© 2008 Nature Publishing Group http://www.nature.com/naturemethods ARTICLES Imaging dynamic cell-cell junctional coupling in vivo using Trojan-LAMP Yan-Ming Guo1,3, Shiuhwei Chen1,3, Premnath Shetty2, Genhua Zheng1, Rueyling Lin2 & Wen-hong Li1 To study the physiological regulation and function of cell-cell gap junction communication in vivo, we developed a bioconjugate of caged dye, named dextran-CANPE-HCC, for imaging cell coupling in small model organisms. In vitro, the compound was photolyzed efficiently with robust fluorescence enhancement. Dextran-CANPE-HCC delivered into Caenorhabditis elegans oocytes was retained in cells throughout development. Using local uncaging, we photolyzed dextran-CANPE-HCC to release the small HCC dye and imaged the dynamics of intercellular dye transfer through gap junction channels, a technique we named Trojan–local activation of molecular fluorescent probes (LAMP). Early during embryonic development, the pattern of cell coupling undergoes dramatic remodeling and imaging revealed that the germ cell precursors, P2, P3 and P4, were isolated from the somatic cell communication compartment. As dextran-CANPE-HCC is chemically and metabolically stable, labeled worms showed very bright signal upon photoactivation after hatching, which allowed us to examine cell coupling in living worms noninvasively. Intercellular communication through gap junction channels is ubiquitous in multicellular organisms and is essential for many vital physiological processes including heart beating, labor, secretion and neuronal communication1,2. There have been extensive studies of the regulation of junctional coupling in cultured cells, in heterologous expression systems such as Xenopus laevis oocytes and in isolated or reconstituted membranes3,4. Although these studies have generated biochemical, biophysical and cellular-biological insights into gap junction channels, relatively few studies are carried out in living organisms. The paucity of in vivo data is due, at least in part, to the fact that we do not yet have a noninvasive and sensitive assay to examine the distribution, strength and dynamics of cell coupling in living organisms. To better examine gap junction coupling in intact living cells or in dissected tissues, we recently developed photouncaging and fluorescence imaging techniques, LAMP and infrared-LAMP5,6, which involve loading cells with a caged, membrane-permeant and acetoxymethyl (AM) ester–containing coumarin dye called NPE-HCCC2/AM (ref. 7). There are several challenges in adapting LAMP to study gap junction coupling in vivo. First, cellular uptake of dyes containing AM esters is generally poor in living organisms, in particular for loading cells that are far away from the body surface. Second, small organic molecules tend to slowly leak out of cells or become compartmentalized in cellular organelles, making it difficult to image them for a long time. Third, these probes must be chemically and metabolically stable, and should not be toxic to the labeled animals. To develop a noninvasive imaging assay to study cell coupling in vivo, we used C. elegans, which is transparent at all stages of development and is thus ideal for optical imaging. The relatively small number of cells (B560 cells in the first larval stage and B1,000 in the adult), the invariant cell lineage and the capacity to image the entire cellular architecture by serial section electron microscopy8 are advantageous for tracking cell-cell communication networks at all stages of this nematode’s development. As invertebrates, C. elegans express innexins rather than connexins9, and 25 innexin genes were identified in the C. elegans genome sequencing project. More recently, innexin-like genes named pannexins have been discovered in mammals10. Although innexins or pannexins share no substantial sequence similarity with connexins, the overall topologies of these different classes of proteins are remarkably similar11, and these proteins have been suggested to be important in mediating cell-cell communication. Currently, little is known about the functions of pannexins in vivo. We report here the development of a new class of bioconjugates of photoactivatable dyes, dextran-CANPE-HCC, for imaging cell coupling in living worms. After injection into the ovary of C. elegans adult hermaphrodites, dextran-CANPE-HCC was retained in cells throughout embryonic development and in hatched worms, with no observable toxic effects on development. This dye remained stable in cells and fluoresced brightly upon photolysis. We characterized the pattern of junctional cell coupling in developing C. elegans embryos, revealing a dramatic remodeling of cell coupling among early blastomeres even before the 4-cell stage, with the germ-line blastomere quickly becoming poorly coupled to somatic cells. We could also uncage the probe in specific cells in hatched larvae to generate bright fluorescence. This allows us to study cell-cell communication in live worms noninvasively with high spatiotemporal resolution. 1Departments of Cell Biology and of Biochemistry, and 2Department of Molecular Biology, University of Texas Southwestern Medical Center, 5323 Harry Hines Blvd., Dallas, Texas 75390, USA. 3These authors contributed equally to this work. Correspondence should be addressed to W.-H.L. ([email protected]). RECEIVED 16 APRIL; ACCEPTED 4 JULY; PUBLISHED ONLINE 1 AUGUST 2008; DOI:10.1038/NMETH.1238 NATURE METHODS | VOL.5 NO.9 | SEPTEMBER 2008 | 835 ARTICLES worms with the dye premixed with bacteria (Supplementary Fig. 1 online). Photolysis MacroWe therefore designed a new class of MacroCage Cage Coumarin + Coumarin molecule molecule bioconjugates of caged probes in which a macromolecule such as dextran served as a carrier for the caged probe and, notably, the Dextran Dextran carrier was linked to a fluorophore indirO ectly through the caging group (type 2 O O –O O O O O O Photolysis C NH C NH H NO H bioconjugate; Fig. 1). This design is distinct N + N O2N N N COO– COO– from conventional bioconjugates of caged O O dyes, in which a fluorophore is permanently Dextran-HCC-NPE Dextran-HCC linked to a macromolecule12 (type 1 bioconjugate; Fig. 1a). In dextran-CANPEb HCC, a coumarin dye, 7-hydroxy coumarin Photolysis MacroMacroCoumarin Cage Coumarin Cage + 3-carboxamide (HCC) is linked to dextran molecule molecule through a bifunctional photolabile protecting group (cage), 1-(4-carbamoyl-2-nitroO phenyl)ethyl (CANPE). Upon photolysis, O O O COO– H – ON O O O O2N N the coumarin fluorophore is released from N – Photolysis COO H COO– + O N N the dextran-cage conjugate, becomes fluo– COO O rescent and freely diffusible, and passes O N O N H Dextran Dextran H through gap junction channels. We named this technique Trojan-LAMP. Dextran-CANPE-HCC HCC We synthesized dextran-CANPE-HCC in 12 steps (Fig. 2a). Dextran-CANPE-HCC Figure 1 | Bioconjugates of caged probes. (a,b) Schematic showing photolysis of conventional bioconjugates (type 1; a) and a new type of bioconjugate (type 2, in which coumarin is released from the has negligible fluorescence. After complete carrier upon photolysis; b) of caged probes (top). Examples for each type of bioconjugates used in this photolysis at 365 nm, the fluorescence study and their photolyzed products are also shown (bottom). intensity increased over 260-fold with 410-nm excitation (Fig. 2b). Previously, we RESULTS have shown that the uncaging efficiency of NPE-caged coumarins is A new class of bioconjugates of photoactivatable probes extraordinarily high, about two orders of magnitude higher than We initially applied the LAMP technique to living worms that of caged fluorescein or rhodamine7, and dextran-CANPEusing NPE-HCCC2/AM (refs. 5,7). However, we detected no HCC retains almost as high a photolytic efficiency (Fig. 2c,d). We calculated its UV light–mediated uncaging cross-section (product cellular loading after incubating worms with the caged dye, and of the uncaging quantum yield (Qu) and extinction coefficient (e) only intestinal cells and lumen were loaded when we fed the b a 1. HNO3, –15 °C, 95% 2. 2-Trimethylsilylethanol, COOH EDC/HCI, pyridine, 67% O2N O O COOCH2CH2TMS COOCH2CH2TMS 2 3 O COO Bu H N O2N 1. DIEA, CH3CN, 51% t N O HO O O HO 4 steps O 2. Tetrabutylammonium fluoride, THF, 66% O H N OH COOH 5 t N(CH2COO Bu)2 O O O O O2N O 2. TFA, CH2Cl2, 100% O O O H N O2N H N N 9 6 Before photolysis 3 0 420 460 440 480 500 c 4 1. TFP, EDC/HCI, DMAP, 89% After complete photolysis 12 Wavelength (nm) O O t COO Bu COOH Dextran amine (40 kDa), DMSO, triethylamine; then dialysis, 60% COOH O O N H Conversion (%) O2N Emission intensity (a.u.) Br Benzoyl peroxide, NBS, 83% – COO N COO – Dextran OTFP 6 100 80 60 NPE-HCC Dextran-CANPE-HCC 40 20 0 Dextran-CANPE-HCC 0 100 200 300 400 500 Time (s) d 100 Figure 2 | Synthesis and characterization of dextran-CANPE-HCC. (a) (2-Trimethylsilyl)ethyl-4-ethyl-3-nitrobenzoate (2), prepared from 4-ethylbenzoic acid, was converted to (2-trimethylsilyl)ethyl-4-(1-bromo)ethyl-3-nitrobenzoate 80 (3), which was then coupled with 7-hydroxycoumarin-3-carboxamide (4, from 7-hydroxycoumarin-3-carboxylate) to NPE-HCC 60 Dextran-CANPE-HCC give caged coumarin-3-carboxamide (5). Subsequent transformations provided 7-{1-[4-(2,3,5,6-tetrafluoro40 phenoxy)carbonyl-2-nitrophenyl]ethoxy}-coumarin-3-carboxamide (6), which yielded dextran-CANPE-HCC upon 0 10 20 30 conjugation. EDC, N-(3-dimethylaminopropyl)-N¢-ethylcarbodiimide; DIEA, N,N-diisopropylethylamine; THF, Time (min) tetrahydrofuran; DMAP, 4-(dimethylamino)pyridine; NBS, N-bromosuccinimide; TFP, 2,3,5,6-tetrafluorophenol; TMS, trimethylsilyl. (b) Fluorescence emission spectra (excitation, 410 nm) of dextran-CANPE-HCC before and after complete photolysis. (c,d) Time course of photoconversion of dextran-CANPE-HCC and NPE-HCC (reference compound) photolyzed at 365 nm (c) or at 740 nm by two-photon excitation (d). Caged HCC remaining (%) © 2008 Nature Publishing Group http://www.nature.com/naturemethods a 836 | VOL.5 NO.9 | SEPTEMBER 2008 | NATURE METHODS 40 ARTICLES a b c2 FHCC (a.u.) 0 Ex P1 AB d UV e P1 f P1 1 Ex AB ABp 0 0 40 80 120 160 ABa Time (s) g UV FHCC (a.u.) ABp 3 ABa Figure 3 | Dye transfer in early embryos. (a–c) Differential interference contrast (DIC) (a) and coumarin fluorescence 2 P1 (b) images immediately after UV-light uncaging of the P1 cell in a 2-cell embryo. Time course (c) of the average HCC 1 fluorescence (FHCC) in three regions of interest (outlined in a in colors that correspond to those in c) in P1, AB and an 0 extracellular area (Ex) within the eggshell. (d–g) DIC (d), GFP–histone H2B fluorescence (e) and coumarin fluorescence (f) 80 120 0 40 images immediately after uncaging ABp in a 3-cell embryo. Dashed lines in the HCC fluorescence time course (g) are the slopes Time (s) indicating the initial dye intensity increase in recipient cells, representing the initial rate of dye transfer from ABp. In this experiment, HCC fluorescence of ABp decreased little owing to saturation of the detector. Dashed yellow outlines indicate the uncaging area. Double-sided arrows indicate the detected coumarin signal from light scattering immediately after uncaging, and single-sided arrows mark the UV-light uncaging (c,g). Scale bars, 10 mm. at 365 nm) to be 5,000 M–1 cm–1 and its two-photon-uncaging cross-section to be 0.5 Goeppert-Mayer (GM; 1 GM ¼ 1050 cm4 s/photon) at 740 nm. (It took longer for two-photon uncaging to be detected to an appreciable degree because we measured the accumulated photolysis of the bulk solution, whereas two-photon excitation only occurs at the focal point of a laser beam.) The high uncaging efficiency makes it possible to use much lower doses of light for photoactivation, thus minimizing photodamage. This is an important consideration for live-cell imaging, especially in experiments involving developing embryos that are more sensitive to phototoxicity13. Patterns of cell coupling in early developing embryos To introduce dextran-CANPE-HCC into C. elegans, we injected the probe into the distal end of gonads of young hermaphrodites. We also injected rhodamine-dextran as a fluorescent marker. The injected dye gradually filled the gonad syncytium and was detected in fertilized embryos in a few hours (Supplementary Fig. 2 online). Throughout development, labeled embryos showed little coumarin fluorescence signal, yet they displayed robust coumarin fluorescence after uncaging, confirming that dextran-CANPE-HCC is chemically and metabolically stable in vivo. We collected embryos from injected worms and studied the pattern of cell coupling during early development14 (see Supplementary Fig. 3 online for a schematic of C. elegans cell lineage). a b P2 c d e FHCC (a.u.) Figure 4 | Dye transfer in early 4-cell embryos. (a–j) Analysis of embryos after local uncaging of EMS (a–e) or ABp (f–j). DIC images (a,f; cell label colors correspond to those of traces in e,j; scale bars, 10 mm), GFP–histone H2B fluorescence images (b,g) and coumarin fluorescence images immediately after (c,h) or B30 s after (d,i) uncaging. Dashed yellow outlines indicate the uncaging areas. Time courses of the average HCC fluorescence intensity of the bulk cytoplasm (e,j). Regions of interest for each cell cover the cytoplasm in the center of the cell in each case. The boundary of each region was typically at least 2 mm away from the cell-cell contact. The pattern of cell coupling is representative of five embryos assayed in the early 4-cell stage. In 1-cell embryos, local uncaging at one end of an embryo generated a sudden increase in coumarin fluorescence near the uncaging area (Supplementary Fig. 4 online). The released HCC rapidly diffused across the entire cell and equilibrated in the cytosol in approximately 6 s, suggesting that HCC fluorophore does not bind strongly to cytoplasmic proteins or granules. This is an important requirement for tracers used to track cell-cell communication, so that the rate-limiting step of cell-cell dye diffusion is through gap junction channels. In 2-cell stage embryos, we locally photolyzed dextran-CANPEHCC in one cell (P1, the donor cell) by directing a narrow beam of UV light to areas away from the cell-cell interface, to minimize UV-light exposure of neighboring cells. After uncaging, we detected a fluorescent signal immediately in the neighboring cell (the AB cell; Fig. 3a–c). This was also seen in the extracellular space and is mainly caused by scattering of coumarin fluorescence from the donor cell to the neighboring areas. We also observed this phenomenon in embryos at other developmental stages (Fig. 3d–g) and in cultured cells at high confluence (data not shown), but it is more pronounced in developing C. elegans embryos, most likely because of extensive cell-cell contact in three dimensions and because of the presence of yolk granules. Apart from the scattering effect, in the majority of experiments done at the 2-cell stage, we did not detect obvious dye transfer ABp UV 2 EMS 1 P2 ABp ABa EMS 0 0 ABa f g P2 ABp EMS h i j FHCC (a.u.) © 2008 Nature Publishing Group http://www.nature.com/naturemethods 4 60 20 40 Time (s) UV ABp 2 ABa 1 P2 EMS 0 ABa 0 30 60 90 Time (s) NATURE METHODS | VOL.5 NO.9 | SEPTEMBER 2008 | 837 ARTICLES leakage as well as of potential indirect dye transfer from a donor to a recipient through ABa an intermediate cell. This approach allowed ABa 1 EMS us to compare relative coupling efficiency P2 ABp among blastomeres and also reduced or 0 P2 120 0 40 80 eliminated variations in absolute fluoresTime (s) cence intensities from experiment to experig f e ABa ABp h UV ment, thus allowing comparisons between EMS embryos. Using this approach, the coupling 1 ABa ABp P2 between AB cells was 10.2 ± 3.5 times (n ¼ 6 P2 0 EMS embryos, mean ± s.d.) stronger than the 0 20 40 60 80 coupling between ABp and P1. Even taking Time (s) P2 i j k l into account the cell volume difference UV between ABp and P1, these data still suggest P2 1 ABp that AB cells are selectively coupled at much ABp greater strength. The coupling between ABa EMS EMS 0 and P1 was also very weak compared with 0 40 80 120 ABa that between AB cells (data not shown). Time (s) p This selective coupling between AB cells m UV n o ABa persisted at the early 4-cell stage. Shortly ABp ABa 1 ABp after the cytokinesis of P1, we uncaged one P2 EMS of its daughter cells, EMS. Coupling between 0 EMS EMS and P2, the other daughter of P1, was 80 120 0 40 Time (s) strong, and there was little dye transfer to q either ABa or ABp (Fig. 4a–e and SuppleFigure 5 | Patterns of cell coupling in late 4-cell embryos. 1 mentary Movie 1 online). Uncaging ABp (a–p) Dye transfer after locally uncaging ABp (a–d), EMS (e–h), resulted in faster dye transfer to ABa P2 (i–l) or ABa (m–p). DIC images (a,e,i,m; cell labels were 0.5 (Fig. 4f–j) than to EMS or P2. colored to correspond to cell traces in d,h,l,p; scale bars, 10 mm), coumarin fluorescence images immediately after As development progresses, the pattern of uncaging (b,f,j,n; dashed yellow outlines indicate uncaging gap junction coupling among these 4 cells 0 areas) and B30 s after uncaging (c,g,k,o), and time courses of underwent a dynamic reorganization. the average HCC fluorescence intensity of the bulk cytoplasm Toward the mid 4-cell stage, the coupling (d,h,i,l,p). Regions of interest for each cell cover the center between AB cells was still strong, and there cytoplasm of the cell, with the boundary of each region typically at least 2 mm away from the cell-cell was little dye transfer from ABp to P2 (data contact. (q) Normalized relative coupling strengths (n ¼ 5, mean ± s.d.) between neighboring cells not shown). However, EMS starts to estabcalculated from the initial dye transfer data after uncaging ABp or EMS. The relative coupling strength between the AB cells was arbitrarily set to 1. lish communication with ABp and ABa. At the same time, the coupling between P2 and between AB and P1 cells (Fig. 3c). Occasionally, however, there was EMS progressively weakened as embryos develop. By the late 4-cell weak coupling between these two cells in late–2-cell embryos. In stage (characterized by the elongation of EMS, which projects addition, there was also a gradual leakage of HCC out of cells, as cellular processes around ABa), P2 is nearly uncoupled from indicated by the decay of P1 fluorescence and the increase in fluoreboth EMS and ABp. Uncaging either ABp or EMS (Fig. 5a–h and scence intensity in the extracellular space (Fig. 3c), possibly mediated Supplementary Movie 2 online) resulted in very slow dye transfer through hemichannels or nonspecific anion transporters15. to P2, but communication between ABp and EMS, ABp and ABa, The next round of cell division starts from the AB cell, followed and EMS and ABa was still strong. Consistent with these data, by the P1 cell. To define the stage of cell cycle more reliably, we uncaging P2 showed little dye transfer to ABp or EMS (Fig. 5i–l), monitored chromosome structure by fluorescence imaging using and uncaging ABa revealed the reciprocal strong coupling between GFP-tagged histone H2B as the marker (strain RW10006 (ref. 16)). AB cells and between ABa and EMS (Fig. 5m–p). We quantified the When the AB cell finishes mitosis, the division of P1 is approaching relative coupling strengths among these cells based on the initial telophase (Fig. 3e). When the cytokinesis of AB cells was complete rate of coumarin intensity increase in recipient cells (Fig. 5q). (see Supplementary Methods online for criteria used), we waited When the P2 cell divides, it generates the C and P3 cells, which for at least another 30 s before uncaging one of its daughter cells, like P2 are located at the posterior end of the developing embryo. ABp. Subsequent imaging revealed that ABa and ABp were strongly After C and P3 formed, we uncaged dextran-CANPE-HCC at the coupled, and that dye transfer reached equilibrium within approxianterior end of an embryo. HCC dye diffused rapidly across the mately 60 s. However, dye transfer between ABp and the dividing embryo. However, when it reached the P3 cell either at interphase P1 cell was much slower (Fig. 3g). or undergoing mitosis, dye diffusion into P3 cell was restricted, To compare cell coupling strength, we calculated the ratio of the suggesting that the P3 cell was weakly coupled to neighboring initial rates of coumarin intensity increase in recipient cells somatic cells throughout its life (Supplementary Movies 3 and 4 (Fig. 3g). We designed this quantification procedure to minimize online). Notably, dye transfer to the C cell appeared to be the same the effects of the initial light scattering, of the subsequent dye as transfer to other somatic cells. The division of P3 generates 2 c d FHCC (a.u.) b UV ABp 2 FHCC (a.u.) FHCC (a.u.) FHCC (a.u.) EMS 838 | VOL.5 NO.9 | SEPTEMBER 2008 | NATURE METHODS pEM AB S pP EM 2 SP2 S EM a- AB AB AB a- AB p Relative coupling strength © 2008 Nature Publishing Group http://www.nature.com/naturemethods a ARTICLES a b P2 ABp c d FHCC (a.u.) cells, P4 and D, at the posterior end in a 28cell stage embryo. Photolysis of dextranCANPE-HCC at the anterior end released HCC dye, which barely diffused into P4 and D cells (Supplementary Movie 5 online). UV 1 ABp ABa EMS P2 EMS Fdextran-HCC (a.u.) © 2008 Nature Publishing Group http://www.nature.com/naturemethods 0 40 80 120 160 0 Blastomere gap junction coupling ABa Time (s) mediates dye transfer g h 4 UV P2 To confirm that the observed cell-cell dye ABp e f ABp transfer is through gap junction channels 3 ABa rather than by other mechanisms such EMS ABp 2 P2 as cytoplasmic bridges (which allow macroP2 1 EMS EMS ABa molecules over tens of kilodaltons to 0 pass17,18), we carried out control experiABa 160 0 40 80 120 ments using 18a-glycyrrhetinic acid (aTime (s) 19 GA) , a compound that has been used to block gap junction transmission. We did Figure 6 | Cell-cell dye transfer in developing C. elegans embryos is through gap junction channels. not observe dye transfer in the presence of (a–d) DIC image (a) and coumarin fluorescence image immediately after (b) or B30 s after (c) uncaging a-GA in a cell that is normally coupled to dextran-CANPE-HCC (type 2) in ABp of a late 4-cell embryo that has been treated with bleach, chitinase and a-GA. Time course of the average HCC fluorescence intensity is plotted in d. (e–h) DIC image (e) and neighboring blastomeres (Fig. 6a–d and coumarin fluorescence immediately after (f) or B80 s after (g) UV-light uncaging of dextran-HCC-NPE Supplementary Methods). In another con- (type 1) in ABp of a late 4-cell embryo. Time course of average dextran-HCC fluorescence intensity of the trol experiment, we photolyzed dextran- bulk cytoplasm is shown in h. Dashed yellow outlines (b,f) indicate the local uncaging area. Regions of HCC-NPE (type-1 bioconjugate) to gener- interest for each cell cover the center cytoplasm of the cell, with the boundary of each region typically at ate dextran-HCC (10 kDa dextran; Fig. 1a least 2 mm away from the cell-cell contact. The results are representative of four uncaging experiments for and Supplementary Fig. 5 online). We did each condition. Scale bars, 10 mm. not expect this dextran-dye to pass through gap junction channels because its molecular weight is above the by B11 s, in the metacarpus by B30 s and it nearly filled the typical molecular exclusion limit (B1,500 Da) of connexin or entire pharynx in B100 s (Supplementary Fig. 6). During the innexin channels3,20. Indeed, we did not observe any movement of experiment, the worm was alive and showed some minor movedextran-HCC to neighboring cells after a local uncaging (Fig. 6e–h), ments sporadically (Supplementary Movie 7 online). further supporting that cell-cell transfer of free HCC in C. elegans embryos is mediated through gap junction channels. Combining Trojan-LAMP with two-photon excitation To assess potential UV-light damage to living embryos during As dextran-CANPE-HCC has high two-photon uncaging efficiency uncaging, we exposed the whole labeled embryos to UV light (Fig. 2d), and because HCC is a good fluorophore for two-photon for the same duration used for local uncaging. These embryos imaging6, we also applied the technique of two-photon excitation developed normally into adults and showed no observable to monitor cell coupling in C. elegans. We photolyzed dextranCANPE-HCC near the posterior terminal bulb of the pharynx by behavioral defects (n ¼ 10 embryos). Moreover, even when we excitation at 740 nm. Subsequent two-photon imaging of released increased the UV light dose tenfold, we still did not observe any abnormality in the embryos or in the adults (n ¼ 10 embryos). HCC by 820-nm excitation showed similar dye diffusion as UV-light uncaging experiments (Supplementary Fig. 7 online). The treated worms showed usual morphology, moved and fed normally, and laid many embryos. This suggests that the Integrating two-photon uncaging and imaging techniques would be most useful in examining cell coupling in three dimensions amount of UV light required for uncaging dextran-CANPE-HCC is well below the UV light dose that may harm cells or perturb when UV-light uncaging alone does not provide sufficient spatial selectivity to mark cells of interest. embryonic development. Imaging cell coupling in living worm larvae In both L1 and L2 stage larvae labeled with dextran-CANPE-HCC, global uncaging of the probe generated intense coumarin signal throughout the worm (Supplementary Movie 6 online). To examine dye transfer in live worms, we performed local photouncaging experiments in the pharynx, which consists of eight groups of muscle cells, pharyngeal muscles 1–8. Neighboring pharyngeal muscle cells are connected by gap junction channels21. To uncage dextran-CANPE-HCC, we focused a UV light laser (365 nm) at the posterior terminal bulb, approximately where group 7 pharyngeal muscles reside (Supplementary Fig. 6a online). Upon delivering laser pulses, HCC fluorescence immediately rose in the irradiated area and the dye rapidly spread toward the anterior of pharynx. We observed HCC throughout the isthmus DISCUSSION To study the regulation and physiological function of cell-cell communication in vivo, major technological advancements are needed in at least two areas: new methods to follow the dynamics of cell coupling in living animals and new reagents to specifically modulate cellular junctional coupling strength in physiological preparations. To establish functional correlation between cell coupling and physiology or behavior in living animals, these techniques need to be minimally invasive, yet capable of tracking or altering the dynamics of gap junction coupling with high spatiotemporal resolution over the course of a physiological measurement or a behavioral task. To address the first technical gap, we developed a new class of bioconjugates of photoactivatable dyes, the first member of which NATURE METHODS | VOL.5 NO.9 | SEPTEMBER 2008 | 839 ARTICLES strength as part of their developmental program. At 20 1C, the entire 4-cell stage P2 only lasts for about 10 min, meaning that P1 EMS EMS EMS and P2 cells maintain gap junction EMS coupling only for minutes in the early 4-cell 2-cell 3-cell Early 4-cell Mid 4-cell Late 4-cell stage. Transient coupling behavior has been Figure 7 | Dynamic gap junction communication network in early developing embryos. Strong cell-cell observed in other organisms, such as in the communication or fast dye transfer is represented by solid arrows; weak coupling or slow dye transfer is developing nervous systems of Daphnia25 or represented by dashed arrows. the leech embryo26, yet with coupling durations ranging from hours to a day. Such is dextran-CANPE-HCC. By comparison with the traditional type I temporary junctional communication has been proposed to have a bioconjugates of caged fluorophores, carrier molecules of type II role in controlling neurogenesis and in the formation of neural bioconjugates can be heavily labeled with caged dyes without circuits27. Future application of the Trojan-LAMP assay is likely to reveal other transient cell couplings during development. In addishowing self-quenching, thus maximizing the efficiency of probe tion, by using multicolor imaging and two-photon uncaging and delivery for a given amount of carrier molecules. Cell-cell communication via gap junction channels is important imaging techniques, we can correlate the dynamics of gap junction in the orderly development of multicellular organisms22. To study coupling with other biochemical or cellular processes in three the developmental importance of gap junction coupling, it would dimensions, which may offer additional insights into the role of be desirable to construct a high-resolution communication map cell coupling in development. which marks the occurrence, the strength and the dynamics of We were able to image uncaged dextran-CANPE-HCC in L1 and junctional coupling with cellular resolution over the course of 2 stage larvae, likely because of its long cellular retention and its development. Because of its limited number of cells, C. elegans is an outstanding stability in vivo. By this time, the development of several attractive system to achieve this goal. Using dextran-CANPE-HCC tissue systems is finished or nearly complete, so coupling dynamics and our new Trojan-LAMP technique, we characterized the can be characterized in many functional systems in wild-type or dynamics of dye transfer at different stages in the C. elegans embryo. mutant worms, including ones with defects in innexin expresOur experiments revealed a dynamic pattern of selective cell sion28,29. Besides C. elegans, other small organisms such as zebrafish, flies and several marine species are also appropriate models for coupling during early development (Fig. 7). Strong cell coupling is first seen between AB daughter cells and then between P1 studying gap junction coupling. As embryos of these animals only daughter cells, so an early 4-cell embryo has two communication modestly increase in size during development, the Trojan-LAMP compartments: one contains ABa and ABp, and the other contains technique may also be applicable to these systems. Also, in mamEMS and P2. By the late 4-cell stage, ABa, ABp and EMS form a malian systems, local electroporation30 may serve as an alternative approach to deliver dextran-dye conjugates to cells, possibly allowstrong communication compartment that is poorly connected with the P2 cell, the germline precursor. The weak communication ing the study of junctional cell coupling in living mammals. In addition to photoactivatable fluorophores, the concept of type between P2 and other somatic cells persisted during subsequent 2 bioconjugates of caged probes can be extended to cage other cell divisions. When the embryo developed to the 28-cell stage, D molecules such as second messengers, agonists or antagonists of and P4 were the only two cells separated from the somatic cellular receptors or ion channels. Macromolecular conjugates of communication compartment. these bioactive molecules linked through appropriate caging groups This high-resolution map of cell-cell coupling offers much more dynamic and detailed information than what was known previously would likewise have prolonged cellular retention time. This would about cell communication during the early embryogenesis of allow us to noninvasively perturb cell signaling with light in living C. elegans. In contrast to our results, another group examined animals over time. Such probes will offer new opportunities to dye transfer in C. elegans embryos by microinjection and ionto- investigate the organization, timing, interaction and function of various biochemical events in vivo. phoresis of Lucifer yellow dye, and concluded that from the 4-cell stage, all blastomeres are well coupled and that restricted dye METHODS diffusion does not start until P4 and D cells are born23. The failure to identify the transient coupling domains in early embryos could Photo-uncaging and imaging dye transfer in C. elegans. Dexbe due to technical limitations of microinjection, including low tran-CANPE-HCC (3–4.5 mM of caged HCC, kept in the dark temporal resolution or cell damage, poor quantification of dye and protected from light during use; measured by its absortransfer kinetics or coupling strength and difficulty of reliably bance at 350 nm, using e350 nm ¼ 25,000 M–1 cm–1) and injecting the dye into a cell at precise moments of development 4–5 mg/ml dextran-rhodamine (40 kDa; Sigma) were injected into gonads of young hermaphrodites. Three to four hours later, we or cell cycle. In addition, Lucifer yellow binds strongly to yolk granules in early C. elegans embryos23,24. This complicates the collected early embryos from injected worms by cutting the worms interpretation of dye diffusion data and diminishes the accuracy near the uterus. Labeled embryos were transferred onto a 2% agar and sensitivity of measuring the rate of cell-cell dye transfer. pad, covered with a coverslip and mounted on an inverted The early separation of germ-line precursor cells from the fluorescence microscope (Axiovert 200M; Carl Zeiss). During somatic cells may suggest a unique cytoplasmic characteristic uncaging and imaging, we used motorized filter wheels (Ludl important for maintaining germ-line potential. Moreover, the Electronics Products) to select excitation and emission wavelengths dramatic remodeling of the coupling pattern during early develby passing light from a xenon lamp (75 W) through bandpass opment suggests that embryos may rapidly adjust cellular coupling filters (Chroma Technology). A neutral density filter was also © 2008 Nature Publishing Group http://www.nature.com/naturemethods AB P1 ABp ABp ABa ABa ABp P2 840 | VOL.5 NO.9 | SEPTEMBER 2008 | NATURE METHODS ABa ABp P2 ABa © 2008 Nature Publishing Group http://www.nature.com/naturemethods ARTICLES added to the light path to reduce the excitation light intensity by B70%. The typical UV-light uncaging duration is B2 s. Bandpass filters were chosen for UV-light uncaging (360 ± 20 nm), coumarin imaging (excitation 425 ± 5 nm, emission 460 ± 15 nm), GFP imaging (excitation 488 ± 7.5 nm, emission 530 ± 20 nm) and rhodamine imaging (excitation 560 ± 20 nm, emission 615 ± 30 nm). A customized multiple-path dichroic mirror was used for the UV-light uncaging and three-color imaging. Epifluorescence was collected with a cooled charge-coupled device (CCD) camera (ORCA-ER; Hamamatsu) under the control of OpenLab software (Improvision). The coupling patterns at different stages of early developing embryos were representative of at least 5 uncaging experiments. Coupling between newly formed sister cells was assayed at least 30 s after the completion of cytokinesis as described in Supplementary Methods. Single-cell uncaging of dextran-CANPE-HCC in living worms was carried out with a MicroPoint laser system (Photonic Instruments) installed on the Axiovert 200M microscope, using a nitrogen UV-light laser (NL100; Stanford Research Systems) and a 2-(4-biphenylyl)-5-(4-t-butylphenyl)-1,3,4-oxadiazol (BPBD) dye cell to provide laser output at 364 nm for uncaging. When imaging worms, 1-phenoxy-2-propanol (0.1% in water) was added to the agar pad to reduce worm movement. Two-photon uncaging and imaging were performed on a LSM 510 imaging system (Carl Zeiss) equipped with a Chameleon-XR laser (Coherent)6. We typically set the laser power below 20 mW at the entrance of the scanning head as measured by a power meter (FieldMate; PM10 sensor; Coherent). The incident laser power at the specimen, estimated by placing the power meter just above the objective, was about half of the value measured at the entrance of the scan head. To uncage dextran-CANPE-HCC, we rasterscanned an area of the posterior terminal bulb at 740 nm briefly. Then, we switched the excitation wavelength to 820 nm to image HCC fluorescence by two-photon excitation. Additional methods. Details of synthesis, purification and characterization of the two types of dextran conjugates, developmental staging and blocking of dye transfer in early embryos, and quantification of the relative cell coupling strength are available in Supplementary Methods. Note: Supplementary information is available on the Nature Methods website. ACKNOWLEDGMENTS Imaging experiments involving two-photon excitation were performed at the Live Cell Imaging Core Facility of University of Texas Southwestern Medical Center and directed by K. Luby-Phelps, who also provided critical comments on the manuscript. We thank the Caenorhabditis Genetics Center for providing worm strains and X. Wang (University of Texas Southwestern) for providing the microinjection apparatus. We thank the Welch Foundation (I-1510) and the US National Institutes of Health for financial support. Published online at http://www.nature.com/naturemethods/ Reprints and permissions information is available online at http://npg.nature.com/reprintsandpermissions/ 1. Goodenough, D.A., Goliger, J.A. & Paul, D.L. Connexins, connexons, and intercellular communication. Annu. Rev. Biochem. 65, 475–502 (1996). 2. Bennett, M.V. & Zukin, R.S. Electrical coupling and neuronal synchronization in the Mammalian brain. Neuron 41, 495–511 (2004). 3. Harris, A.L. 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