca2+ peak correlated much stronger with the moment of egg cell fertilization, which is indicated by a sudden movement of the sperm cell nucleus, than that of central cell fertilization (Fig. 1g,h) corroborating that this second Ca2+ peak in the egg cell corresponds to the timing of its own fertilization.
Distinct triggers of two Ca2+ spikes in the egg cell
The two spikes in [Ca2+]cyt clearly seem to represent characteristic Ca2+ dynamics of the egg cell during double fertilization. While the temporal correlation of these peaks with the events occurring in the male gametophyte was striking, we wanted to prove the existence of a causal relationship. To do so, we used a mutant of the GCS1/HAP2 gene, which encodes a highly conserved male gamete transmembrane protein in various eukaryotes including A. thaliana21,22. In the gcs1/hap2−/+ mutant, pollen tube discharge occurs normally, but the sperm cells do not fuse with the egg or central cell, probably due to a defect in a step after the cell attachment21,22,23. In the semi-in vivo assay used here, the two sperm cells of the gcs1/hap2 mutant pollen do not indeed move towards or fuse with their targets but remain at the location where they were ejected (Fig. 2a, Supplementary Movie 3). In these samples, only the first Ca2+ spike was observed in the egg cell and no subsequent Ca2+ spike was detected (Fig. 2a,b). In the absence of pollen tube discharge, no Ca2+ spike was detected (Supplementary Fig. 2a,b, Supplementary Movie 4). These observations are consistent with the first Ca2+ peak being triggered by pollen tube discharge and the second peak requiring a gamete fusion event.
On pollen tube discharge, both the pollen tube and the receptive synergid cell rupture, and their contents can be exposed to the egg cell6,24, which involves high concentration of Ca2+ deriving from the synergid cell24,25. To examine whether such exposure to external Ca2+ can trigger cytosolic Ca2+ elevation in the egg cell, we performed laser disruption of one of the synergid cells in semi-in vivo cultivated ovules. The femtosecond pulse laser normally used for two-photon microscopy is able to disrupt a single cell within thick tissues by focusing high energy in short pulses without thermal damage26. Following such a laser-mediated disruption of a synergid cell, cytosolic Ca2+ spikes in the egg cell were observed in eight cases out of 10 (Supplementary Fig. 3a,b, Supplementary Movie 5). In contrast, when the central cell was disrupted in a similar fashion, only a weak Ca2+ spike was observed in the egg (n=6; Supplementary Fig. 3c,d, Supplementary Movie 6).
To dissect the relationship between the second Ca2+ spike and double fertilization, we next used an A-type cyclin-dependent kinase (cdka;1) mutant27,28. About 40% of the pollen tubes of the cdka;1 mutant only carry a single sperm cell29. This single sperm cell can fertilize either the egg cell (18.9%) or the central cell (5.8%) (ref. 29). In ovules in which the egg cell but not the central cell was fertilized by the cdka;1 single sperm cell, two Ca2+ peaks were observed (Fig. 2c,d, Supplementary Movie 7), with the timing of the second peak being correlated with the timing of the egg cell fertilization event (Fig. 2d). In contrast, when the central cell was fertilized by the cdka;1 single sperm cell, only one detectable Ca2+ peak was observed and it temporally correlated with the moment of pollen tube discharge (Fig. 2e,f, Supplementary Movie 8). These results clearly indicate that the second Ca2+ peak in the egg cell depends on egg cell fertilization and is independent of central cell fertilization. To ascertain the relationship between the moment of gamete membrane fusion and the second Ca2+ spike, a marker line labelling the egg cell plasma membrane by TagRFP19 was combined with the cytosolic YC3.60 marker line. This enabled us to determine that the second Ca2+ spike coincided with the movement of the sperm nucleus across the egg cell plasma membrane (Fig. 2g,h, Supplementary Movie 9). This was consistent with the behaviour of the sperm cell nucleus and Ca2+ elevation during in vitro fertilization in maize7,10. We conclude that the second Ca2+ spike in the egg cell is associated with gametic fusion, that is, plasmogamy of the egg cell.
Calcium spikes in the central cell
To complement the data obtained in egg cells, we examined Ca2+ dynamics in the other crucial cells of the female gametophyte, the central cell and the two synergid cells. Using cell-specific YC3.60 marker lines (FWA promoter for the central cell and MYB98 promoter for the synergid cell) and spinning-disk confocal microscopy. In vitro fertilization assays performed in Nicotiana tabacum had not revealed any Ca2+ peaks in the central cell30. When we observed the Ca2+ levels in the central cell of Arabidopsis at 1 frame per min, we did not detect any Ca2+ spikes (data not shown). However, image acquisition at two frames per min enabled us to detect Ca2+ spikes under the experimental condition we used. Coinciding with the moment of pollen tube discharge, Ca2+ spikes were observed in all samples (n=13) (Fig. 3a,b, Supplementary Movie 10, Supplementary Fig. 1c). After pollen tube discharge, a second Ca2+ spike was observed in 10 of 19 samples (Supplementary Table 1). The duration of the second spike was 1.7±0.7 min and as in the case of the egg cell, no oscillatory pattern was observed following fertilization in the central cell. Occasionally, the second peak correlated with central fertilization (4 of 10) but in others it coincided with egg cell fertilization (5 of 10 including two cases of simultaneous double fertilization; Supplementary Table 1). In two of 10 cases, second peaks correlated with neither egg cell fertilization nor central cell fertilization. However, we never observed a Ca2+ spike in the central cell before pollen tube discharge (n=8 which observed at least 20 min before pollen tube discharge).
Distinct calcium oscillations in the two synergid cells
It was suggested that Ca2+ oscillation and burst occur in the synergid cell at pollen tube arrival and discharge, respectively14, but the two synergid cells were not studied individually. In our setup, we were able to simultaneously monitor Ca2+ dynamics in the two synergid cells in those 18 samples where these could be distinguished (Fig. 3c,d, Supplementary Fig. 3d,e). Before pollen tube arrival at the ovule, no oscillatory signal was detected under the experimental condition we used (n=3), consistent with the previous report14. When a pollen tube contacted the synergid cell, alternating Ca2+ oscillations occurred in the two synergid cells with the FRET/CFP ratio being similar in the two cells (Fig. 3c,e, Supplementary Movie 11). Just before pollen tube discharge, Ca2+ oscillation stopped and continuous, rapid elevation of cytosolic Ca2+ occurred in both synergid cells. Interestingly, the Ca2+ level in the receptive synergid cell before pollen tube discharge was higher than in the persistent synergid cell in 12 of 18 samples, suggesting that the receptive synergid is predetermined before pollen tube discharge. Immediately following pollen tube discharge, both synergids displayed sharp, short lived Ca2+ peaks followed by a rapid return to the earlier Ca2+ levels. To our surprise, the persistent synergid cell started oscillation again after double fertilization occurred (Fig. 3e, Supplementary Movie 11, Supplementary Fig. 4).
Discussion
We observed Ca2+ dynamics in all the female gametophytic cells directly involved in the double fertilization of Arabidopsis. The egg cell displayed two distinct spikes on pollen tube discharge and gamete fusion, respectively. To examine the origin of the first Ca2+ spike, we performed cell disruption analysis. When one of the two synergid cells was disrupted using laser, a transient Ca2+ spike was detected in the egg cell, but no distinct signal was detected when the central cell was disrupted. It has been reported that synergid cells contain a high concentration of Ca2+ in their cytosol compared with the other female gametophyte cells24,31. Disruption of the synergid cell might therefore have caused an elevation of the external Ca2+ that was sufficient to cause the cytosolic Ca2+ concentration in the egg to spike. On the other hand, it has been reported that mechanical stimulation can trigger cytosolic Ca2+ elevation32. When one of the two synergid cells was disrupted, it immediately shrank (Supplementary Movie 5), a phenomenon that resembles that of pollen tube discharge. Therefore, another possibility is that the mechanical stimulation resulting from synergid cell disruption might have caused cytosolic Ca2+ elevation in the egg cell. Taken together, our data suggest that the first Ca2+ spike in the egg cell is at least partly due to synergid cell degeneration triggered by pollen tube discharge and is independent of fertilization. High cytosolic concentration of Ca2+ at the tip of the pollen tube14 and mechanical pressure by the discharged pollen tube contents6 are also possibly involved in the Ca2+ spike of the egg cell during pollen tube discharge. The egg cell is known to secrete an EC1 peptide following pollen tube discharge but before fertilization. This peptide has been reported to activate sperm cells for fusion33. It is therefore reasonable to speculate that the egg cell senses pollen tube discharge and this Ca2+ spike triggers peptide secretion.
In animals like frogs and several marine invertebrates, polyspermy (the fertilization of an egg by two or more sperm cells) is prevented by an electrical charge across the surface of the egg (fast block in a few seconds) and/or by modification of the extracellular egg coat by a secretion reaction (slow block in dozens of seconds), following gamete fusion34. A Ca2+ wave in the fertilized egg triggers the secretion reaction associated with the slow polyspermy block34. In the flowering plants, the mechanism of polyspermy block is unknown. However, the phenomenon was recognized by in vitro fertilization analysis in maize about 20 years ago7. Recent genetic approaches suggest the existence of a polyspermy block for both female gametes with the block in the egg cell being stronger than that in the central cell13. We speculate that the second Ca2+ spike during fertilization of A. thaliana might be involved in blocking polyspermy. The fact that the Ca2+ peak was observed simultaneously with the movement of the sperm nucleus across the plasma membrane of the egg cell at an image acquisition rate of four frames per min (Fig. 2g,h), suggests that Ca2+ elevation begins within seconds after gamete fusion. The origin of this cytosolic Ca2+ peak remains elusive. However, in the maize in vitro system using isolated egg cells, the origin of the [Ca2+]cyt elevation in the fertilized egg cell has been suggested to be an intracellular Ca2+ store rather than global influx from the outside20. Interestingly, the first Ca2+ spike on pollen tube discharge does not seem to be involved in blocking polyspermy because discharge by gcs1/hap2 pollen tubes does not inhibit fertilization by a second, wild-type pollen tube even when its arrival and discharge occur several hours later35. Hence, the two Ca2+ peaks, triggered by pollen tube discharge and fertilization, respectively, seem to have different physiological roles.
Unlike most animal eggs, no oscillations of Ca2+ were observed in the fertilized egg cell of A. thaliana. After the single fertilization-induced Ca2+ peak, [Ca2+]cyt decreased to a resting level within 4.7±1.2 min and no subsequent peak was observed for at least 45 min after fertilization. It cannot be excluded that there might be other spikes that could not be detected in our 15–30 s time-lapse in vivo imaging, but no oscillation was detected in the in vitro system using isolated maize eggs either10,20 nor in independent work on the Arabidopsis female gametophyte using a different Ca2+ probe36. This is consistent with previous in vitro fertilization analyses that showed no subsequent peak for at least 50 min after fertilization10. The presence of a single pulse of Ca2+ rather than oscillations during gamete fusion has been reported in some animal species, for example cnidarians, echinoderms, fish and frogs3. However, in these species, a single Ca2+ pulse typically fails to fully activate the oocytes, whereas multiple Ca2+ spikes tend to successfully release oocytes from meiotic arrest to form both polar bodies37,38,39. Multiple spikes are likely to provide a more robust trigger, and the pattern of Ca2+ spikes might depend on the necessity of a resumption from meiotic arrest3. In flowering plants, no resumption from meiotic arrest is required40. Instead, flowering plants show unique cell cycle control in fertilization among eukaryotes; sperm cells of Arabidopsis in G2 phase have been proposed to fuse with the egg cell in G1/S or G2 phase and with the central cell in G2 phase41. Different mechanisms of cell cycle arrest and activation might exist. Moreover, the transcriptional activation of male and female genomes in the zygote is critical for establishing apical–basal cell polarity over a long period of time before the first division42,43. Our data suggest that unlike egg cell functioning in animals such as hamster, in Arabidopsis, a single spike of [Ca2+]cyt at fertilization with a duration that is much shorter than that observed during maize in vitro fertilization7,20, might be sufficient for blocking polyspermy and initiation of the developmental programme.
The other female gamete, the central cell, showed a Ca2+ peak correlated with pollen tube discharge and sometimes showed a second Ca2+ spike, which did not display any consistent correlation with the timing of the central cell fertilization or that of egg cell fertilization. It can be stated, however, that the second Ca2+ spike in the central cell is related to the gametic phase of double fertilization after the release of the sperm cells. Determination of fertilization targets during the gametic phase of double fertilization is still largely unknown but must require complex gamete recognition and/or blocking polyspermy in both female gametes13. The second Ca2+ spike observed in the central cell might reveal unidentified cell-to-cell communication in double fertilization, although development of a high-speed and high-sensitivity microscope system will be necessary to detect faint Ca2+ spikes efficiently.
Both synergid cells showed Ca2+ oscillation after pollen tube arrival, but before pollen tube discharge, with the receptive synergid cell showing superior Ca2+ elevation (flooding) confirming independent studies36,44. Components of the FERONIA receptor kinase signalling pathway are required for appropriate calcium dynamics in the synergid cells44. The Ca2+ elevation in the receptive synergid cell might be involved not only in its subsequent degeneration5 but also in the interaction with the pollen tube by extruding Ca2+ through calcium channels, which in turn trigger pollen tube rupture45. On pollen tube discharge, a strong Ca2+ spike was observed in both synergid cells. This Ca2+ spike might result from the breakdown of the receptive synergid cell including its vacuole and/or from the mechanical stimulation during pollen tube discharge24. To our surprise, an onset of Ca2+ oscillation in the persistent synergid cell following double fertilization was observed. Completion of fertilization in the two female gametes independently, but additively, suppresses the attraction activity of the persistent synergid cell46, which eventually degenerates during the onset of seed development47. It is conceivable that Ca2+ oscillation in the persistent synergid cell is triggered by fertilization of the female gametes and that this Ca2+ signature is involved in the cessation of synergid cell function.
To summarize, we revealed distinct Ca2+ dynamics in the crucial female gametophytic cells during double fertilization. In the future, new technology such as optical manipulation of Ca2+ spiking48 may provide insights into physiological roles of the Ca2+ signalling observed in this study. Knowledge of these Ca2+ dynamics and their physiological roles will accelerate the identification of key molecules involved in intra- and intercellular signalling during double fertilization.
Methods
Plant materials and growth conditions
A. thaliana ecotype Columbia (Col-0) was used as the wild type. The pHTR10::HTR10-mRFP6, pRPS5A::H2B-tdTomato49, pDD45::TagRFP-PIP2a19, gcs1/hap2−/+ (ref. 21) and cdka;1−/+ (ref. 27) lines have been described previously. Seeds were sterilized with 5% sodium hypochlorite containing 0.5% Triton X-100 and germinated on plates containing 0.5 × Murashige and Skoog salt (pH 5.7; Wako Pure Chemical, Osaka, Japan), 2% sucrose, Gamborg’s B5 vitamin solution (Sigma) and 0.3% Gerlite (Wako Pure Chemical) in a growth chamber at 22 °C under 24-h light after cold treatment (4 °C) for 2 days. Ten-day-old seedlings were transferred to soil (Hanachan-baiyoudo; HANAGOKORO, Nagoya, Japan) and grown at 22 °C under 24-h light.
Semi-in vivo fertilization assay
Pollen tube growth medium (14% sucrose, 0.001% boric acid, 1.27 mM Ca(NO3)2, 0.4 mM MgSO4, 1.5% agarose (50081; Lonza) and adjusted to pH 7.0 with KOH) was used for the semi-in vivo fertilization assay. For the well, 1-mm thick silicon rubber (6-611-02, AsOne) was placed on a 2,550-mm coverslip (C025501, Matsunami). About 150 μl of medium melted at 65 °C was poured into the well, and covered with another coverslip. Flowers were emasculated 12–18 h before hand pollination. Pistils held on a glass slide with double-sided tape were hand pollinated under a stereomicroscope, and cut with a 27-gauge needle (NN-2738R, Terumo) at the junction between the style and ovary, and placed on the medium. The pistils were excised ovules with a 0.5-mm-diameter insect pin. The ovules were placed immediately on the medium within 2 mm of the distance from the pistil. Double fertilization was observed 5–8 h after pollination at 20 °C in the dark.
Vector construction
The YC3.60 coding sequence followed by the nopaline synthase terminator (NosT) was digested with BamHI and EcoRI from pACT1::YC3.60 vector50 and cloned into the binary vector pPZP211 (ref. 51) using BamHI and EcoRI sites, resulting in pPZP211-YC3.60. The YC3.60 coding sequence was also digested with BamHI and SacI from pACT1::YC3.60 vector and cloned into a subcloning vector pBlueMAP42 derivative in which multiple cloning sites located between AscI sites were replaced by multiple cloning sites from the pPZP vector followed by NosT sequence, resulting in pBlueMAP-YC3.60. Promoter regions of MYB98 (ref. 52), FWA53 and DD45 (ref. 16) were amplified by PCR from genomic DNA with primer pairs (5′- caccaagcttGGTGAAGAGAGAGAGAGAGA -3′ and 5′- cgcggatccGTGTTCTTGATCACGTGTGAAG -3′ for MYB98 promoter; 5′- cccaagcttGGTAGGCTAATAATCAGAAGCCC -3′ and 5′- cgggatccTTTCCCTCAATGCAATAACCTG -3′ for FWA promoter; 5′- ggagtcgacCTCAGAGAACATGAACGGGTC -3′ and 5′- ggagtcgacTATTCTTTCTTTTTGGGGTTTTTG -3′ for DD45 promoter). The MYB98 and FWA promoters were inserted into the pPZP211-YC3.60 using HindIII and BamHI, resulting in the binary vectors pPZP211-pMYB98::YC3.60 and pPZP211-pFWA::YC3.60. The DD45 promoter was subcloned in the pBlueMAP-YC3.60 using SalI. A cassette containing the DD45 promoter followed by YC3.60 and NosT was cut with AscI and ligated in a pMDC99 (ref. 54) derivative in which ccdB was removed by EcoRI digestion and self-ligation, resulting in the binary vector pMDC99-pDD45::YC3.60.
The binary vectors pPZP211-pMYB98::YC3.60, pPZP211-pFWA::YC3.60 and pMDC99-pDD45::YC3.60 were introduced into Agrobacterium tumefaciens strain GV3101 and then transformed into wild-type A. thaliana plants (Col-0) using the floral dip method. Transformed plants were selected on Murashige-Skoog plates containing 50 μg per 1 ml kanamycin for pPZP211-pMYB98::YC3.60 and pPZP211-pFWA::YC3.60 or 20 μg per 1 ml hygromycin B for pMDC99-pDD45::YC3.60.
Microscopy settings
For calcium imaging, we used four microscope systems: spinning-disk confocal microscopes, laser scanning confocal microscope and two-photon excitation microscope.
Confocal images were acquired using an inverted microscope (IX-81; Olympus, Tokyo, Japan) equipped with an automatically programmable XY stage (MD-XY30100T-Meta; Molecular Devices, Sunnyvale, CA), a spinning-disk confocal system (CSU-X1; Yokogawa Electric, Tokyo, Japan), 445 nm (Stradus; Vortran Laser Technologies, Sacramento, CA) and 561 nm (Sapphire; Coherent, Santa Clara, CA) LD lasers and EM-CCD camera (Evolve 512, Photometrics, Tucson, AZ). Time-lapse images were acquired every 10–60 s using multiple z-planes (3.0-μm intervals) and three to 11 planes with a × 40 water-immersion objective lens (UApo 40XW3/340, WD=0.25 mm, NA=1.15; Olympus) or with a × 60 silicone immersion objective lens (UPLSAPO60XS, WD=0.30 mm, NA=1.30; Olympus) mounted on a Piezo focus drive (P-721; Physik Instrumente, Karlsruhe, Germany). For rapid imaging, the images were acquired every 10–15 s with single z plane. Exposure times were 100–300 ms for CFP and Venus, and 50–100 ms for mRFP. We used three band-pass filters, 482/35 nm for CFP, 578/105 nm for Venus and 600/37 nm for mRFP. Images were processed with Metamorph (Universal Imaging Corp., Downingtown, PA) to create maximum intensity projection images and to add colour.
For split-view imaging, we used an inverted microscope (IX-81; Olympus) equipped with an automatically programmable XY stage (BioPrecision; Ludl Electronic Products Ltd, Hawthorne, NY), a spinning-disk confocal system (CSU-W1; Yokogawa Electric), 445 nm (Stradus; Vortran Laser Technologies) and 561 nm (Sapphire; Coherent) LD lasers and EM-CCD camera (ImagEM 1K; Hamamatsu Photonics, Shizuoka, Japan). Time-lapse images were acquired every 10–60 s using multiple z-planes (3.0-μm intervals) and three to 11 planes with a × 40 water-immersion objective lens (UApo 40XW3/340) or with a × 60 silicone immersion objective lens (UPLSAPO60XS). For rapid imaging, the images were acquired every 10–15 s with single z plane. Exposure times were 100–300 ms for CFP and Venus, and 50–100 ms for mRFP. We used three band-pass filters, 482/35 nm for CFP, 578/105 nm for Venus and 600/37 nm for mRFP. Images were processed with Metamorph (Universal Imaging Corp.) to create maximum intensity projection images and to add colour.
For laser disruption, we used a laser scanning inverted microscope (LSM780-DUO-NLO; Zeiss, Göttingen, Germany) equipped with a Ti-Sapphire femtosecond pulse laser (Chameleon Vision II; Coherent). A Ti:sapphire laser tuned to 800 nm was used for disruption and excitation. To disrupt single cells, the targets were irradiated by femtosecond pulse laser with one-frame scanning. Before and after laser irradiation, time-lapse images were acquired using single z plane with a × 40 water-immersion objective lens (LD C-APOCHROMAT, WD=0.62 mm, NA=1.10; Zeiss). The images were acquired every 15 s at 250 ms per scan. Each image is the average of two lines. Emitted fluorescence signals were detected by the external Non-Descanned GaAsP Detectors. We used a filterset for CFP/YFP (1756-084; Zeiss), 460–500 nm for CFP, 525–560 nm for Venus. The images were acquired and analysed using the ZEN 2010 software (Zeiss).
Two-photon images were acquired using a laser scanning inverted microscope (A1R MP; Nikon, Tokyo, Japan) equipped with a Ti-Sapphire femtosecond pulse laser (Mai Tai DeepSee; Spectra-Physics, Mountain View, CA). A Ti:sapphire laser tuned to 800 nm was used for excitation. Time-lapse images were acquired using multiple z-planes (2.0 or 3.0 μm intervals) and four to eight planes with a × 40 water-immersion objective lens (CFI Apo LWD × 40 WI, WD=0.61 mm, NA=1.15; Nikon). The images were acquired every 60 s at 500 ms per scan. Each image is the average of two lines. Emitted fluorescence signals were detected by the external Non-Descanned PMT Detectors. We used two dichroic mirrors, DM495 and DM560, and three band-pass filters, 479/40 nm for CFP, 534/30 nm for Venus, and 578/105 nm for mRFP. The images were acquired and analysed using the NIS-Elements AR software 4.10 (Nikon).
Image processing
All images were adjusted for brightness and contrast by Adobe Photoshop CS4 (Adobe Systems, Inc., San Jose, CA). MacBiophotonics ImageJ software (http://www.macbiophotonics.ca/) was used for editing of the images and movies. Images were aligned to correct for experimental drift using the ImageJ plugin ‘align slices in stack’ (https://sites.google.com/site/qingzongtseng/template-matching-ij-plugin). For FRET pixel-to-pixel ratiometric processing and efficiency analysis, corrected FRET images were obtained by using the FRET dialogue feature of Metamorph (Universal Imaging Corp.). CFP and FRET emissions were summed over an entire cell after background subtraction, and the FRET:CFP emission ratio was calculated. Representative FRET/CFP ratio images are shown in the intensity modulated display mode with 32-intensity in 8-ratio.
Author contributions
T.H. designed the study. Y.H. and M.N. carried out most experiments. M.N. and H.T. cloned YC3.60 constructs. Y.H. did data analysis. Y.H., D.K. and H.T. wrote the manuscript. Y.H. and D.K. arranged the figures. A.G. and T.H. edited the manuscript.
Additional information
How to cite this article: Hamamura, Y. et al. Live imaging of calcium spikes during double fertilization in Arabidopsis. Nat. Commun. 5:4722 doi: 10.1038/ncomms5722 (2014).
Supplementary Material
Acknowledgments
We thank Michitaka Notaguchi for discussion and critical comments on our work. We also thank Megumi Iwano for technical advice and discussion. We thank Atsushi Miyawaki for providing the YC3.60 plasmid. We thank Tomoko Igawa for providing the pDD45::TagRFP-PIP2a seeds. We thank Yoshitaka Sekizawa and Hideki Tanaka for technical assistance with the spinning-disk confocal system, CSU-WI. H.T. was supported by grant numbers 5834 from the Japan Society for the Promotion of Science Fellowships. This research was supported by Japan Advanced Plant Science Network. This work was supported by grants from the Japan Science and Technology Agency (ERATO project to T.H.) and the Ministry of Education, Culture, Sports, Science and Technology, Japan (no. 11025940 to D.K.).
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