A Cdc42-mediated supracellular network drives polarized forces and Drosophila egg chamber extension.

Actomyosin supracellular networks emerge during development and tissue repair. These cytoskeletal structures are able to generate large scale forces that can extensively remodel epithelia driving tissue buckling, closure and extension. How supracellular networks emerge, are controlled and mechanically work still remain elusive. During Drosophila oogenesis, the egg chamber elongates along the anterior-posterior axis. Here we show that a dorsal-ventral polarized supracellular F-actin network, running around the egg chamber on the basal side of follicle cells, emerges from polarized intercellular filopodia that radiate from basal stress fibers and extend penetrating neighboring cell cortexes. Filopodia can be mechanosensitive and function as cell-cell anchoring sites. The small GTPase Cdc42 governs the formation and distribution of intercellular filopodia and stress fibers in follicle cells. Finally, our study shows that a Cdc42-dependent supracellular cytoskeletal network provides a scaffold integrating local oscillatory actomyosin contractions at the tissue scale to drive global polarized forces and tissue elongation.

A ctomyosin networks are functionally organized in cells to generate contractile forces that drive cell shape changes. In epithelia, the architecture of actomysin networks can extend beyond the size of a single cell: this results in supracellular actomyosin structures emerging at the scale of a tissue or of the entire animal. Supracellular actomyosin networks are commonly reported in developmental processes and tissue repair during wound healing. These cytoskeletal structures provide large scale mechanical forces and can function as segregating barriers 1,2 or as mechanical actuators responsible for tissue remodeling as for example epithelial buckling 3 , closure 4,5 , and extension 6,7 . While we do have a good understanding of the molecular processes and their regulation controlling the cytoskeleton in the cell, little is known on how cellular properties and mechanics are integrated at the tissue level and finally at the animal level to give shape.
In this study, we focus on tissue extension and take advantage of a recently established model process: the elongation of the Drosophila egg chamber. The egg chamber is composed of a monolayer follicular epithelium surrounding a 16-cell germline cyst. During oogenesis, the egg chamber gradually changes its shape from round to elongated by extending along the anteriorposterior (AP) axis 8 . Tissue elongation occurs between stage 6 (S6) and S10B, and it is controlled by two distinct processes: global egg chamber fast rotation from S6 to S8 (refs. 9,10 ) and oscillating contractions of basal non-muscle myosin II (Myo-II) between S9 and S10B 11 . We here report that during S9-S10B a supracellular actomyosin network along the dorsal-ventral (DV) axis is established via polarized intercellular filopodia that interdigitate.
Filopodia are dynamic, finger-like plasma membrane protrusions of cells that act as antennae to sense the mechanical and chemical environment, and thus they are often regarded as "sensory organelles" 12,13 . Filopodia are involved in many biological processes, such as growth cone guidance, cell migration, wound closure, and macrophage-induced cell invasion [12][13][14] . These thin membrane protrusions are 60-200 nm in diameter and contain parallel bundles of 10-30 actin filaments held together by actin-binding proteins 15,16 . The formation of parallel actin bundles and filopodia is initiated by the IRSp53-mediated plasma membrane bending and the recruitment of the small GTPase Cdc42 and its downstream effectors, including ENA/ VASP, WASP/N-WASP, and mDia2 (refs. [17][18][19][20][21]. These Cdc42 effectors synergistically nucleate actin polymerization to deliver actin monomers to the filopodia tip, and thus the barbed end of the actin filaments is directed towards the protruding membrane [17][18][19][20][21] . In addition to chemical cue sensing, filopodia can probe the mechanical properties of the physical environment surrounding the cell (e.g., the extracellular matrix) [22][23][24][25][26][27][28][29][30] , and eventually apply traction forces 31,32 . Nevertheless, it is still unknown whether cells use filopodia to mechanically sense each other and if filopodia mechanosensitivity plays a role in epithelial morphogenesis. Recently, filopodia have been reported to be present between follicular epithelial cells at basal domains 9 . Nevertheless, their regulation and function are yet unknown.
By using live-cell imaging together with genetic, optogenetic, and infrared (IR) femtosecond (fs) laser manipulations, here we demonstrate that (1) stress fibers at the basal domain of the Drosophila ovarian follicular epithelial cells exert polarized contractile forces parallel to the DV axis both at the intracellular and supracellular scales; (2) intercellular filopodia, which extend towards the dorsal and ventral sides in a polarized manner, can be mechanosensitive and function as cell-cell anchoring sites between stress fiber networks, and (3) both intercellular filopodia and intracellular stress fibers are under the control of the activity of the small GTPase Cdc42. Our data support the notion that intercellular filopodia function as guiding cues organizing F-actin stress fibers parallel to the egg chamber DV axis. Finally, a Cdc42dependent supracellular F-actin network integrates local Myo-IIdependent cellular contractions to drive a global DV-polarized contraction force and AP-directed tissue elongation.

Results
Supracellular fibers emerge from interdigitating filopodia. During egg chamber elongation at S9-S10, the actin stress fibers at the basal side of follicle cells are polarized and run parallel to the DV direction 33 (Fig. 1a). Actin stress fibers are periodically distributed along the AP axis with an interval of~9 µm (as revealed by Fourier analysis in Fig. 1b and Supplementary Fig. 1) corresponding to follicle cell AP length. No periodic F-actin distribution is detected along the DV axis ( Fig. 1c and Supplementary Fig. 1). This shows that F-actin has a discrete cellular organization along the AP axis but not along the DV axis. Remarkably, a supracellular actin fiber pattern emerges along the DV axis (Fig. 1a, d). To understand how filamentous actin structures spanning multiple cells emerge, we imaged isolated clones with mCD8 membrane marker to discern the organization of F-actin in single cells along the DV axis. Actin bundles radiate from the medial stress fiber network, and they normally extend to the cell dorsal and ventral cortexes thus forming polarized protrusions (Fig. 1e). By performing live imaging of Enabled (ENA), we could confirm that these protrusions are filopodia (Supplementary Fig. 2a, b). Filopodia of opposing cells interdigitate (Fig. 1f, g) and penetrate the actomyosin cortex of the neighboring cell (Fig. 1h). As shown in previous studies 34 , E-cadherin based junctions are present at the sub-basal cortex including along the filopodia (Fig. 1i). While actin bundles extend from medial stress fibers to the sub-basal cell-cell contact zone forming filopodia, Myo-II is not enriched at this zone and concentrates instead in the medial region (Fig. 1j).
During stages 7-8, filopodia at the basal side of follicle cells are unidirectionally polarized along the DV axis, following the orientation of egg chamber rotation 9 . After egg chamber rotation arrests at the end of S8, filopodia gradually increase their length and become bidirectionally polarized; they reach their maximal length between middle and late S9, and then shorten in S10B ( Supplementary Fig. 2c).
To summarize, at S9 a supracellular F-actin network parallel to the DV axis emerges from bidirectionally polarized filopodia that interdigitate and penetrate the actomyosin cortex of opposing cells ( Supplementary Fig. 2d).
Cdc42 controls filopodia and stress fiber formation. It is known that filopodia formation is under the control of the Rho-family small GTPase Cdc42 (refs. 19,20 ). We, therefore, assessed whether Cdc42 is involved in the control of intercellular filopodia in follicle cells. Firstly, we examined the localization of the Cdc42 protein which, like Rac1 and Rho1 proteins, appeared to be enriched at the sub-basal cell-cell contact zone of follicle cells ( Fig. 2a and Supplementary Fig. 3a, b). Chemical and genetic inhibition of Cdc42 activity, but not Rac1 or Rho1 activity, reduced filopodia length (Fig. 2b, c and Supplementary Fig. 3c-f, h, i) and also affected the filopodia directionality ( Supplementary  Fig. 4). The inhibition of Cdc42 activity by its dominant-negative (DN) form or by the loss-of-function (LOF) mutation 35 also decreased the intensity and changed the central/lateral distribution of the basal actomyosin network (Fig. 2b, d-g and Supplementary Fig. 3h, j). In contrast, the inhibition of Rac1 or Rho1 activity did not affect the distribution of the medio-basal actomyosin network ( Supplementary Fig. 3e, g). Furthermore, basal Myo-II periodic oscillations were still present with smaller amplitude in cells with reduced Cdc42 activity in contrast to cells expressing Rho1DN (Fig. 2h, i and Supplementary Movies 1-3). These results show that Cdc42 is required for filopodia formation and to organize the basal actomyosin network whereas Rho1 controls the medial actomyosin oscillations.
Cdc42 effectors control both stress fibers and filopodia. To further investigate the role of Cdc42 in filopodia and stress fiber formation, we tested three Cdc42 downstream effectors: WASP, Enabled, and Dia [18][19][20] .
RNAi inhibition of each effector resulted in similar phenotypes, as observed in Cdc42 downregulation experiments: (1) filopodia length reduction (Fig. 3a, b), (2) basal Myo-II intensity decrease (Fig. 3a, c), and (3) central/lateral redistribution of stress fibers (Fig. 3a, d). Next, we characterized the effect of Cdc42 inhibition on these effectors. Cdc42 activity inhibition by its DN form strongly reduced the medio-basal distribution of all effectors, compared to wild-type cells (Fig. 3e-h). Moreover, concurrent expression of Enabled and Cdc42DN recovered the basal F-actin distribution and also returned the filopodia length back to normal ( Fig. 3i-k). Similarly, significant but weaker recovery effects were observed when either WASP or Dia was concurrently expressed with Cdc42DN ( Supplementary Fig. 5).
Finally, our data corroborate the notion that Cdc42 signaling controls filopodia formation and the organization of medio-basal stress fibers.   Supplementary Fig. 6a). We produced transgenic flies expressing PA-Cdc42 in the constitutively-active (CA) or DN form and a light-insensitive control in which the C450M mutation stabilizes the dark-state conformation of LOV2 (refs. 36,37 ). For either the PA-Cdc42CA or PA-Cdc42DN form, exposure to blue light was able to significantly increase or decrease, respectively, the accumulation of PAK1-RBD-GFP at the basal cortical domain of follicle cells compared to the dark conditions ( Supplementary Fig. 6b, c). Furthermore, compared with the C450M light-insensitive control, expression of PA-Cdc42DN in dark condition led to little effect on basal Myo-II and F-actin signals ( Supplementary Fig. 6d, e). Taken together, these results demonstrate the effectiveness of PA-Cdc42CA and PA-Cdc42DN in vivo. First, we tested the effect of Cdc42 photo-inhibition on intercellular filopodia in follicle cells at late S9 and S10A. The inhibition of Cdc42 activity by light reduced the length of filopodia within 10 min (Fig. 4b, c). Subsequently, we checked the effect of Cdc42 photo-inhibition on the basal actomyosin network of follicle cells at late S9 and S10A. Light-induced inhibition of Cdc42 activity gradually decreased the medio-basal distribution of F-actin and Myo-II signals within 20-30 min (Fig. 4d, e and Supplementary Movies 4 and 6). The C450M light-insensitive control caused no significant effect (Fig. 4d, e, Supplementary  Fig. 7a, b and Supplementary Movies 5 and 7). In addition, the activation of PA-Cdc42DN at the apical domain had no prominent effect on basal stress fibers ( Supplementary Fig. 7c-e). This demonstrates that stress fibers are under the control of basal Cdc42 activity.
Furthermore, we confirmed that Cdc42 photoactivation restores stress fiber formation in Cdc42-LOF mutant follicle cells. In these mutant cells, basal stress fibers are severely disrupted and misaligned. However, the activation of PA-Cdc42CA by light significantly recovered the formation and distribution of stress fibers within the medio-basal region in a short time period (Fig. 4f, g). Finally, PA-Cdc42CA activation in Cdc42-LOF mutant clones rescued filopodia length, while C450M light-insensitive control caused no significant effect (Supplementary Fig. 7f, g).
Finally, these results further support Cdc42 spatiotemporal control over filopodia and stress fibers.
Cdc42 non-cell autonomous role in stress fiber organization. Since intercellular filopodia, which extend in a polarized manner along the DV axis and penetrate the neighboring cell cortex, are under the control of Cdc42, we tested whether Cdc42 plays a non-cell autonomous role in stress fiber organization. Three cell categories can be defined in follicular epithelial tissues containing Cdc42DN clones: (1) clone cells, (2) cells neighboring clone cells, and (3) cells not neighboring clone cells. While cells not neighboring Cdc42DN clones show the normal stress fiber distribution parallel to the DV axis, both clones and clone neighbors showed stress fiber mis-organization (Fig. 5a, b and Supplementary  Fig. 8e). Cdc42DN clones and clone neighbors also showed the redistribution of the actin bundles (lateral vs. medial, e.g., Fig. 2d and Supplementary Fig. 8c, d). This led us to ask whether this local non-cell autonomous effect was due to reduced Myo-II contractility (hypothesis 1) or to the loss of intercellular filopodia (hypothesis 2), both being mediated by the inhibition of Cdc42 activity. To test the first hypothesis, we specifically reduced actomyosin contractility by interfering with the Rho1 pathway. The inhibition of Rho1 or ROCK activity in clone cells had no major effect on the neighboring and more distant wild-type cells, thus ruling out the first hypothesis (Supplementary Fig. 8 and ref. 11 ). To test the second hypothesis, we took advantage of the PA-Cdc42DN optogenetic construct that allows spatiotemporal specific Cdc42 inhibition. We specifically photoactivated the subbasal cell-cell contact zone of PA-Cdc42DN clone cells from which the filopodia radiate and monitored stress fiber organization in a neighboring wild-type cell (Fig. 5c). During photoactivation, filopodia of photoactivated Cdc42DN clones retracted and the actomyosin medial network of the neighboring wild-type cell was disrupted (Fig. 5d-i). Photoactivation had no effect on the light-insensitive control PA-Cdc42DN C450M cells (Supplementary Fig. 9). Finally, this shows that Cdc42 plays a non-cell autonomous role in stress fiber organization that could be mediated by intracellular filopodia.
Cortical tension anisotropy is under the control of Cdc42. Basal actomyosin contractility drives tissue elongation 11 . While it is known that basal Myo-II contractility is necessary to reduce basal cell area in a polarized manner along the DV axis 11 , cell basal tension anisotropy has never been tested directly. We implemented IR fs laser ablation to dissect the actomyosin cytoskeleton    Cdc42 controls supracellular tension and tissue elongation. We have demonstrated that at S9-S10 follicle stress fibers generate DV-polarized contractile forces at the cellular scale ( Fig. 6) while fiber actin structures, resulting from the stress fibers and filopodia intermingling, emerge at the supracellular scale (Fig. 1). We therefore wondered if polarized supracellular forces are acting on the follicular epithelium. To test this, we used IR laser ablation and dissected the basal actomyosin network over a 100 µm line (about ten cells). If forces are only acting at the cellular scale, multiple local recoils of the actomysin network would occur (a recoil for each ablated cell network). If supracellular forces emerge from the interaction of local contractile units, a global recoil at higher speed would be expected. Upon ablation along a line parallel to the AP direction, the basal network recoiled along the DV axis with a maximum speed of 0,76 µm s −1 on average. The recoil resulted in one single large opening in the basal network (Fig. 7a, d and Supplementary Movie 11). This demonstrates that a supracellular force is acting at the level of the follicular epithelium and that this is >3 times greater than the contractile force acting at the cellular scale. Ablation along the DV axis resulted in a much slower recoil (0,07 µm s −1 maximum speed on average) compared to AP (Fig. 7b, d and Supplementary Movie 12), showing that tension anisotropy is also established at the tissue scale. IR fs laser ablation has been demonstrated to be capable of high-resolved dissection of the actomyosin network with little or no perturbation of the cell membrane 38,40 . Our experiments corroborate this notion: membranes are preserved since they (i) are visible after ablation and (ii) stretch under the action of tissue scale unbalanced forces ( Fig. 7a and Supplementary Movie 11). These observations suggest that cell unities are preserved after IR fs tissue scale dissection.
Tissue scale IR fs ablation results in the dissection of the basal network, including both the medial-basal actomyosin stress fibers and the basal junctional F-actin network that is not enriched with Myo-II (Fig. 1j). In order to specifically probe the medial-basal actomyosin stress fibers network (which is the focus of our study), we performed a tissue scale segmented ablation to dissect the actomyosin stress fibers while avoiding the sub-basal cell-cell contact zones (probed already in a previous study 41 ). The tissue scale segmented ablation still resulted in one single large opening (see Supplementary Movie 13). In addition, network recoil maximum speed after segmented dissection was >3-fold greater than after single cell network dissection ( Supplementary Fig. 11). These evidences show that egg-chamber surface mechanics, during stage 10, is dominated by polarized supracellular tension generated by the medial-basal actomyosin stress fiber network.
We further tested tissue scale forces in follicular epithelia containing large Cdc42DN clones. Under these conditions, tension was drastically reduced along the DV axis as observed in subcellular dissection experiments (Fig. 7c, d). Therefore, we assessed the effect of Cdc42 inhibition on tissue shape. Egg chambers containing clones of Cdc42 mutant cells were significantly more round-shaped than wild type (Fig. 7e, f). This round egg chamber shape was mainly due to the Cdc42-LOF in follicle cells, since the expression of Cdc42DN specifically in follicle cells resulted in an equally strong phenotype (Fig. 7e, f) despite no apical-basal polarity loss nor any egg chamber rotation defects ( Supplementary Fig. 12). These results show that DVpolarized supracellular tension and AP-directed global tissue elongation are under the control of Cdc42.
To further investigate the role of filopodia in establishing a functional supracellular contractile network, we probed filopodia mechanosensitivity and mechanical function. Firstly we performed IR nano-dissection of stress fibers juxtaposed to filopodia: this induced stress fiber tension release and filopodia retraction ( Fig. 7g white arrowhead, h). Remarkably, filopodia juxtaposed to preserved stress fibers did not retract ( Fig. 7g yellow arrowhead,  h). This data shows that filopodia in follicle cells are tension sensitive. We next aimed to test whether filopodia are mechanically coupled to neighboring cell cortexes. To test this, we performed a supracellular laser dissection parallel to the AP direction intersecting a filopodium (Fig. 7i first panel). The hypothesis supposing a strong mechanical coupling between the filopodium and the neighboring cell cortex can be ruled out if, during recoil, the filopodium tip were to move following the displacement of the cell from which it radiates. Remarkably, after dissection, the filopodium tip moved away from the cell that it belonged to: this resulted in filopodium stretching ( Fig. 7i and Supplementary Movie 14). After persisting in a stretch configuration for several minutes, the stretched filopodium partially retracted as the tip finally moved back in a way that was similar to a spring that, under load, has been stretched out and then suddenly released from one extremity (Fig. 7i last panel and  Supplementary Movie 14). This directly demonstrates that filopodia can be coupled to neighboring cells, thus functioning as mechanical anchors and establishing the bridging links between cell cortexes. In contrast to other epithelial cells, in which Myo-II is enriched at junctions generating forces that are directly transmitted from cell to cell 38,42 , in follicle cells Myo-II is not enriched at basal junctions and concentrates instead in the medial region. How can then forces be transmitted from one cell to the other at the basal domain in the follicular epithelium? Here, we show that filopodia, bridging basal networks to establish F-actin supracellular patterns, can be mechanosensitive and anchored to neighboring actomyosin cortexes presumably via E-cadherin mediated adherens junctions. Filopodia could thus function as cell-cell coupling units. While previous work has shown that actomyosin stress fiber organization is not affected in integrin downregulated follicular epithelia 34 , further work is necessary to rule out the possibility that the extracellular matrix may also function as a scaffold integrating stress fiber contractions during S9.
Our work demonstrates that Cdc42 has a non-cell autonomous role in stress fiber organization. By inhibiting Cdc42, specifically at the sub-basal cell-cell contact zone of PA-Cdc42DN clones, we show that filopodia retract and that stress fibers of neighboring wild-type cells are mis-organized within a time period of tens of minutes. This suggests that filopodia could function also as guiding cues to organize stress fibers. A recent study shows that engulfed cadherin "fingers" are asymmetrically distributed between endothelial cells to maintain actomyosin network polarity during collective cell migration 43 . These findings delineate a functioning mode in which thin protrusions might commonly serve to coordinate the collective behaviors of cell sheets.
During the early stages of Drosophila oogenesis, global egg chamber rotation polarizes (1) the extracellular matrix, (2) the intracellular basal F-actin network, and (3) the filopodia (the latter in a unidirectional manner) 9,10,44,45 . When rotation is arrested at early S9, filopodia maintain a DV polarity but become bidirectional penetrating the cortexes of dorsally and ventrally positioned neighboring cells. As egg chamber development proceeds, stress fibers become densely packed and more aligned while filopodia retract beginning at S10B. While during S9 and S10A, bidirectional filopodia might provide a physical cue to guide stress fibers and to stabilize their DV polarity, filopodia might become dispensable in later stages after stress fiber maturation. Filopodia bidirectional polarity might be under the control of the prepolarized extracellular matrix. Further work is necessary to better understand the origin of bidirectionally polarized filopodia.
Finally, we show that actomyosin stress fiber dynamics and organization are separately controlled. While Rho1-ROCK signaling controls basal Myo-II oscillations (as also shown in previous work 11,34,46 ), Cdc42 controls stress fiber distribution. While both levels of control are necessary for tissue extension, future work is needed to better understand the role and mechanics of Myo-II periodic oscillations acting at the cell scale and of Myo-II phase waves propagating along the egg chamber.

Methods
Drosophila stocks and genetics. The following fly stocks were used (information is listed in Supplementary Table 1 All stocks and crosses were maintained at room temperature. For signal analysis in mosaic tissues, hsFLPase was induced twice, for 1 h at 37°C, with a 5-h interval, then flies were kept at 18°C for 2 days and then fattened at 25°C overnight before dissection. For the analysis of tissue elongation, P [hsp70-flp]; +/+; Ay(CD2)Gal4 was used for cross and later heat shock treatment, which can induce more than 90% clone cells in the egg chamber. hsFLPase of this mosaic system was induced for 1 h at 37°C once, then flies were kept at 18°C for 1-2 days and then fattened at 25°C for overnight before dissection. For follicle rotation, P[hsp70-flp]; UAS-dsRed; Ay(CD2)Gal4 was used for cross and later heat shock treatment, which can induce more than 90% clone cells in the egg chamber. hsFLPase of this mosaic system was induced for 1 h at 37°C once, then flies were fattened at 25°C overnight before dissection in order to achieve the moderate expression of Cdc42DN without the disruption of apical/basolateral polarity of follicle cells. For MARCM experiments of the global tissue elongation or the analysis of F-actin/myosin subcellular distribution, flies with the genetic backgrounds (either: cdc42 [4] P{neoFRT}19A/P{hsFLP}1, P{tubP-GAL80}LL1 P{neoFRT}19A; tubGal4 UAS-mCD8GFP or: cdc42 [4] P{neoFRT}19A/P{hsFLP}1, P{tubP-GAL80}LL1 P{neoFRT}19A; tubGal4 mCD8GFP/Sqh:: RLCmyosinII-mCherry) were used. P{neoFRT}19A/P{hsFLP}1, P{tubP-GAL80}LL1 P{neoFRT}1A; tubGal4 mCD8GFP flies were used as a control. hsFLPase was induced five times for 1 h at 37°C over 2 days, flies were kept at 18°C for 4-5 days and then fattened at 25°C overnight before dissection.  [4] p{neoFRT}19A/P{hsFLP}1, P{tubP-GAL80}LL1 P{neoFRT}19A; tubGAL4, UAS-mCD8GFP was used for cross with UAS-PA-Cdc42CA or UAS-PA-Cdc42CA C450M transgenic fly. hsFLPase was induced four times for 1 h at 37°C over 2 days, then flies were kept at 18°C for 2 days and then fattened at 25°C overnight before dissection. All steps were carried on in dark conditions, including cross, maintenance, and heat shock, as for PA-Cdc42DN experiments. Drosophila ovaries were dissected in weak light conditions, and egg chambers were mounted under red light condition before blue light illumination.
DNA constructs and transgenic fly generation. N-terminal-mCherry-tagged PA-Cdc42CA (Q79L/E91H/N92H), PA-Cdc42DN (T17N) and the light-insensitive controlPA-Cdc42CA C450M and PA-Cdc42DN C450M were inserted into the pUASt Drosophila expression vector using the Gateway recombination system Fig. 4 Optogenetics reveal specific spatial and temporal control of Cdc42. a Schematic diagram showing the mechanism of PA-Cdc42 photoactivation by blue light (hv). b, d, e, f, g. Time-lapse series of representative mCherry-tagged PA -Cdc42DN-expressing (b, d, e) and mCherry-tagged PA-Cdc42CAexpressing follicle cell with cdc42 [4] mutant genetic background (f, g), labeled with mCD8GFP (b), MyoII-GFP (d, f) and UtrABD-GFP (e, g). PA indicates the time of photoactivation. Arrow heads indicate filopodia in b. c Average filopodia length per cell (from seven egg chambers) in the n individual PA-Cdc42DN clone cells before and 10-15 min after photoactivation. p = 0.0099 by two-sided Mann-Whitney test. d, e, f, g (central panel). Relative (central/ lateral) distribution over time of MyoII (d, f) and F-actin (e, g) for a representative case in the indicated genetic backgrounds. d, e, f, g (right panel). Relative (central/lateral) distribution of MyoII (d, f) and F-actin (e, g) before and 25-30 min after photoactivation in the n individual cells under the indicated genetic backgrounds. For MyoII signal, the PA-Cdc42DN before-vs. after-photoactivation comparison: p < 0.0001, the PA-Cdc42DN C450M before-and after-photoactivation comparison: p = 0.7107; for F-actin signal, the PA-Cdc42DN before-vs. after-photoactivation comparison: p = 0.0005, the PA-Cdc42DN C450M before-and after-photoactivation comparison: p = 0.972; for MyoII signal, the PA-Cdc42CA before-vs. after-photoactivation comparison: p = 0.0022; for F-actin signal, the PA-Cdc42CA before-vs. after-photoactivation comparison: p = 0.0006; all by two-sided Mann-Whitney test. Data are presented as mean values +/− SEM. Scale bars are 5 μm in b, d, e, f, g.  Dissection and mounting of the Drosophila egg chamber. One-to three-day-old females were fattened on yeast with males for 1-2 days before dissection. Drosophila egg chambers were dissected and mounted in live-imaging medium (Invitrogen Schneider's insect medium with 20% FBS and with a final PH adjusted to 6.9), using a similar version of the protocol described in ref. 50 . In contrast to the normal mounting conditions, egg chambers were slightly compressed to overcome the endogenous curvature. Under this condition, basal oscillation pattern, intensity and period were similar to those observed under conditions without compression.
GST pulldown. The assay of Cdc42 activity in cell lysates was performed as described in ref. 51 . Briefly, the p21-binding domain (PBD) domain from PAK1 was subcloned into pGEX-4T1 vector and expressed as an N-terminal GST fusion protein in BL21(DE3) competent E. coli (New England BioLabs). GST-PDB was purified from bacterial lysates using glutathione magnetic beads (Thermo-Scientific). The PA-Cdc42 lit state mutant (I531E/I539E) or dark-state mutant (C450A, L514K, G528A, L531E, N538E) were expressed in HEK293 cells via transient transfection with Fugene6 (Promega). HEK293 cell line was from Genetica, MA, USA, and it was not authenticated. This cell line has been regularly tested negative for Mycoplasma contamination. Lysates from HEK293 cells were incubated with~10 μg of GST-PDB beads and incubated at 4°C for 1 h. Following incubation, beads were washed, boiled with sample buffer, and analyzed via western blot.
Imaging and photomanipulation. Time-lapse imaging was performed with a Zeiss LSM710 or Leica SP8 confocal microscope with a 40×, numerical aperture 1.3 inverted oil lens, with a 488 nm argon laser and a 561 nm green laser in LSM710 or a 552 nm laser in SP8. The basal focal plane, which is about 1 μm beneath the basal surface inside the cell, was selected during live imaging to maximize the basal Myo-II intensity. For the dynamics of UtrABD-GFP, the similar basal focal plane was selected to maximize the basal F-actin intensity, as for basal Myo-II dynamic imaging. The same microscope setup was used when comparing intensity between different samples. For the dynamics of follicle cell rotational movement, the focal plane, which is centered at follicle cell nuclei, was selected to maximize the nuclear dsRed to better view the localization of individual follicle cells. Imaging data have been collected by Zeiss Zen software (version: Zen 2007 light edition) or Leica Metamorph software (version: Metamorph 7.8.13.0) or Leica SP8 LAS software (version: LAS X).
For photoactivation experiment, live-cell imaging was performed using a Zeiss LSM710 confocal microscope with a 40×, numerical aperture 1.3 inverted oil lens, with a 488 nm argon laser and a 561 nm green laser. To photoactivate, the 458 nm laser was set at 6-8% power for 0.1 ms per pixel in a 5-15 μm circle or rectangle and the photoactivation scan took~15-20 s. After 30 s, follicle cells were imaged using 488 or 568 nm. This series of steps was repeated for the duration of the timelapse experiment.
Drug treatments. Egg chambers were dissected in live-imaging medium, and then incubated with Cdc42 inhibitor ML141 52 (Sigma) at 400 μM, Rac inhibitor NSC23766 53 (Sigma) at 400 μM, Rho1 inhibitor Rhosin 54 (Merk) at 400 μM for 20 min before being mounted for imaging. Information of chemical inhibitors is listed in Supplementary Table 2.
Image processing and data analysis. Images were processed with MATLAB (version: R2018a) and Image J (version: 1.51j8). For all images the background (intensity of area without sample) was subtracted.
Image J was used to calculate the intensity of an individual cell as the average value of all pixels within the cell area. In the time-lapse experiments, images were processed by MATLAB to correct photo-bleaching automatically. To determine the signal ratio between the medio-basal region and the outside region close to basal junction, each follicle cell was separated into these two regions (one is medio-basal cortex, which is around 1/2 at center region, while the other is around 1/4 regions near both anterior and posterior junctional membrane), and then the signals in either region were analyzed using ImageJ.
For the quantification of egg chamber rotation, the rotation speed of follicle cells was measured from the time-lapse images of S6-S7 egg chambers expressing nuclear dsRed driven by FLP-OUT system. The time-lapse positions of individual follicle cell nuclear centers were automatically tracked by MATLAB and the migration speed was automatically calculated also by MATLAB. Migration speed (each dot in Supplementary Fig. 12c) was obtained from the average of each follicle cell nuclear movement in the same egg chamber.
The distribution of oscillation periods was generated by measuring the intervals between each pair of adjacent peaks. We applied autocorrelation to calculate the period of a time series with different time offsets. This method averages out irregularities in the sequence and gives a similar average period. To quantify the percentage distribution of the oscillating time period, the 25 to 30 minute-dynamic intensity of the n individual cells (n is indicated in Fig. 2i) from four independent LS9 egg chambers was tracked, then the oscillating cycle time of each individual cell was calculated by the autocorrelation method.
Tissue elongation was measured by the A-P to D-V length ratio of S10 and S14 egg chambers.
For the quantification of the planar cell polarity of stress fibers in follicle cells, we calculated the order parameter, S, for the mutant clone, neighboring WT and far WT follicle cells (three categories of follicle cells) in egg chambers, by a similar version of the protocol described in ref. 9 . We defined S as: S = 2(<cos 2 (θ ij )> -1/2), where θ ij is the angle between the directors of cells i and j. The average was performed over all unique cell pair combinations in each category of follicle cells.
Box and whiskers plots (GraphPad Prism software) were used to represent the filopodia length and distribution as well as stress fiber orientation, and also the data with sample number >10: boxes extend from the 25th to 75th percentiles, the mid line represents the median and the whiskers indicate the maximum and the minimum values. GraphPad Prism software (version: 8.0.1) has been used for box and whiskers plots.
For filopodia length analysis, the average filopodia length per cell was quantified. For each analyzed individual cell, all filopodia not <0.5 µm were measured.
Ablation experiments. Ablations of basal actomyosin stress fibers were performed using a 780 NLO (Zeiss) inverted confocal microscope, equipped with the Spectra-Physics Mai Tai DeepSee IR fs laser (Newport Corp., Irvine, CA, UAS), using 40×/ N.A. 1.2 water-immersion objective (ZeissC-Apo 421767-9970). Ablations were obtained by exposing the fibers to the focused beam with an average power of 200 mW (at 950 nm with 90% transmission) measured on the focal plane of the objective using a thermic slide-photoreceptor. IR fs laser dissections were performed using FRAP function of ZEN software. The region of interest (ROI) was always set to a horizontal line (the egg chamber was thus digitally rotated accordingly for AP or DV ablations). The frame rate is constant regardless of the length of the ROI. Images were acquired in mono-photon mode, using an Argon laser (488 nm) and DPSS 561 nm.  expressing (a, b) and expressing (c, d) the Cdc42DN transgene marked by mCD8GFP coexpression, before (panel on the left) and after ablation (indicated by the dashed line) of the basal actomyosin network along the AP (a, c) and the DV (b, d) axes. MyoII is visualized by using a MyoII-mCherry construct. Right panel: kymographs illustrating network recoil along the DV (a, c) and the AP (b, d) axes after ablation. The results shown in a-d have been successfully repeated from the at least four independent experiments. e Maximum recoil speed after ablations in the n individual control (only mCD8GFP expressing) and Cdc42DN clones. For the control DV vs. AP comparison: p < 0.0001; for the Cdc42DN DV vs. AP comparison: p = 0.0788; both by two-sided Mann-Whitney test. f, g Timelapse series of a representative wild-type cell, neighboring (f) or distantly located (g) from Cdc42DN-expressing clones, before and after ablation (indicated by the dashed line) of the actomyosin network along the AP axis. Right panel: kymographs illustrating network recoil after ablation. The results shown in f, g have been successfully repeated from the at least four independent experiments. h Maximum recoil speed after ablations in the n individual wild-type cells that are neighboring or distantly located from Cdc42DN-expressing clones. p < 0.0001 by two-sided Mann-Whitney test. Data are presented as mean values +/− SEM. Scale bars are 5 μm in a, b, c, d, f, g.
Measurements of the maximum recoil speed were performed with Fiji software, using the particle image velocimetry (PIV) plugin 55 . For each ablation event, the velocity vector field was determined by PIV between the pre-cut frame and an image 2 s post-cut. The maximum recoil speed was estimated from the velocity vector field as for the average velocity component orthogonal to the cut line.
Reporting summary. Further information on research design is available in the Nature Research Reporting Summary linked to this article.

Data availability
The data sets generated during and/or analyzed during the current study are available from the corresponding author on request. The source data underlying Figs. 2c, f, g, 3b-d, h, j, k, 4c-g, 5b, e, g, i, 6e, h, 7d and f, Supplementary Figs. 3d, f, g, i, j, 4a, b, 5b, c, 6c, e, 7b, d, e, g, 8b, d, e, 9c, e, g, 10d, 11, and 12c are provided as a Source Data file.

Code availability
The codes used for analyses of different images are available from the corresponding author on request.