Rac1 activation can generate untemplated, lamellar membrane ruffles

Membrane protrusions that occur on the dorsal surface of a cell are an excellent experimental system to study actin machinery at work in a living cell. Small GTPase Rac1 controls the membrane protrusions that form and encapsulate extracellular volumes to perform pinocytic or phagocytic functions. Here, capitalizing on rapid volumetric imaging capabilities of lattice light-sheet microscopy (LLSM), we describe optogenetic approaches using photoactivable Rac1 (PA-Rac1) for controlled ruffle generation. We demonstrate that PA-Rac1 activation needs to be continuous, suggesting a threshold local concentration for sustained actin polymerization leading to ruffling. We show that Rac1 activation leads to actin assembly at the dorsal surface of the cell membrane that result in sheet-like protrusion formation without any requirement of a template. Further, this approach can be used to study the complex morpho-dynamics of the protrusions or to investigate specific proteins that may be enriched in the ruffles. Deactivating PA-Rac1 leads to complex contractile processes resulting in formation of macropinosomes. Using multicolour imaging in combination with these approaches, we find that Myo1e specifically is enriched in the ruffles. Combining LLSM and optogenetics enables superior spatial and temporal control for studying such dynamic mechanisms. Demonstrated here, the techniques implemented provide insight into the complex nature of the molecular interplay involved in dynamic actin machinery, revealing that Rac1 activation can generate untemplated, lamellar protrusions.

the complex membrane ruffling and closure required to form macropinosomes. Several studies have described the role of Rac1 in the formation of membrane ruffles and macropinosomes. Expression of the inactive mutant of Rac1 (Rac1T17N) inhibits macropinosomes, whereas the dominant active mutant (Rac1G12V) stimulates macropinosomes [11,12]. Indirect aggravation of Rac1 activity through constitutively active p21-acivated kinase induces macropinosome formation [13]. The elucidation of activities regulating Rac1 was furthered by photoactivable Rac1 (PA-Rac1), a light-sensitive version of Rac1, created by fusing constitutively active Rac1Q61L with the light oxygen voltage (LOV) domain and the carboxyterminal helical extension of phototropin 1 [14,15]. PA-Rac1 was used to decipher the role of activation and deactivation of Rac1. PA-Rac1 expressed in Raw264 macrophages induced membrane ruffling and macropinocytic cup formation [16]. They further demonstrate that deactivation of Rac1 is crucial for the progress of pinocytic cup closure. In line with this model of Rac1 switching, in the structurally analogous process of phagocytosis, Ikeda et al. show that Rac1 switching at the correct spatio-temporal instance is necessary for phagosome formation [17]. In general, the phagosome or macropinosome formation can be simplified into a two-step process-the first step of extending the membrane protrusion three-dimensionally, and the second step of engulfment/wrapping around leading to closure. All the previous evidence of Rac1 being constitutively active leading to defects in the closure of macropinocytic or phagocytic cups suggests that Rac1 switching is necessary to switch from the growth phase to engulfment and closure phase. Recently, Fritz-Laylin et al. used LLSM to image neutrophil-like HL-60 cells and found two important aspects of lamellar protrusions that formed in the absence of any substrate interactions: (1) free standing lamellae combine to give rise to complex geometries that are essentially lamellar and (2) lamellar protrusions do not require any 'surface template' [18].
Investigating the morphodynamics of membrane protrusions formed on the dorsal surface of the cell is challenging. Despite the accumulation of much data on the phenomenology of membrane lamellipodial and ruffle formation, it has been difficult to image the membrane ruffles formed at the dorsal surface of the cell. All these characteristics demand imaging techniques to be capable of acquiring rapid volumetric imaging that minimize photo-bleaching effects. In the present report, we set out to use lattice light-sheet microscopy (LLSM) in combination with optogenetics to investigate PA-Rac1-mediated membrane protrusions on the dorsal surface and investigate the spatio-temporal events leading to Rac1 activation cycling-mediated macropinosome formation. An optogenetic approach, in which a photo-activatable chimeric construct alters to near-native functionality upon activation by light, is valuable to study such protein-based switches in complex protein machinery systems, and in combination with lattice light sheet that enables fast, volumetric live cell imaging, it becomes a powerful tool to investigate the processes on the dorsal membrane of the cell. Using this experimental system, we demonstrate that: 1. Continuous activation of PA-Rac1 is required for effective ruffle formation on dorsal surface; sequential photoactivation re-initiates polymerization-induced growth of pre-formed ruffles. 2. PA-Rac1-based ruffles are intrinsically sheet-like and can be generated spontaneously on the dorsal surface or can lift-off from lamellipodia attached to substrate. 3. Optogenetic stimulation of PA-Rac1 allows characterizing various morphodynamical features as well as ruffle-associated proteins.

Continuous activation of Rac1 activity is required for effective ruffle formation
To visualize dorsal membrane ruffling on-demand, we imaged human retinal pigmented epithelial (RPE1) cells transiently transfected with pTriExmCherry PA-Rac1 as previously described [15,16]. We used RPE-1 cells as they have been used extensively for studying macropinosome formation as well as membrane ruffling [19]. This approach enabled us to optogenetically activate Rac1 signalling and induce dorsal ruffling of the membrane in RPE-1 cells as well as allowing us to visualize this process using fluorescence imaging. To visualize the dynamic and transient Rac1 ruffles on the dorsal surface of live cells, we resorted to lattice light-sheet microscopy [20], which provides rapid and photo-gentle volumetric imaging at near diffraction limited resolution (Fig. 1a).
To produce precise temporal activation of PA-Rac1, we attempted two strategies of optogenetic excitation. We attempted to activate PA-Rac1 using a 445-nm laser passing through the spatial light modulator and excitation objective to produce a 'full length' or 'quarter length' multi-bessel beam excitation profile (Fig. 1b, c). While spatial precision could be achieved in specific regions of the cell using protein constructs that display direct activity such as photoconversions (data not shown) or more complex process exemplified by lightinduced oligomerization of Cry2-Olig mCherry (Additional file 1: Movie S1), we did not observe any induced ruffling processes using this approach (Fig. 1d). We attributed this to the fact that such SLM-based photoactivation is discontinuous over the volume of the cell, as molecules are only activated at that instance when they are in the imaging plane and not during the scanning of the entire volume. As a volume is scanned and the excitation plane coincides again, the time-gap is equivalent to the time required for the capture of the entire volume at best. Therefore, where a single plane is only exposed for 40 ms as a typical example (exposure time of the camera) while the time for one volume is 4 s (for 100 planes) results in discontinuous excitation. The absence of ruffling under this excitation mode may suggest a time-based limitation manifesting as a result of insufficient local concentration of activated PA-Rac1 to generate ruffles (see the 'Discussion' section) (Fig. 1c). Therefore, despite being not well understood, the widely acknowledged presence of complex processes which occur downstream of Rac1 activation [21] suggests that this time-based limitation we observe is not solely governed by insufficient Rac1 activation, but a combination of activated Rac1 reaching a threshold concentration and then subsequently allowing sufficient time for further downstream processes to occur, crucial for ruffles c Schematic representation of optogenetic excitation using the SLM to produce controlled 445-nm excitation, shown in right panel. Using the SLM in the excitation path results in discontinuous excitation. d RPE1 cell stimulated using SLM-based excitation (as described in c) of PA-Rac1 does not suppress filopodia (red arrows) and no ruffles are observed. Scale bar = 5 μm. e Schematic representation of wide-field optogenetic excitation passed through the detection objective leading to continuous excitation, shown in right panel. f Dorsal membrane ruffles (magenta arrows) and increased protrusion along the coverslip (green arrows) produced following wide-field optogenetic stimulation (as described in e). Scale bar = 10 μm. g Growth of PA-Rac1 ruffles in response to photoactivation. Scale bar = 3 μm. h Boxplot of PA-Rac1 ruffle length (μm) vs photoactivation laser power (mW). Outer range shows total range, box height shows the standard deviation, and inner bar shows mean (n = 45 ruffles) to form. Further, Fritz-Laylin et al. [18] propose that protrusion morphology is dependent on the molecular arrangement of such initiators. Arrangement of molecules in such a manner presumably requires further complex interactions, each of which may contribute to a time-based limitation (see the 'Discussion' section). A continuous excitation in time, through the imaging process in LLSM should allow sufficient time for enough number of molecules as well as subsequent downstream events taking place, to result in protrusion formation. We, therefore, resorted to a wide-field excitation strategy focusing the 445-nm laser at the back focal plane of the detection objective ( Fig. 1e; see the 'Methods' section). This produced continuous optogenetic stimulation that was independent of the volumetric imaging of the sample (Fig. 1e). This mode of photoactivation leads to effective PA-Rac1 activation and transformation of the dorsal surface of the cell from filopodial protrusions and small membrane ruffles to large-scale sheet-like membrane ruffles as has been previously reported (Fig. 1f, Additional file 2: Movie S2) [15,16]. All experiments described below were carried out using wide-field (continuous) photoactivation. Efficient ruffle formation involves the following process: (a) there is an overall decrease in the filopodia, and punctate structures appear that grow along its length (Fig. 1g). (b) At this regime, the characteristic length of the ruffles is dependent on laser power (Fig.  1h). (c) At higher laser powers, the ruffles grow and merge with one another, resulting in formation of complex branched geometries (Additional file 3: Movie S3). PA-Rac1 was found to be membrane localized, as previously reported [14], and enriched in the ruffles following photoactivation ( Fig. 1f, g, Additional file 2: Movie S2 and Additional file 3: Movie S3) and as such PA-Rac1 mCherry signals can be used to visualize and identify the ruffles.

Repetitive photoactivation sequences reveal re-initiation of growth on pre-formed ruffles
Our observations suggest that with continuous excitation, a threshold concentration of activated PA Rac1 molecules is achieved that result in local cytoskeletal rearrangements. PA-Rac1-mediated actin reorganizations then lead to efficient lamella formation. This activated Rac1-dependent process represents a barrier that cannot be overcome in discontinuous photoactivations. We reasoned that a ruffle generated in the first cycle would have molecular arrangements and actin meshwork architecture that would be pre-disposed for re-initiation of a collapsing ruffle. To test this, we performed repeated consecutive stimulation experiments on cells expressing PA-Rac1 (Fig. 2a, b). Using VR, we quantified the length of distinguishable membrane protrusions (Fig. 2e, Additional file 4: Movie S4). The first two stimulations did not lead to a discernible increase in the height of the ruffle protrusions, but rather an increase in the length that reflects an increase in net polymerization. The second and third stimulations led to a stepwise increase in the overall height of the membrane protrusions and extrusion of very long sheets on the dorsal surface. This suggests that pre-activated, but collapsing ruffles can be reactivated, leading to re-initiation of assembly of actin meshwork. The increase in the height of the protrusions supports the idea of polymerization forces at play along the direction of protrusion when PA-Rac1 is activated. Further, upon turning off the activation laser after the third stimulation, the complex membrane folds collapsed onto very bright compact structures owing to actomyosin contractility ( Fig. 2a-c, red boxes, Additional file 5: Movie S5). Interestingly, following the collapse, activating the PA-Rac1 resulted in 'unfurling' of compact contracted membrane folds (Fig. 2c, stimulation 4, magenta and green arrows). These unfurling events showed rotational motions driven by the polymerization forces (Fig. 2c, d, magenta and green arrows, Additional file 6: Movie S6). These observations clearly demonstrate that PA-Rac1 activation results in a polymerization dominant phase that is capable of stretching the membrane resulting in unfolding of complex membrane folds.
While lamellipodial protrusions are mainly actindriven structures, in some cases also a microtubule association was also observed [22,23]. To investigate whether dynamic microtubules are associated with the PA-Rac1 membrane protrusions, we co-transfected cells with EB1-GFP and investigated the localization and dynamics of protrusions in response to the optogenetic activation of PA-Rac1. We observed no microtubules entering the dorsal ruffles ( Fig. 2f, Additional file 7: Movie S7). Inhibiting microtubule polymerization using nocodazole had no effect on the process of ruffling by activation of PA-Rac1 as observed visually or by quantification of ruffle lengths and heights which (Fig. 2g, h). The absence of microtubule-ruffle interactions may be attributed to the transient nature of the ruffles, the sharp angle of propagation between the microtubules and ruffles or the dense actin meshwork architecture preventing microtubule entry. These observations taken together suggest that actin machinery is the dominant structural component orchestrating membrane ruffle dynamics.
PA-Rac1 produces larger and straighter membrane protrusions than PMA PA-Rac1 induced ruffle dynamics strongly suggest that actin polymerization forces dominate during the PA-Rac1 activated phase. To characterize the mechanical properties and the dimensions of the membrane ruffles, We compared ruffles that are stimulated using photoactivation of PA-Rac1 with those formed by stimulation with 100 nM PMA, a chemical agonist that induces membrane ruffling [24] (Fig. 3a). Upon Rac1 activation, we observed templated assembly of dorsal ruffles which polymerized from lamellipodia at the cell periphery before 'lifting off' and propagating along the dorsal cell surface (Fig. 3c, Additional file 8: Movie S8) as also observed by Begemann et al. [25]. Moreover, we also noted that dynamic membrane protrusions formed across the dorsal surface in response to PA-Rac1 activation (Fig.  3b). The observed membrane transformations are complex and developing image analysis-based algorithms to precisely segment out such dynamic pleomorphic dynamic structures with varying fluorescence intensities present various difficulties. We resorted to a virtual reality (VR)-based approach [26], where the threedimensional movies were rendered to enable the depth perception in the volumetric images akin to naturally evolved depth perception in vision of our surroundings. Using VR, we measured the end-to-end distances and the contour lengths of the ruffles as viewed from the top (Fig. 3d). Although the membrane ruffle is a sheet-like structure that is attached to the basal substrate in a very complex manner through acto-myosin cortex and other cytoskeletal structures, its two-dimensional conformation in the membrane plane is strikingly similar to that of a semiflexible filament (Fig. 3e). This allowed us to quantify their 2D conformations of different activations in terms of the persistence length l p , by analysing their squared end-to-end distance R 2 ee as a function of the contour length L using expression (eq. 1) for the 2D worm-like chain model (Fig. 3f) [27,28]: The persistence length of PA-Rac1 ruffles (~5 μm) is considerably larger than that of PMA-activated ruffles (~0.8 μm) (Fig. 3f), which perfectly agrees with their visual perception in Fig. 2a. At the same time, this does not necessarily means that PA-Rac1 ruffles are correspondingly stiffer: the PMA ruffles may be equally stiff but have a smaller persistence length owing to their intrinsic curvature, potentially due to concomitant myosin activity. Then, the observed persistence length l p, obs is related to the persistence lengths corresponding to the bending stiffness of the structure and its intrinsic curvature, l p and l p, int , respectively, via the relationship l − 1 p;obs [29,30]. Assuming that the PMA ruffles have l p close to that of the PA-Rac1 ruffles, we can estimate the intrinsic curvature-related persistence length of PMA ruffles as~1 μm.
We also measured the height of the ruffle along the length as well as the thickness in deconvolved images (Fig. 3h, i). We observed that while membrane ruffles showed variation in their height during the encapsulation process, they showed a rather uniform and consistent thickness with a mean of 0.83 μm across their length (Fig. 3g, h). The PA-Rac1-based dorsal ruffles showed a characteristic width similar to that observed in neutrophil-like HL-60 cells (0.78 μm by LLSM, 0.54 μm by spinning-disk and 0.64 μm by SEM) [18,31], suggesting that there exists a linear arrangement of regulatory molecules that produces ruffles in a similar manner. The PA-Rac1 activation may drive an increase in polymerization leading to the slightly thicker sheets observed in our experiments. Further, the variation in height over few micrometres of ruffle length was below 110 nm, as measured in deconvolved data sets using segmentations based on thresholding that can delineate edges with sub-pixel resolution (Fig. 3i, Additional file 9: Movie S9). This suggests that the PA-Rac1-generated ruffles are devoid of any tent-pole like arrangements [32] and can sustain dependence on polymerization forces. The relatively small standard deviation of the height along the length of the ruffles can be attributed to complex interplay between actin polymerization at the edge of the ruffle and the linear sheet-shape of the ruffle. Since Rac1 activity is known to increase Arp2/3-based branched actin meshwork [33,34], a noise suppression system involving these parameters may be envisaged as has been described for the leading edge of cells [35].
Our observations of intrinsically sheet-like ruffles of several micrometres long, generated by PA-Rac1, suggest that protrusion formation can also take place with initiation coming from chemical activation of Rac1 than mechanical curvature-dependent activation alone [25]. In this case, we have used PA-Rac1, but across the diverse roles of Rac1-driven ruffling, there exist multiple mechanisms of activation to produce migration [36,37], micropinocytosis [3] or macrophage tunnelling nanotube biogenesis [38]. There is no consensus on what distinguishing factors determine circular and linear dorsal ruffles apart from their geometry. Linear ruffles are generally associated with the lamellipodia and circular dorsal ruffles are typically stimulated by an agonist [5]. We consistently observed that activated PA-Rac1 resulted in stiffer and more linear ruffles, whereas switching off PA-Rac1 caused ruffles to fold over, showing rotational features characteristic of circular dorsal ruffles [39]. This suggests that the rotational characteristics that define 'circular' dorsal ruffles may be a complex interplay of polymerization and contractile forces.

Deactivation of PA-Rac1 leads to buckling and closure
We hypothesized that the reason for the ruffles formed by PMA to be consistently curved as compared to PA-Rac1-induced ruffles may be the contractile forces that cause membrane sheet protrusions to fold and collapse leading to engulfment. Therefore, we tested whether increased polymerization-induced forces keep the ruffle in a 'stretched' geometry and therefore whether upon releasing the PA-Rac1 from the activated state, the contractile forces dominate which leads to ruffle collapse. To assist resolvable observations, we combined PMA and PA-Rac1-mediated stimulation, as above (Fig. 4a, Additional file 8: Movie S8). During optogenetic PA-Rac1 activation, we observed that large dorsal ruffles formed at the cell periphery (Fig. 4a, white box 3B, white arrows). We observed that deactivating PA-Rac1 led to various behaviours suggestive of contractile forces, which included buckling (Fig. 4a, c, red arrows 3F, white arrows) and formation of cup-like structures (Fig. 4a, d, Magenta arrows). Further, upon switching off the photoactivation laser, splitting of ruffles (Fig. 4a, blue arrows) and subsequent recoil of the split ruffle was also observed that led to buckling and folding of the ruffle onto itself (Fig. 4a, e, green arrows). This led to cup closure and macropinosome formation (Fig. 4g, Additional file 8: Movie S8, Additional file 9: Movie S9 and Additional file 10: Movie S10).
Macropinocytosis, phagocytosis and ruffling are all processes that involve a substantial extension of sheet-like protrusions of an actin network-filled membrane that undergoes folding or wrapping to result in engulfment [1]. At both mechanical and biochemical levels, these processes have a lot in common, including involvement of Rac1 [2]. Previous studies have shown that activation of Rac1 is sufficient to form macropinocytic or phagocytic cups, but deactivation or decline in Rac1 activity is necessary to lead to cup closure [16]. In this regard, it is evident that the spatial coordination of cup closure is a significant task as it needs to occur at the right place without pushing out the engulfed fluid in macropinosome. In naturally occurring macropinocytosis, Rac1 deactivation may occur through coordinated recruitment of Rho GEFs and GAPs [40,41]. Here, using PA-Rac1, we show that the process of ruffling that leads to engulfment can be 'held' at the polymerization forcedominated stage and can be released by switching off the photoactivation laser, resulting in contractile forces to dominate and cause engulfment.

Myo1E associates with membrane ruffles with high spatio-temporal coincidence
To test if we can measure the partitioning of proteins specifically into the ruffles and their dynamics with respect to the formation of ruffles, we investigated the dynamic localization of various myosins during the PA-Rac1-stimulated ruffling process. MyoIIA is not known to be part of ruffling machinery; however, both Myo1e and MyoX have been reported to localize to the phagocytic cup in macrophages [17,42,43]. Myo1e has also been implicated in linking PI (3,4,5)P3 to actin remodelling in chemotaxis, macropinocytosis and phagocytosis in Dictyostelium [44,45]. Both Myo1e and MyoX have PH-domain that can enable binding to PI(3,4,5)P3. Though phagocytic cups and macropinocytic cups are structurally similar-consisting of lamellar structureswe investigated the associations of particular myosins with PA-Rac1-based ruffles to ask whether there are distinguishing features. Therefore, we assayed if MyoX and Myo1e were specifically enriched in PA-Rac1 ruffles. We expressed MyoIIA, MyoX or Myo1e along with PA-Rac1, photoactivated PA-Rac1 (WF mode) and performed 2-colour imaging (Fig. 5d, Additional file 11: Movie S11). We did not detect any enrichment of MyoIIA or MyoX, in comparison to Myo1e, which showed a high level of specific enrichment, similar to the PA-Rac1 YFP-positive control (Fig. 5a). Myo1e localized to PA-Rac1 ruffles at the same time as its formation (Fig. 5b, e). Correlation analysis showed a single peak at 0 s, indicating simultaneous recruitment of Myo1e to PA-Rac1 signal at time scales longer than the timeresolution of our measurements (8 s) (Fig. 5c). MyoX, on the other hand, inhibited the ruffle formation arising on the dorsal surface of the cell. The only ruffles observed were the one originating from lamellipodia (data not shown).
While MyoX has been reported to be localizing in phagocytic cups, we could not detect any MyoX signal in PA-Rac1-based ruffles. However, the appearance of Myo1e in the ruffles is in agreement with a recent study that showed that Myo1e played a role in phagocytic cup closure in the context of Fc receptor-induced phagocytosis [43]. It is also of note that Myo1e or Myo1f have been implicated in lamellipodial neutrophil migration [46] and FAK-PI3K-RAC1-associated B-cell migration [47]. Together, our results suggest that some general architectural components of the lamellar protrusion machinery may be conserved, and there may be other differences between phagocytic, pinocytic and lamellipodial protrusions with distinct sets of myosins engaged in different processes.

Discussion
We have combined LLSM with optogenetic activation for measuring the morphodynamics of PA-Rac1-based ruffling processes with high spatio-temporal resolution. Processes on the dorsal side of the cell are difficult to measure by many traditional geometries of imaging. We demonstrate that optogenetic approaches to study processes, where a threshold number of molecules need to be activated over time, can be achieved using simpler optical arrangements of wide-field photoactivation, even though use of SLMs offers precision control over space and time.
The results presented here clearly demonstrate that to achieve efficient ruffling, the photoactivation needs to be continuous. This is in line with previous studies that postulate a concentration dependence of Rac1 by virtue of its bivalent interaction with the wave regulatory complex (WRC). Chen et al. [34] propose a model where maximal WRC activation is evinced by simultaneous engagement of two Rac1 molecules per WRC and may control actin dynamics by sensing the local density of Rac1 [37]. From the results demonstrated in this study, along with previously reported molecular interactions that govern branched actin formation downstream of Rac1, a multi-step process can be envisaged. Photoactivation of Rac1 triggers Arp2/3-mediated actin branching, which is mediated through the WRC [48,49]. However, Arp2/3's mediation and suggested role in dictating ruffle morphology would require time for further molecular rearrangements in specific patterns [18]. A study complementary to ours, where the authors use single particle tracking of Rac1 coupled with optogenetic activation of Rac1 (albeit, indirect, using Tiam1 recruitment to membrane) demonstrates that activated Rac1 immobilizes at the protrusion tip [50]. With actin polymerization generating pushing forces against the membrane that can generate negative curvature, I-Bar protein IRSp53, which is known to interact with Rac1, and WAVE is recruited, which positively reinforces the protrusion geometry [25,51,52]. This positive feedback loop of curvature seeded by stimulated PA-Rac1 promoting I-Bar sensing would presumably enable sustained activation of Rac1. However, the extent of this The mechanism entails IRSp53 forming a higher order oligomer structure to enhance favourable protrusion geometry; a process which may also present a threshold. Taken together, a complex interplay between the membrane tension, polymerization forces of actin and organization of the branched actin meshwork through PA-Rac1-IRSp53-Wave-Arp2/3, positive feedback to reinforce protrusion geometry and Rac1-WRC activation kinetics is envisaged that leads to generation of lamellar protrusion (Fig. 6). This complex interaction cycle is sustained as long as PA-Rac1 is active and the local concentration of active Rac1 is constantly maintained. This organizational architecture is maintained at least for a few minutes even after switching off the photoactivation laser, which results in re-initiation of protrusion upon re-activating PA-Rac1. As has been highlighted, it is clear that polymerization events and ruffle formation is a complex, multifaceted process whereby the multitude of events imposes a time-based limitation, attributing for the lack of ruffling under a discontinuous excitation mode. Our approach will be valuable to decipher the roles of other molecular effectors of the acto-myosin protrusion machinery such as Cdc42, formins and specific myosins [53].

Conclusion
Rac1 activation is critical in a number of distinct processes that involve transient actin-driven membrane protrusions including receptor-stimulated macropinocytosis, pinocytosis, lamellipodial driven migration [16,36,54]. Photoactivation allows disentangling time and activitydependent processes as demonstrated here by PA-Rac1. Our approach, demonstrated here, is widely applicable to investigate processes occurring at the dorsal surface of the cell, more accessible owing to the imaging geometries of the light-sheet based microscopes. We believe optogenetics, in combination with light-sheet approaches, can be instrumental in studying the spatiotemporal activity, localization and function of various other proteins, morphodynamics of protrusions and other complex phenomenology associated with the unsupported dorsal membrane surface.
Microtubule depolymerization was carried out by incubating the cells with 25 μM nocodazole for 2 h in DMEM and imaged in the LLSM with media containing 25 μM nocodazole.

Microscopy
Cells were imaged using a lattice light-sheet microscope (3i, Denver, CO, USA). Excitation was achieved using 488-, 560-and 640-nm diode lasers (MPB communications) at 1-5% AOTF transmittance through an excitation objective (Special Optics 28.6 × 0.7 NA 3.74-mm immersion lens) and was detected via a Nikon CFI Apo LWD 25x 1.1 NA water immersion lens with a × 2.5 tube lens. Live cells were imaged in 8 mL of 37°C-heated DMEM and were acquired with 2x Hamamatsu Orca Flash 4.0 V2 sCMOS cameras. For SLM-based optogenetic excitation, 445 nm with full or quarter mask patterns was included in the sequence with 100% laser power. For wide-field excitation, a 1 W 445 nm was attenuated with neutral density filters, expanded and focused on the back focal plane using a 700-mm focal length laser. Laser powers were modulated using a neutral density filter wheel as measured at the back focal plane of the collection objective. Lasers were blocked physically using a beam blocker (Thor labs) manually by keeping time using number of volumes acquired and recorded. Images were acquired using 3i Slidebook and deskewed using custom codes and deconvolved using Richardson-Lucy algorithm [59,60].

Image analysis and segmentation
To quantify ruffle lengths, maximum intensity projection images were generated and analysed using FIJI. The images, after thresholding, were skeletonized and parameters were extracted using the plugin 'analyse skeleton' [61]. To measure the ruffle thickness, profiles across the cross section of ruffles from deconvolved single planes of the volumetric stack were measured. To measure the contour lengths, SyGlass VR was used [26]. Images were surface rendered, and the contour lengths were drawn manually. The collated data was exported, and end-to-end distance was extracted from the first and last coordinates of each ruffle. The dependences of the squared end-to-end distance on the contour length were fit with a 2D worm-like chain model: ðR 2 ee Þ¼8l 2 p ½L=ð 2l p Þ-1 þ expf-L=ð2l p Þg (Eq. 1) [27,28]. Similarly, heights were measured manually along the length using the surface-rendered boundary of the protrusion and base of the ruffle. Intensity measurements for ruffles were carried out by manually defining regions of interest (ROI) that consisted of PA-Rac1 signal, and the intensity of second channel pertaining to different myosin types was extracted. A similarly sized ROI (equivalent in pixel numbers) was chosen as a cytosol control to normalize. Intensities were plotted in Origin Pro. Cross-correlation between the signals in the two channels was performed using Origin Pro.