Designing novel artificial microswimmers or self-propelled particle systems is currently a subject of vast interest in active matter for a variety of reasons. First, they provide us with model systems to study the collective behaviour of their more complex natural counterparts1,2,3,4. Second, they display a variety of non-equilibrium phenomena, such as active clustering, segregation and anomalous density fluctuations1,2,3,4. Several experimental studies have been reported on artificial microswimmers, invoking and using different swimming strategies1,2,3,4,5,6,7,8,9,10. One class consists of internally driven systems of which Janus particles are an example, inducing motion by converting chemical energy on one side of the particle from its local environment1,2,3,4,11. In these synthetic systems, rotational diffusion of the particle randomises the propulsion direction, but its directionality, i.e., the velocity vector with respect to the metal-coated hemisphere, remains constant4,11.

On the other hand, the position and/or the orientation of driven particles can be controlled using external stimuli such as magnetic and electric fields6,7,12. However, unavoidable field-induced (magnetic/electric) long-range dipole–dipole interactions between the particles by external fields13,14,15 usually preclude studies of collective behaviour controlling solely the activity12. We are only aware of recent proof-of-principle studies that considered a single internally driven particle achieving propulsion direction reversal using a wettability contrast on both sides of Janus particles at different temperatures8,16, but as these are limited by heat transfer rates, they are inherently slow. To study the effect on collective behaviour, the dynamics of switching need to be faster than the intrinsic time scale of the systems, e.g., rotational diffusion. In nature, some microorganisms do indeed display rather fast periodic reversals in the direction of motion, examples including Myxococcus xanthus17, Pseudoalteromonas haloplanktis18 and Vibrio alginolyticus19, using complex molecular mechanisms. Interestingly, these marine microorganisms exhibit a rich collective behaviour, examples including accordion wave patterns20, and high-performance chemotaxis21.

Controlling and switching the nature of interactions (e.g., attractive to repulsive and vice versa) between individual units without changing the chemistry of starting building blocks is a major challenge in soft condensed matter22. Yuan et al.22 have recently achieved this by exploiting  the difference in the elastic response of a complex liquid crystal matrix to different light modulations. In this work, we use a simple approach to design novel synthetic active particles capable of performing fast propulsion direction reversals in combination with the switchable nature of interactions by simply changing the wavelength of light. In order to achieve such a model system, we take advantage of the different photocatalytic activity of a single Janus particle, specifically a half-gold-coated anatase TiO2 particle, under distinct wavelengths of light. Control over the surface chemistry enables a rapid reversal of propulsion direction. An advantage of our nearly two-dimensional (2D) system is the ease of imaging which makes it ideally suited to address the question: how does the reversal of propulsion direction of the individual propelling unit affect the collective behaviour? As an example we exploit these particles to drive the passive particles into dynamic and reversible 2D assemblies via light-switchable propulsion, which changes the interaction between the active and passive particles from attractive to repulsive. The photocatalytic decomposition of hydrogen peroxide produces concentration gradients which depend on which side is being activated. As the particles are force free, the phoretic forces resulting from the concentration imbalance around the particles need to be compensated by a directed motion subject to fluid drag. However, as the gold cap is heavier than the other side, this biases the quiescent orientation of the cap relative to the wall. As a consequence, the symmetry of the resulting disturbance hydrodynamic flow fields of the activated particles depends on the cap orientation and regulates interactions between active and passive particles. As a proof of principle, we use additional external stimuli to control the cap orientation even more, to show that the interaction between active and passive can be switched between attractive to repulsive and vice versa by changing the cap orientation. To elucidate the mechanism further, we study phoretic flow fields created by active particles attached to a wall with the cap orientation being fixed. These experiments are also used to better understand the flow fields around individual particles. For dilute suspensions of active particles, even when mixed with passive ones, the complex phoretic effects can be well captured using simple hydrodynamic scaling models. The use of low concentrations of directionally controlled and switchable particles in the sea of passive ones enables therefore new routes to design materials, sculpting them from within.


Light-switchable propulsion direction reversal

We use a Janus particle with different photocatalysts on each side, activated simply by changing the wavelength and the intensity of light to control over the propulsion direction and strength. Our experimental system consists of half-gold-coated anatase TiO2 particles with a diameter (σ) of 3.5 μm (see scanning electron microscopy image, Fig. 1a, inset) in an H2O2 solution. These Janus particles are heavier than the dispersing medium, thus they sediment to the bottom of the observation chamber. The gravitational length, i.e., the height to which the particles can be pushed up by thermal fluctuations, is only 30 nm, which makes the system essentially two dimensional. Under bright field illumination the particles undergo Brownian motion near a wall, commensurate with their size and the viscosity of the solution (Fig. 1a–c). When UV light (λ ~ 370–385 nm) is sent through the microscope objective lens, the particles start propelling in the direction of the TiO2 side, the bright side of the particle as shown in Fig. 1d–f. For the particle shown in Fig. 1d–f, this implies motion to the right as indicated by the red trajectory. At this particular fuel concentration (12 vol% H2O2 solution) and light intensity (3.5 mW cm−2), the particles are propelled with a speed of 16–18 μm s−1. Conversely, when light is switched from UV to green light (3.5 mW cm−2, λ ~ 535–565 nm), the particle instantaneously changes its propulsion direction and moves in the opposite direction (the dark side of the particle), however, with lower speeds of 4–5 μm s−1, as shown in Fig. 1g–i. We note that the swimming speed of the particles that is triggered by the UV light is 3–4 times higher than that of green light illumination (Fig. 1d–i). This can be attributed to the fact that the anatase TiO2 particles (Supplementary Fig. 1 confirms the XRD spectrum for the anatase phase) are photocatalytically more efficient under UV than green light23. We note that a high-intensity mercury white light source (25 mW cm−2) also induces the same propulsion speed and direction as the green light.

Fig. 1: Reversing the propulsion direction using different wavelengths of light.
figure 1

ai Time-lapsed bright field microscopy images are showing the mode of the motion and the overlaid trajectories revealing the typical trajectories, respectively. The half-Au-coated anatase TiO2 particles are dispersed in 12 vol% H2O2 solution. Note the bright side is the TiO2 side while the dark side is the half-gold-coated cap. In the schematic, the gold colour corresponds to the gold-coated side of the particle, whereas the light brown represents the sintered TiO2. Colour of lightning bolt illustrates the wavelength of light used in the experiment. ac Brownian motion of the particle. Inset shows a scanning electron microscopy (SEM) image of the Au-coated TiO2 Janus particle. df The swimmer propels in the forward direction under illumination UV light. gi The swimming direction of the particle is reversed after a switch to green light. The arrow depicts the direction of the propulsion. The brightness and contrast of the images are adjusted using ImageJ. Scale bar is 5.0 μm. Scale bar in the inset is 2.0 μm.

In order to quantify the propulsion strength, we measured particle trajectories by extracting the particle’s centroid from the time-lapsed images using a particle-tracking algorithm24 (see Supplementary Note 3). The overlaid time-lapse bright field image sequences show the typical trajectories and the direction of propulsion. For clarity, we overlay trajectories with different colours to distinguish each different mode of propulsion: dark gold for Brownian motion (Fig. 1a–c), red for the forward motion driven by the UV illumination (Fig. 1d–f), and green for the backward motion triggered by the green light (Fig. 1g–i). Additionally, the light-switchable propulsion directional reversal can be repeatedly achieved as many times as needed (see Supplementary Movie 1) as long as the sufficient fuel is present. To the best of our knowledge, we are not aware of any internally driven synthetic experimental system with such an exquisite control over the propulsion directional reversal and strength controlled by the intensity of light (see Supplementary Fig. 2). Strikingly, the trajectories of the particles (see Supplementary Movie 1) resemble the motion of run-and-reverse behaviour of some marine microorganisms17,18,19.

The exact description of the photocatalytic decomposition reactions25,26,27 and their underlying mechanisms involved in the particle’s propulsion direction reversal are chemically complex in nature, but a qualitative explanation is provided. Under the UV irradiation, the decomposition of H2O2 is triggered by the photoinduced electron–hole pair generation23,28 on the surface of anatase TiO2. The resulting holes oxidise the H2O2, thereby creating the protons on the TiO2 side of the Janus particle. The generated protons are subsequently involved in the reduction reaction at the Au-coated side of the particle (see Supplementary Fig. 3). The flux of freed protons generates a fluid flow towards the Au hemisphere that induces the self-electrophoretic motion on the other side of particle, i.e., along the TiO2 side which is the bright side of the particle (Fig. 1e–h). Under green or high-intensity visible light illumination, the Au-coated side of the particle is involved in the decomposition reaction, which in combination with the weak photocatalytic nature of anatase TiO2 at this wavelength results in an opposite concentration gradient (see Supplementary Fig. 3) that induces a self-diffusiophoretic motion in the direction of the Au hemisphere (see Supplementary Fig. 3). It has been reported that Au-coated Janus particles (e.g., Au-coated Janus silica and Au-coated Janus polystyrene) show self-propulsion behaviour induced by self-thermophoresis29 under green light illumination. However, this occurs in the direction of the un-coated side of the particle, which is the opposite of what we observe here. In order to verify our hypothesis whether gold can decompose H2O2 or not, we repeated the experiments with half-Au-coated silica as well as Au-coated polystyrene particles and maintain the similar experimental conditions. We measured the propulsion speed (2–3 μm s−1 in 15 vol% H2O2 solution) in the direction of the un-coated side, which is consistent with a previous study29. However, our self-propelled particles show self-propulsion in the opposite direction (see Fig. 1g–i), suggesting that the photocatalytic decomposition of H2O2 on the surface of anatase TiO2 is the dominant contribution. For what follows it suffices to note that the spatial dependency of the concentration fields and the subsequent motions are controlled by the wavelength of the light used.

Collective motion—fusion and fission

To date, mainly simulation and theoretical studies have predicted that motility alone is sufficient to drive dynamic clustering followed by a phase separation in active systems30. However, most of the experimentally observed clustering and phase separation in phoretic systems results from a combination of motility and the presence of short-range attractions that are mediated by the asymmetric distribution of the chemical fuel species around the Janus particle30,31,32,33. In the present experimental system, because of the presence of a wall, the disturbance velocity flow fields generated by the phoretic effects are asymmetric and directional. The resulting hydrodynamic interactions strongly affect the collective dynamics. In this regard, we increased the particle concentration to an area fraction ϕa = Nap/A ≈ 0.06, N being the total number of particles, A the surface area of the system, and ap the surface area of a single particle. Upon illumination with green light, the particles spontaneously start clustering and show long-ranged attractions between the particles. As a consequence, small clusters (2–4 particles) of nuclei are formed in different locations, which then evolve into a few medium-sized (8–10 particles) clusters by coalescence of the smaller ones. Next, these medium-sized clusters further combine into a single defect-free large cluster at the expense of all available small clusters of particles as shown in Fig. 2a–f. This phenomenon resembles fusion, leading to crystallisation of the particles (see Supplementary Movie 2). We measure the inter-particle distance as a function of time to quantify how fast the particles are approach each other and form clusters. The inter-particle approach velocity shows a long-range spatial dependency (1/r1.25) (Supplementary Fig. 4) and these long-range attractions result from the solute-mediated diffusiophoresis25,26,34.

Fig. 2: Fusion and fission dynamics of switchable photoresponsive colloids.
figure 2

af Fusion: Time-evolution and dynamic growth show the fusion of the active particles into a single cluster. gk Fission: Time-evolution of the fission dynamics shows the big cluster under the UV illumination. This single cluster explodes into small clusters when the direction of propulsion of the particle is reversed. l Small clusters dissolve when the illumination switches to green light. Colour of lightning bolt shows the wavelength of light used in the experiment. m-Projected orientations of the caps reveal the self-trapping of the particles in a cluster, and the melting of the cluster when the propulsion direction is reversed. mp Red colour arrow points the propulsion direction along the TiO2 side, bright side of the particle. qt Magenta colour arrow depicts the propulsion direction reversal under green or high-intensity white light illumination. Scale bar is 5.0 μm.

To probe the dynamic response of the particle’s propulsion reversal, we switch from green to UV illumination, which causes the cluster to explode and break up into an array of small clusters as well as individual particles that swim outwards as shown in Fig. 2g–l. The whole process of clustering (Fig. 2a–f) and exploding (Fig. 2g–l) resembles fusion and fission phenomena (see Supplementary Movie 2), which occur over a wide-range of length scales spanning from subnuclear35 to colloidal36 to cells37 to macroscopic scales38. During the disassembly of the cluster we observe two distinct time-dependent regimes. Immediately after switching the propulsion direction, the particles at the edge of the cluster that have an outward propulsion direction escape first and move ballistically with velocities as high as  ~40–50 μm s−1. Meanwhile, particles at the centre of the crystal are unable to escape because they block each other’s path.

To elucidate the role of the cap orientation of the individual particles on the observed fusion–fission behaviour, we analyse images of projected orientations of the caps within a cluster (Fig. 2m–t). To this end, we exploit the intensity difference between the two sides of the particle to identify the cap orinetation. The bright side is the TiO2 hemisphere, while the dark side is the half-gold-coated cap. Figure 2m–p shows the majority of the particles swim inward along the periphery of the cluster, while the particles with outward propulsion direction leave the cluster and swim away (right top-corner in Fig. 2m–p). When the propulsion direction of the individual particles is reversed by switching light from UV to green light, the cluster subsequently melts and all particles move away (Fig. 2q–t).

The fission process can be easily understood by realising that a swimmer surrounded by neighbouring ones in a fused cluster is unable to propel in the outward direction as it is trapped by neighbours (see Fig. 2m–p). Therefore, the particle is continually exerting a propulsion stress on neighbouring swimmers which generates a force imbalance from the centre to the outward layer of the cluster due to different orientations of the swimmers, which leads to an explosive disintegration. This observed fission process indicates that upon switching to UV light the velocity field around each particle is repulsive (Fig. 2g–k). The presence of these extra active stresses has been modelled as a swim pressure for situations where this stress is isotropic39. During the disintegration process some clusters having anisotropic shapes show a pronounced rotational motion (see Supplementary Movie 2). Due to the distribution of cap orientations of particles within a cluster (Fig. 2m–p), a few small clusters live longer than the other ones. We expect that the clusters would lose their identity when the propulsion direction of all the particles is directed outward. When we reverse the sequence of light irradiation (from UV to green light), we observe similar trends, but the explosion of clustered particles is not as strong as in the case of vice-versa illumination (Fig. 2g–k). This can be attributed to fact that the propulsion force is three times higher under UV light compared to the green light, as can be inferred from the propulsion velocity of individual particles.

To better understand the underlying mechanism responsible for the repulsion of active particles under UV illumination, we repeated the experiments with the isotropic anatase TiO2 particles while maintaining the same intensity (3.5 mW cm−2) of light and the fuel concentration. Previous theoretical studies have predicted the hydrodynamically mediated diffusiophoretic attraction and repulsion between the pairs of isotropic particles would lead to clustering and self-propulsion of their assemblies40. In our experiments, when a cluster of isotropic TiO2 particles is exposed to UV illumination, surprisingly, particles start to move outward radially. The overlaid trajectories depict the motion of isotropic particles in 12 vol% of H2O2 solution as shown in Fig. 3a–h. In our experiments, the average velocity of the particles versus time shows a power-law dependence Vpt−0.69±0.04. We can explain this behaviour using a scaling argument by modelling the particles as sources of the solute. The gradient of this solute along the surfaces of the particles gives rise to a phoretic slip11,41,42, which induces a flow of the solution. In the far-field limit, an isotropic sphere produces a chemical concentration field which dies out with distance as 1/r. If another sphere, placed at a distance l, moves in this concentration field, we find that its leading order velocity should be V ~ l−2. Since V = dl/dt, integrating this relation, we find l ~ t1/3, and finally  V ~ t−2/3 ≈ t−0.67, close to experimental observations. To gain further insight into the observed dynamics, we performed numerical simulations taking into account pairwise interactions of particles due to their induced phoretic flows40 (see Methods section on phoretic motion of isotropic active spheres). The simulation shows similar trajectories (Supplementary Fig. 5) when started from the initial positions taken from the corresponding experiment. An empirical fit to the experimental data for the velocity shows good agreement with simulations and the theoretical scaling in Fig. 3i. These experimental findings suggest that the observed repulsive interactions between the Janus particles under UV light can be attributed to a self-diffusiophoretic effect. To further confirm our hypothesis, we analytically calculated the solute concentration field around an isotropic TiO2 particle in proximity to a wall, and the resulting streamlines of the hydrodynamic flow field (see Supplementary Fig. 6a and Supplementary Note 5 for the full description of calculations). Our calculations indeed confirmed the flow fields around the isotropic TiO2 particle is repulsive. On the other hand, the Janus nature of the particle greatly amplifies what effectively can be described as a repulsive behaviour (Fig. 2g–k).

Fig. 3: Response of the isotropic TiO2 particles under the illumination of UV light.
figure 3

ah Time-lapsed bright field micrographs show the pushing behaviour of individual swimmers against the neighbouring particles. These repulsions are isotropic. Overlaid trajectories reveal the dynamic response of the particles. i The average velocity over all particles decays with time as Vt−0.69±0.04 and follows the predicted far-field scaling (t−0.67). The blue line is the prediction of the theoretical model obtained by numerical simulations. The error bars in i represent the standard deviation of the average velocity over all particles. j-o Dynamic response of the passive particles to an immobile active particle under the illumination of UV light. jo Time-lapsed overlaid trajectories show the tracer passive particles experience isotropic repulsions and push the tracers radially. p An empirical fit of the experimental velocity data shows the predictions of the theoretical model for the dynamics of tracer particles (solid line). The experimental average velocity over the all particles decays with time and follows the numerically obtained flow field produced by an immobilised active particle, modelled as a near-wall Stokeslet. Broken blue line is the far-field prediction which is expected to be valid at much longer times. The error bars in p represent the standard deviation of the average velocity over all particles. Scale bar is 5.0 μm.

Active and passive mixtures—interplay between attractions and repulsions

Unlike previous studies on active and passive mixtures, such as light-activated clustering of active and passive mixtures43,44 and micropumps26,45, here we combine the fast switchability of the direction and the subsequent attraction/repulsion using different wavelengths of light illumination and relatively fast switching, compared to the diffusive time scale of the particles. To get further insight into the effect of propulsion direction reversal on the (dis)assembling behaviour in the active–passive mixtures, we first immobilised an active particle on a glass substrate and added passive particles as tracers to capture the flow field around it (see Fig. 3j–o). This experiment creates a simpler situation where we can study the phoretic flows around the particle in detail, and investigate how the flow field can be described. Moreover, this provides insights for the more complex case of freely moving particles. Bright field microscopy images show that the particle is attached on the gold-coated side, visible as the dark side of the particle. In the case of inwards flow created by the active particle, passive particles organise into a hexagonal structure around the immobile active particle under green light illumination (Fig. 3j), which is consistent with the behaviour of active and passive mixtures in Fig. 4a–c. Under UV illumination the flow direction is reversed, which causes the passive particles to be radially pushed away (see Supplementary Movie 3), as shown in Fig. 3j–o. As discussed before, in the case of a freely moving active particle, the phoretic slip is towards the gold-coated side of the particle under UV illumination; therefore, the direction of propulsion is towards the TiO2 side. As the particle is attached to the wall, a repulsive flow field is produced, which can be modelled by a near-wall point force (a Stokeslet), in contrast to force-free swimmers which can be expected to give rise to force dipole flow fields46.

Fig. 4: Switchable photoresponsive colloidal particles in a sea of passive particles: from pulling to pushing.
figure 4

ac Assembly: Sequence of time-lapsed images show first the dynamic clustering of passive particles around the active particle under the green light illumination. df Disassembly: Sequence of time-lapsed images obtained upon the switching of the illumination to UV light. Overlaid trajectories reveal the outward motion of the passive particles. Inset f, overlaid trajectory shows the active particle motion. Cyan colour corresponds to the trajectory of the passive particles the red colour represents the active one. The black arrow depicts the position of the active particle. Colour of the lightning bolt represents the wavelength of light used in the experiment, respectively. g Time-stamped trajectories show motion of passive particles under UV light illumination. Scale bar is 5.0 μm. Scale bar in the inset is 10.0 μm.

We use a minimal model to describe the experimentally observed repulsive flow, a fixed particle (downward cap orientation) sets up an osmotic flow which can be described by a Stokeslet near a wall47 (see Supplementary Informations for the detailed model). A comparison of the experimentally observed velocities with a Stokeslet solution gives reasonable agreement (Fig. 3p). In contrast to earlier work involving attraction by an immobilised active particle31, the dynamics in our case are restricted to a 2D plane parallel to the wall at a distance h. The velocity of a tracer depends on the distance from the Stokeslet as \(R/{({R}^{2}+4)}^{5/2}\), where R = r/h is the rescaled distance46. We integrated numerically this relation to get the velocity of passive tracer particles which is empirically fitted to the experimental data (Fig. 3p). Good agreement with the experimental far-field behaviour of the in-plane Stokeslet flow, decaying as 1/R4, is found. However, in the near field the Stokeslet fails to describe the observed behaviour as other factors come into play (e.g., steric, slip, lubrication, and potentially electric interactions have a pronounced effect). Furthermore, the change in illumination will only lead to the reversal of the direction of the flow and the magnitude of the Stokeslet, not affecting its qualitative characteristics.

Control over cap orientation

For the freely moving particles, the disturbance velocity fields (force dipoles) will be closely related to those inferred from the fixed particles. To demonstrate further the role of cap orientation and the direction of resulting flow fields, we control the orientation of the gold cap using an external magnetic field (see Supplementary Fig. 7). This strategy allows us to switch the flow fields generated by active particles from repulsive to attractive and back. Supplementary Figure 7 demonstrates that the role of the cap orientation and the nature of the disturbance velocity fields are the key for controlling attraction versus repulsion. We demonstrated two ways to control the direction of the flow field from repulsive to attractive: (i) for a given wavelength, changing the cap orientation externally, and (ii) for a given cap orientation, changing the wavelength has the same effect. The latter provides an elegant route to exploit these effects to direct reconfigurable assembly and disassembly process in passive–active mixtures. We start with a dilute dispersion (ϕa < 0.5%, area fraction) of active particles in a concentrated dispersion (ϕp ≈ 12%) of passive silica particles (σp = 2.1 μm). When green light is on, the active particles spontaneously act as nucleation sites and they pull the neighbouring passive particles isotropically towards them while moving (Fig. 4a–c). As shown in Fig. 4a–c, when the passive particles accumulate around the active particle their propulsion speeds drastically decrease (<1.0 μm s−1). At this fuel concentration and light intensity, the range of the attractions between the active and passive particle is about 4–5σ. We note that this clustering is not caused by opposite charges on active/passive particles because both are negatively charged (with zeta potentials of ζactive ≈ −39 mV, and ζpassive ≈ − 48 mV). When we switch the light illumination to UV, the active particles instantaneously reverse their propulsion direction and increase their propulsion speed (Fig. 4d–f). The passive particles are now pushed away by the active ones (Fig. 4d–f), which creates a depletion zone (~8−10σ) around the active particle as shown in the inset of the Fig. 4f. Time-stamped trajectories depict the motion of passive particles in Fig. 4g. The trajectories of passive particles (cyan colour) illustrate the direction of the flow that is created by the propelling particle, and the red colour shows its the propulsion path (the inset of the Fig. 4f). This observation of the pushing behaviour and the creation of a depletion zone (see Supplementary Movie 4) is reminiscent of electroosmotic-flow-driven micropumps25,26. To control the interplay between attraction and repulsion, i.e., pulling and pushing behaviour of the active particles in passive mixtures, we vary the intensity of the UV light while the visible light intensity is kept constant. The attraction dominates at low intensities (<50% of Imax) and repulsive behaviour is only observed at the high intensities. Next, we increase the surface area fraction of passive particles (ϕp ≈ 35%) while the active particle concentration is kept constant (ϕa < 0.5%). Under UV irradiation, passive particles are compressed locally by the active particles (see Supplementary Movie 5), thus inducing local crystallisation as shown in Supplementary Fig. 8. During the compression process the velocity of the active particle is reduced by factor of 10, i.e., to 1.6 μm s−1. As we demonstrate here, our self-propelled particle system can be used to stir locally to drive the passive particles in dynamic assemblies which are relaxed and expand after UV light is turned off.

We note that the rotational dynamics of an isolated self-propelled particle is entirely diffusive, self-propulsion does not change it1,2,3. However, it has been recently reported that multibody effects will have stronger effects on rotational dynamics in the active and passive mixtures48,49. This is observed in our work for the case of attractive interactions. Owing to attractions with surrounding passive particles, the active particle’s rotational diffusion is slowed down (much smaller than the rotational diffusion of passive particle, Dr ≈ 0.0305 s−1) and the propulsion direction is now dominated by the passive particle’s arrangement (assembly) around the active particle as shown in Supplementary Fig. 9. However, for the repulsive case we do not see any measurable crowding effects.

When we increase the concentration of active particles to match that of the passive particles (here ϕp ≈ 15%, ϕs ≈ 12%), we observe a dynamic phase separation in which the active particles cluster together in the centre and the passive particles organise around the active cluster resembling a core–shell like configuration under green light, as shown in the Supplementary Fig. 10. This can be attributed to the fact that flow-mediated interactions between the active–active particles are stronger than those of the active–passive particles. Next, these small clusters further merge into a large cluster and then eventually reach a larger core–shell like structure (Supplementary Fig. 10a–f). Depending on the wavelength of light illumination used, the active particles can induce either attractions or repulsions with the passive particles, thereby assembling or disassembling around them (Fig. 4).

In conclusion, we developed a facile route to produce switchable photocatalytic swimmers which exhibit an almost instantaneous reversal of propulsion direction between both ends of the half-gold-coated anatase TiO2 particles by light modulation. The fast optical switching makes it possible to direct the assembly and disassembly by the mere control of the wavelength and intensity of light. The typically observed growth of the active clusters is a consequence of the solute-mediated long-range attractions to induce a fusion process, while the breakage process result of the propulsion reversal coupled with the propulsion strength and the gold cap orientation from the particle that gives some force imbalance across the fusion cluster that can trigger the fission process. Moreover, the small clusters surviving the fission process can be attributed to the different orientations of the active particles. These active particles can act as seed particles in active–passive mixtures, and conveniently drive the assembly and disassembly of passive particles by light modulation. Additionally, we are able to qualitatively explain the experimental results using a simple hydrodynamic scaling. We believe that the process of forced disintegration, as opposed to Brownian spreading, has new dynamical features which allow greater control over the collective dynamics of phoretic active matter. Our system paves a new way to realise fast switching between nature of interactions from attractive to repulsive, and back enable the design of reconfigurable materials by sculpting them from within. Moreover, the presented experimental system opens a new avenue for developing a new theoretical framework of active systems where the propulsion speed becomes a vector quantity, instead of a scalar parameter of the model.


Fabrication of self-propelled particles

TiO2 particles were synthesised following the procedure of He et al.50 (see Supplementary Note 1). We used thermal sintering to convert amorphous TiO2 particles to anatase phase. To obtain half-Au-coated anatase TiO2 particles, a monolayer of particles was first deposited on a glass slide. Gold was then sputter-coated (Safematic, CCU-010 HV Compact Coating) over the monolayers to get a final thickness of  ~40 nm. Next, particles were detached from the glass slide by sonication (Bandelin, Sonorex) for 4–5 min and collected by sedimentation. Finally, hybrid TiO2–Ni–Au particles were used to control the cap orientation using external magnetic field, in this case, a Ni layer was deposited and sandwiched between the TiO2 and gold (see Supplementary Note 2 for more details).

Imaging and data analysis

We followed the particle dynamics using an inverted microscope (Zeiss 200M) equipped with a high numerical aperture oil objective lens (×60 1.25 NA, ×100 1.3 NA, Oil, EC Plan NeoFluar) and with a mercury lamp (X-Cite 200 DC, Excelitas Technologies, USA), and a Nikon inverted fluorescence microscope equipped with a CCD camera (Olympus CKX41). Light that was sent through the microscope objective lens and the intensity of light was  uniform across the area of interest. Moreover, the light source is equipped with a manual knob to control the intensity of light. Different bandpass filters were used to restrict light emission to 370–385 nm (UV) and 535–565 nm (green). With our current experimental setup, we found that the time required to switch between two wavelengths is about 0.6 s. This is fast enough for the current study, as the time scale of switching needed to be smaller than the persistence time (≈35 s, 1/Dr, rotational diffusion of the self-propelled particle) for the self-propulsion. The intensity of light emission was measured with a photo detector (Thorlabs, PM 100D). We acquired images with frame rates ranging between 5 and 50 fps. The brightness and contrast of the images were adjusted using ImageJ. The particle’s centroid was extracted from time-lapsed images using ImageJ plugin, Trackmate24.

Mean-squared displacement

Using time-lapsed particle coordinates we measured the mean-squared displacement (MSD), thereby the propulsion velocity of the SPPs using home-written Matlab programme. The mean-squared displacement of SPPs differs significantly from the passive particles51. By fitting the mean-squared displacement curve with 〈Δr2〉 = 〈[r(t + Δt)−r(t)]2〉 = v2t2 + 4Dtt, where Dt is translational diffusion coefficient and ν is the propulsion velocity, for time scales much smaller than the rotational diffusion of the particle51, we measured the propulsion speed of the particles for a known H2O2 (BASF, Germany) concentration solution. A typical MSD curve for forward and backward motion of particles is shown Supplementary Fig. 11. The forward propulsion speed of SPPs is vf = 16.0 ± 2.0 μm s−1 and backward motion is vb = 4.8 ± 0.6 μm s−1 in 12 vol% H2O2 solution. We used the high fuel concentration to achieve higher propulsion speeds with a low intensity of light illumination (3.5 mW cm−2) to avoid any thermal heating effects in our study.

Phoretic motion of isotropic active spheres

A system of two isotropically active spheres has been analysed by Michelin and Lauga52 in detail for arbitrary separations. In the far-field limit, it can be regarded as one sphere moving in the concentration gradient created by the other. The leading order concentration field produced by a uniformly active sphere of radius R is given by

$$c(r)=\frac{{\mathcal{A}}}{\kappa }\frac{{R}^{2}}{r},$$

where r is the distance from the sphere, \({\mathcal{A}}\) is the chemical activity of the surface and κ is the diffusivity of the solute. For two spheres separated by a distance d, each particle is exposed to two concentration gradients: one stemming from its isotropic emission and another generated by its neighbour. Since the latter is asymmetric, it leads to propulsion with a velocity V which for uniform surface mobility \({\mathcal{M}}\) to leading order reads

$${\bf{V}}\,=\,\frac{{\mathcal{A}}{\mathcal{M}}{R}^{2}}{\kappa {d}^{2}}\hat{{\bf{d}}},$$

where \(\hat{{\bf{d}}}\) is a unit vector pointing along the symmetry axis of the system.

This calculation enables us to simulate the far-field dynamics in systems of many spheres by superposition of pairwise interactions. Within this framework, in free space, the velocity of the particle i is given by

$${{\bf{V}}}_{i}=\frac{{\mathcal{A}}{\mathcal{M}}{R}^{2}}{\kappa }\sum _{j\ne i}\frac{{{\bf{r}}}_{j}-{{\bf{r}}}_{i}}{| {{\bf{r}}}_{j}-{{\bf{r}}}_{i}{| }^{3}}.$$

This equation is the basis for our simulations of spreading of a cluster of active particles. To this end, we consider a cluster of N = 21 particles with their initial positions \({\{{{\bf{r}}}_{i}\}}_{i = 1,\ldots ,N}\) taken from the experimental configuration as in Fig. 3a. The positions of the particles are then evolved using a standard Euler scheme in Matlab. Then the average velocity is calculated as a function of time, as depicted in Fig. 3i.

For this type of interaction, a scaling argument can be made to understand spreading of particles under repulsive interactions. Since the velocity scales with the distance as V ~ r−2, integration gives r ~ t1/3, and thus the scaling V ~ t−2/3, which is very close to the experimentally measured exponent (0.69 ± 0.04), as described in the paper.

Phoretic flow due to a fixed sphere

A phoretic particle can propel itself by generating gradients of physical quantities such as temperature, electric charge, concentration of solute and exploiting the flow generated by these inhomogeneous fields. The gradients are generated close to the particle surface, thus leading to local slip flows. Similar to swimming microorganisms, the flow signature in the far-field is that of a force dipole v(r)

$${\boldsymbol{v}}({\boldsymbol{r}})=\frac{p}{8\pi \eta {r}^{2}}\left[3(\hat{{\boldsymbol{r}}}\cdot \hat{{\boldsymbol{p}}})-1\right]\hat{{\boldsymbol{r}}},$$

where p is the dipole strength, \(\hat{{\boldsymbol{r}}}={\boldsymbol{r}}/r\), and the unit vector \(\hat{{\boldsymbol{p}}}\) describes the orientation of the dipole. The flow field decays with distance like 1/r2, that is faster than the point force Stokeslet solution which decays as 1/r. This is due to the force- and torque-free character of motion of a swimmer in a viscous fluid. Depending on the sign of the dipole moment p, we discern pushers (p > 0) which typically generate their propulsion from the back and push the fluid along the direction of motion, dragging it in from the sides, and pullers which have the same flow field streamlines with reversed direction of flow.

However, when such a particle is confined next to a surface and immobilised, it is still creating flow and stirring the surrounding fluid. In this case, the net thrust generated by the phoretic flow is not balanced by the viscous drag force. Consequently, there is a net force pointing in the normal direction. Thus the flow field around can be modelled as one generated by a point force singularity acting close to a planar no-slip wall. The effect of the wall is accounted for by considering image singularity solutions, and the resulting flow field is given by the Blake tensor47 and for the case of normal force is sketched in Supplementary Fig. 6b.

Assuming the point force to be at a distance h to the wall, the flow due to a force F in the plane z = h is given in terms of the rescaled distance r = x/h and dimensionless time t scaled by 2πηh2/3F as


The flow in the direction normal to the wall is smaller in magnitude. Henceforth we consider lateral motion of the due to a fixed particle.

In the far field, the following scaling dictates the relation: the velocity field scales as V ~ r−4, which is integrated to give t ~ r5 or r ~ t1/5. Combining these, we obtain V ~  t−4/5, which is slower than the experimentally observed spreading. However, since the particles involved have a finite size and are in a crowded environment, the far-field effects in the flow are expected to be seen at long times. At short times, the finite size of the tracers results in complex many-body hydrodynamic effects and thus no simple scaling can be found. To elucidate these effects, we have integrated Eq. (5) numerically. In Supplementary Fig. 12, we present a comparison of two test trajectories of tracers starting at r0 = 0.1 which are advected in the flow due to a Stokeslet and subsequently decay as r−4, far-field component.

In Fig. 3p we present an empirical fit of the data to the theoretical curves obtained above. There are two fitting parameters in the problem: the strength of the source Stokeslet and the unit of time by which we rescale to make time dimensionless. These two factors come in when rescaling the experimental data to compare with simulations given in dimensionless units. Here they were chosen in such a way that the theoretical curve passes through most experimental points.