When photons interact with matter, forces and torques occur due to the transfer of linear and angular momentum, respectively. The resulting accelerations are small for macroscopic objects but become substantial for microscopic objects with small masses and moments of inertia, rendering photon recoil very attractive to propel micro- and nano-objects. However, until now, using light to control object motion in two or three dimensions in all three or six degrees of freedom has remained an unsolved challenge. Here we demonstrate light-driven microdrones (size roughly 2 μm and mass roughly 2 pg) in an aqueous environment that can be manoeuvred in two dimensions in all three independent degrees of freedom (two translational and one rotational) using two overlapping unfocused light fields of 830 and 980 nm wavelength. To actuate the microdrones independent of their orientation, we use up to four individually addressable chiral plasmonic nanoantennas acting as nanomotors that resonantly scatter the circular polarization components of the driving light into well-defined directions. The microdrones are manoeuvred by only adjusting the optical power for each motor (the power of each circular polarization component of each wavelength). The actuation concept is therefore similar to that of macroscopic multirotor drones. As a result, we demonstrate manual steering of the microdrones along complex paths. Since all degrees of freedom can be addressed independently and directly, feedback control loops may be used to counteract Brownian motion. We posit that the microdrones can find applications in transport and release of cargos, nanomanipulation, and local probing and sensing of nano and mesoscale objects.
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The data for Fig. 5b are provided as source data with this paper. Other data supporting the conclusions of this study are available in the paper (including Supplementary Information).
The codes used during this study are available from the corresponding authors upon reasonable request.
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Financial support by the German Research Foundation (DFG grant no. HE5618/10-1) and the Volkswagen Foundation via an ‘Experiment!’ grant (both received by B.H.) is gratefully acknowledged.
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Extended Data Fig. 1 Fabrication of the gold nanomotors.
Upper row: Optical micrograph of a gold flake (a) and scanning helium ion micrographs of the nanomotor structures (b-d) after outline milling with focused helium ion beam. Lower row: Optical micrograph (a) and scanning electron micrographs (b-d) of the nanomotor structures after the gold flake is peeled off. The inset of the upper panel of a is an optical micrograph of the gold flake when its right corner is covered by a dried-out droplet of PVA solution. The outline of the gold flake and the boundary of the PVA droplet at the gold flake region are illustrate by the dashed lines in the lower panel of a.
Extended Data Fig. 2 Fabrication of the microdrone body.
a, Gold nanomotors are fabricated on top of a spin-coated HSQ layer on an ITO/glass substrate. b, An etching mask of HSQ with the same shape of the microdrone body but increased thickness is created in the first electron beam lithography (EBL) step. c, The bottom HSQ layer is etched through with buffered oxide etch (BOE). The top mask is also thinned down and the wet etching leads to an unwanted side profile. d, The sample is spin-coated with HSQ again and the final body with defined shape and dimensions is created in the second EBL step. In panels a-c, the top and bottom HSQ layers are presented in different colors for better illustration.
Extended Data Fig. 3 Transfer of microdrones to a water cell.
Reflection (a-c) and phase-contrast transmission (d) optical micrographs of microdrones of a sample at key steps of the transfer process. a, On the glass substrate after ITO etching. The microdrones have moved slightly after the etching. The inset shows the well-aligned array before ITO etching. The shiny dots and disk are gold markers for pattern alignment for electron beam lithography. b, A PMMA piece with the microdrones attached on the top. A zoom to the area indicated by the dashed rectangle is shown in the inset (same for c and d as well). It is seen that the microdrone array is right-left flipped as compared to a. c, A PVA piece with the microdrones attached on the top. The microdrone array is flipped again as compared to b. d, The microdrones are transferred to water. The water droplet has a volume of about 2.5 µL and is sandwiched between two glass coverslips with a spacer of PDMS (165 μm thick). Now the microdrones are seen as the swarm of dark dots. The air bubble to the right will disappear with time.
Extended Data Fig. 4 Schematic of the optical setup.
The inset to the left sketches the fact that both laser beams are focused by the lens to the back focal plane (BFP) of the top objective (for polarized light) to create unfocused light fields. Both 830 and 980 nm laser beams pass a polarizer (horizontal direction) positioned directly behind the laser diodes. The two light beams are overlapping after the dichroic mirror LP 900 nm. The polarization compensator is used to correct the influence of the dichroic mirror LP 900 nm to the linear polarization of the 980 nm beam. The components and the water cell are not to scale.
Supplementary Figs. 1–5, Notes 1–3 and Videos 1–5.
Supplementary Video 1
Effect of the torque resulting from the transfer of the spin angular momentum of photons. Two types of microdrone with two identical motors are excited in the same light field of 830 nm. The two microdrones differ in the orientation of the motors, such that the two torque components on the right side of equation (1) have the same sign for one microdrone but have opposite signs for the other. As a result, the former microdrone rotates in the same direction as the circular polarization (orange arrow) with a higher speed, while the latter microdrone rotates in the direction opposite to the circular polarization with a slower speed.
Supplementary Video 2
Brownian motion of the microdrones inside the water cell after release when there is no driving light.
Supplementary Video 3
Actuation of two-motor microdrones. The original video has a frame rate of 100 fps, but is slowed down to 30 fps here. The parameters at the top are updated every six frames. The changing colour of the trajectories represents the progressing time. The positions of the motors (red points) are determined by fitting each of their images in the movie frames (dark spots) with a 2D elliptical Gaussian function. The centre of the microdrone and the orientation angles (yaw, pitch and roll) are extracted from the fitted motor coordinates.
Supplementary Video 4
Actuation of four-motor microdrones. The original video has a frame rate of 100 fps, but is slowed down to 30 fps here. The parameters at the top are updated every six frames. The changing colour of the trajectories represents the progressing time. The positions of the motors (red points) are determined by fitting each of their images in the movie frames (dark spots) with a 2D elliptical Gaussian function. The centre of the microdrone and the orientation angles (yaw, pitch and roll) are extracted from the fitted motor coordinates.
Supplementary Video 5
Continuous actuation of a four-motor microdrone in all three independent degrees of freedom.
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Wu, X., Ehehalt, R., Razinskas, G. et al. Light-driven microdrones. Nat. Nanotechnol. 17, 477–484 (2022). https://doi.org/10.1038/s41565-022-01099-z
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