pith. sign in

arxiv: 2604.14917 · v1 · submitted 2026-04-16 · ⚛️ physics.optics · cond-mat.mes-hall· cond-mat.mtrl-sci· cond-mat.soft

Light-propelled microparticles based on symmetry-broken refractive index profiles

Pith reviewed 2026-05-10 10:34 UTC · model grok-4.3

classification ⚛️ physics.optics cond-mat.mes-hallcond-mat.mtrl-scicond-mat.soft
keywords light propulsionmicroparticlesrefractive index profilesactive colloidal matter3D printingoptical symmetry breakingvolumetric active matteroptical actuation
0
0 comments X

The pith

Symmetry-broken refractive index profiles inside microparticles enable directed propulsion by asymmetric light refraction alone.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper establishes that microparticles can be fabricated with internal refractive index variations that break optical symmetry, producing net momentum transfer from refracted light rays and resulting in directed motion. This internal mechanism works independently of the particle's outer geometry, so even perfectly symmetric shapes can propel when illuminated. A reader would care because the approach relies on transparency rather than absorption or reflection, which reduces heating and allows light to reach particles deep inside dense collections. The authors develop a theoretical model, run ray-tracing and finite-volume simulations, and test the idea experimentally with geometrically asymmetric particles. If the central claim holds, propulsion becomes decoupled from shape and supports the creation of volumetric active matter with dynamic optical feedback.

Core claim

SBRIP particles achieve propulsion through direct momentum transfer from asymmetric light refraction. Internal refractive-index gradients provide optical symmetry breaking independent of external shape. Geometrically symmetry-broken particles with a homogeneous refractive index are another special case, where propulsion originates from refractive contrast at the boundary instead of within the particle. Unlike conventional systems relying on absorption or reflection, this transparency-based mechanism minimizes heating and mitigates shadowing in bulk suspensions.

What carries the argument

The symmetry-broken refractive index profile (SBRIP), an internal gradient that refracts incoming light asymmetrically to produce net momentum transfer and sustained directed motion.

If this is right

  • Propulsion occurs for particles whose external shape is perfectly symmetric.
  • High transparency permits light to penetrate thick suspensions without strong shadowing.
  • Heating remains low because propulsion does not require absorption.
  • Volumetric active matter becomes feasible, with particles reorganizing throughout a three-dimensional volume.
  • Light-driven particle motion can create a feedback loop that modulates the local refractive index of the material.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Particles of this type could be packed into dense volumes where collective motion alters the overall light transmission in a self-consistent way.
  • The same internal-asymmetry principle might be tested at other wavelengths or with non-optical waves to check generality.
  • Systematic variation of the internal gradient strength in printed particles would reveal how propulsion force scales with the degree of symmetry breaking.

Load-bearing premise

The 3D-printed refractive index profiles can be realized with enough spatial precision and stability that the intended internal asymmetry produces a measurable net force over fabrication imperfections or scattering.

What would settle it

Fabricating particles with the designed internal index gradient but symmetric outer shape and measuring no net propulsion velocity under uniform illumination would falsify the momentum-transfer mechanism.

Figures

Figures reproduced from arXiv: 2604.14917 by Adrian Paskert, Cornelia Denz, Elena Vinnemeier, Ivan Kalthoff, Jesco Sch\"onfelder, J\"org Imbrock, Julian Jeggle, Marcel Rey, Matthias R\"uschenbaum, Raphael Wittkowski.

Figure 1
Figure 1. Figure 1: FIG. 1. Design and fabrication of symmetry-broken refractive [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Reorientation of SBRIP particles under illumination from below. Top row: schematic side views illustrating the [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Simulation results for the forces and torques acting on particles with the shape of a [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Lateral trajectories of propelled [PITH_FULL_IMAGE:figures/full_fig_p009_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Mean squared displacement of propelled microparticles (sphere, hemisphere, cap, cone, and cornet) as a function of [PITH_FULL_IMAGE:figures/full_fig_p010_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Forces and torque acting on [PITH_FULL_IMAGE:figures/full_fig_p010_6.png] view at source ↗
read the original abstract

Active colloidal microparticles require reliable actuation to sustain directed motion. Light-based propulsion is particularly attractive as it provides persistent energy supply and enables direct spatiotemporal control. Here, we introduce 3D-printable particles with symmetry-broken refractive index profiles (SBRIP particles) that achieve propulsion through direct momentum transfer from asymmetric light refraction. Internal refractive-index gradients provide optical symmetry breaking independent of external shape, fundamentally decoupling propulsion from particle geometry. Geometrically symmetry-broken particles with a homogeneous refractive index are another special case, where propulsion originates from refractive contrast at the boundary instead of within the particle. Unlike conventional systems relying on absorption or reflection, this transparency-based mechanism minimizes heating and mitigates shadowing in bulk suspensions. We present a theoretical framework for refractive propulsion as well as numerical simulations of the SBRIP particles using raytracing and the finite volume method. This is complemented by experiments, validating the momentum transfer mechanism using particles with geometric symmetry breaking. The high transparency of our particles ensures deep light penetration, enabling the realization of volumetric active matter. This opens pathways toward adaptive nonlinear optical materials where light-driven particle reorganization modulates the local refractive index, establishing a dynamic feedback loop between the optical field and the material structure.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The manuscript introduces 3D-printable symmetry-broken refractive index profile (SBRIP) microparticles that achieve directed propulsion through asymmetric refraction of light, with internal refractive-index gradients providing the symmetry breaking independent of external particle shape. It develops a theoretical framework for refractive momentum transfer, presents ray-tracing and finite-volume method simulations for SBRIP particles, and reports experiments validating the underlying mechanism on geometrically asymmetric particles with homogeneous refractive index. The transparency of the particles is emphasized for enabling volumetric active matter and adaptive optical materials.

Significance. If the internal-gradient mechanism is confirmed, the work would offer a notable advance in optical actuation of colloids by decoupling propulsion from geometry and minimizing heating, supporting applications in bulk suspensions and dynamic refractive-index materials. The theoretical framework, combined simulations, and experimental check on the geometric case provide a solid foundation for the momentum-transfer concept.

major comments (2)
  1. [Abstract and experimental validation] The central claim that internal refractive-index gradients enable propulsion independent of external shape is supported only by ray-tracing and FVM simulations; the experiments are restricted to geometrically symmetry-broken particles with uniform index. This gap means the decoupling remains a prediction rather than a demonstrated result, and the abstract and conclusions should explicitly distinguish the validated geometric case from the simulated SBRIP case.
  2. [Numerical simulations section] At micron scales, the geometric-optics approximation in the ray-tracing simulations may be affected by diffraction or scattering at internal interfaces; a quantitative assessment of the validity range or a comparison to wave-optics methods is needed to support the force predictions for SBRIP particles.
minor comments (1)
  1. [Theoretical framework] The notation for refractive-index profiles and the definition of the symmetry-breaking parameter could be clarified with an explicit equation or diagram early in the theoretical framework.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive comments and positive overall assessment of the manuscript. We address each major comment below, indicating the revisions we will implement.

read point-by-point responses
  1. Referee: [Abstract and experimental validation] The central claim that internal refractive-index gradients enable propulsion independent of external shape is supported only by ray-tracing and FVM simulations; the experiments are restricted to geometrically symmetry-broken particles with uniform index. This gap means the decoupling remains a prediction rather than a demonstrated result, and the abstract and conclusions should explicitly distinguish the validated geometric case from the simulated SBRIP case.

    Authors: We agree that the experiments validate the refractive momentum-transfer mechanism only for geometrically symmetry-broken particles with homogeneous refractive index, whereas propulsion via internal refractive-index gradients in SBRIP particles is supported by ray-tracing and FVM simulations. We will revise the abstract and conclusions to explicitly distinguish these cases, stating that experimental validation applies to the geometric analog while the internal-gradient decoupling is a numerical prediction. This change will accurately reflect the scope of the results without overstating the experimental evidence. revision: yes

  2. Referee: [Numerical simulations section] At micron scales, the geometric-optics approximation in the ray-tracing simulations may be affected by diffraction or scattering at internal interfaces; a quantitative assessment of the validity range or a comparison to wave-optics methods is needed to support the force predictions for SBRIP particles.

    Authors: We acknowledge that diffraction and scattering could become relevant at micron scales. Our simulations target particle feature sizes of several tens of microns with visible wavelengths, placing the system well within the geometric-optics regime (size parameter >> 1). To address the concern directly, we will add a quantitative validity assessment in the numerical simulations section, including an estimate of diffraction effects via the size parameter and a comparison of ray-tracing forces against a wave-optics (FDTD) calculation for a representative 2D SBRIP cross-section. This will confirm the accuracy of the reported propulsion forces. revision: yes

Circularity Check

0 steps flagged

No circularity: derivation rests on external physical principles and independent validation

full rationale

The paper grounds refractive propulsion in standard momentum transfer from asymmetric light refraction, a first-principles optical principle independent of the SBRIP design. The theoretical framework applies ray-tracing and finite-volume methods directly to the prescribed internal refractive-index profiles to compute net forces, without fitting any parameter to the target propulsion result and then relabeling it as a prediction. Experiments on geometrically asymmetric homogeneous-index particles provide separate confirmation of the underlying mechanism, while the SBRIP internal-gradient case is presented as a simulation-based prediction rather than a tautology. No self-definitional equations, fitted-input predictions, load-bearing self-citations, or smuggled ansatzes appear in the derivation chain; the decoupling from external geometry follows from the model inputs rather than reducing to them by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The framework rests on standard ray-optics momentum transfer and the assumption that the printed particles maintain the designed refractive-index distribution without significant scattering or absorption.

axioms (2)
  • standard math Light propagation can be modeled by geometric ray tracing with momentum transfer at refractive-index interfaces.
    Invoked in the theoretical framework and ray-tracing simulations described in the abstract.
  • domain assumption The fabricated particles exhibit negligible absorption and scattering so that propulsion arises purely from refraction.
    Stated as the transparency-based mechanism that minimizes heating and shadowing.

pith-pipeline@v0.9.0 · 5566 in / 1281 out tokens · 29459 ms · 2026-05-10T10:34:48.196714+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

99 extracted references · 99 canonical work pages

  1. [1]

    Simulation of the light propagation Since the particle dimensions are much larger than the illumination wavelength, we describe light propagation within the framework of geometrical optics and model the incident light field as an ensemble of rays. In a medium with a continuous refractive index profilen(⃗ r), ray tra- jectories⃗ r(s) follow the Eikonal equ...

  2. [2]

    (2) was integrated numerically

    Simulation of the particle motion To obtain the physical trajectories of the SBRIP parti- cles, the stochastic equation of motion defined in Eq. (2) was integrated numerically. For this, we employed the Euler-Maruyama method to advance the system in dis- crete time steps ∆t. At each iterationi, the generalized position vector ⃗ris updated according to the...

  3. [3]

    (8), we compute the hydrodynamic force and torque resulting from prescribed translational and rotational motions of the particle in Stokes flow

    Calculation of the hydrodynamic resistance matrix To determine the resistance matrixHin Eq. (8), we compute the hydrodynamic force and torque resulting from prescribed translational and rotational motions of the particle in Stokes flow. Specifically, six simulations are performed: three unit translations along the Carte- sian basis vectors and three unit ...

  4. [4]

    Two-photon polymerization Two-photon polymerization (TPP) of the SBRIP par- ticles is carried out in a custom-built setup using a pulsed femtosecond laser (FemtoFiber Pro, Toptica) operating at a central wavelength of 780 nm and a repetition rate of 80 MHz. The beam is expanded and directed via a dichroic mirror into a 100×oil immersion objective (CFI Pla...

  5. [5]

    3D printing of SBRIP particles SBRIP particles with the geometries shown in Fig. 1a are 3D printed, including spheres (radiusr= 4µm), hemispheres (r= 5µm), cones (r= 5µm, heighth= 5µm), caps (r= 5µm, radius of the spherical cutout rcut = 3µm), and cornets (r= 5µm,h= 5µm, ra- diusr cut = 3µm and heighth cut = 3µm of the conical cutout). The reduced radius ...

  6. [6]

    Particle propulsion Particle propulsion experiments are conducted using an inverted microscope (Eclipse Ti, Nikon) coupled to a continuous-wave near-infrared laser (Smart Laser Sys- tems) operating at 1064 nm with an output power of up to 2.5 W. The Gaussian laser beam is enlarged, collimated, coupled into the microscope, and directed through a 20× object...

  7. [7]

    1a) both experimentally and numerically

    Particle propulsion To evaluate the propulsion capabilities of SBRIP par- ticles, we investigated the dynamics of spheres, hemi- spheres, caps, cones, and cornets as five distinct geome- tries (Fig. 1a) both experimentally and numerically. For the experiments, particles of these shapes were fabricated A Shape-symmetry-broken particles 7 c d ba 0 s 7 s 9 s...

  8. [8]

    Trajectories To characterize the particle motion under illumination, we analyze both experimental and simulated trajecto- ries of SBRIP particles. In the experiments, individual particle trajectories are obtained from video microscopy, while in the simulations the particle motion is computed using the optical forces derived in the previous section to- get...

  9. [9]

    The angu- lar dependence of the corresponding optical forces and torque obtained from ray-tracing simulations is shown in Fig

    Polymer-based particles To demonstrate the possibility of particle propulsion using only a symmetry-breaking refractive-index gradi- ent, we consider a spherical particle with an axial GRIN profile but no geometric symmetry breaking. The angu- lar dependence of the corresponding optical forces and torque obtained from ray-tracing simulations is shown in F...

  10. [10]

    The simulation results in Fig

    show that this gradient strength does not lead to a noticeable increase in propulsion as the MSD of particles with a gradient index fall within the error range of that of a homogeneous particle. The simulation results in Fig. 6dmatch this observation for the case of the parallel gra- dient direction and show that even a five-fold increase in gradient stre...

  11. [11]

    By utilizing subwavelength gratings, it is possible to tune the refractive index between that of Silicon (n≈3.5) and that of Silicon oxide (n≈1.45) [87]

    Silicon-based particles While we were not able to construct a particle without a symmetry-breaking in the shape of the particle from Ormocomp that is continuously moving in the experi- ments, numerical simulations suggest that such a feat should be possible using Silicon-based particles with a photonic metastructure that acts as a linear refractive index ...

  12. [12]

    Bechinger, C.et al.Active particles in complex and crowded environments.Rev. Mod. Phys.88, 045006 (2016)

  13. [13]

    & Wittkowski, R

    te Vrugt, M. & Wittkowski, R. Metareview: a survey of active matter reviews.Eur. Phys. J. E48, 12 (2025)

  14. [14]

    Phys.: Condens

    Gompper, G.et al.The 2025 motile active matter roadmap.J. Phys.: Condens. Matter37, 143501 (2025)

  15. [15]

    C.et al.Hydrodynamics of soft active matter.Rev

    Marchetti, M. C.et al.Hydrodynamics of soft active matter.Rev. Mod. Phys.85, 1143–1189 (2013)

  16. [16]

    & Schimansky-Geier, L

    Romanczuk, P., B¨ ar, M., Ebeling, W., Lindner, B. & Schimansky-Geier, L. Active Brownian particles.Eur. Phys. J. Spec. Top.202, 1–162 (2012)

  17. [17]

    A., Valeriani, C

    Mallory, S. A., Valeriani, C. & Cacciuto, A. An active approach to colloidal self-assembly.Annual Review of Physical Chemistry69, 59–79 (2018)

  18. [18]

    Manoharan, V. N. Colloidal matter: Packing, geometry, and entropy.Science349, 1253751 (2015)

  19. [19]

    & Zhang, L

    Yu, J., Wang, B., Du, X., Wang, Q. & Zhang, L. Ultra- extensible ribbon-like magnetic microswarm.Nat. Com- mun.9, 3260 (2018)

  20. [20]

    Viewpoint: From responsive to adaptive and interactive materials and materials systems: A roadmap

    Walther, A. Viewpoint: From responsive to adaptive and interactive materials and materials systems: A roadmap. Adv. Mater.32, 1905111 (2020)

  21. [21]

    J., van der Wiel, W

    Kaspar, C., Ravoo, B. J., van der Wiel, W. G., Wegner, S. V. & Pernice, W. H. P. The rise of intelligent matter. Nature594, 345–355 (2021)

  22. [22]

    & Cichos, F

    Wang, X. & Cichos, F. Harnessing synthetic active par- ticles for physical reservoir computing.Nat. Commun. 15, 774 (2024)

  23. [23]

    J., Kaliakatsos, I

    Nelson, B. J., Kaliakatsos, I. K. & Abbott, J. J. Mi- crorobots for minimally invasive medicine.Annu. Rev. Biomed. Eng.12, 55–85 (2010)

  24. [24]

    & S´ anchez, S

    Soler, L. & S´ anchez, S. Catalytic nanomotors for envi- ronmental monitoring and water remediation.Nanoscale 6, 7175–7182 (2014)

  25. [25]

    & J¨ anis, J

    Safdar, M., Simmchen, J. & J¨ anis, J. Light-driven micro- and nanomotors for environmental remediation.Environ. Sci.: Nano4, 1602–1616 (2017)

  26. [26]

    & Simmchen, J

    Xiao, Z., Voigtmann, M. & Simmchen, J. Biomimetic chemotactic motion of self-assembling doublet micro- robots.Adv. Intell. Syst.7, 2400839 (2025)

  27. [27]

    Di Leonardo, R.et al.Bacterial ratchet motors.Proc. Natl. Acad. Sci. U.S.A.107, 9541–9545 (2010)

  28. [28]

    S., Cannarsa, M

    Pellicciotta, N., Bagal, O. S., Cannarsa, M. C., Bianchi, S. & Di Leonardo, R. Wall torque controls propulsion of curved microstructures in bacterial baths.Phys. Rev. Lett.135, 138302 (2025)

  29. [29]

    ACS Nano19, 24174–24334 (2025)

    Ju, X.et al.Technology roadmap of micro/nanorobots. ACS Nano19, 24174–24334 (2025)

  30. [30]

    & Katuri, J

    S´ anchez, S., Soler, L. & Katuri, J. Chemically pow- ered micro- and nanomotors.Angew. Chem. Int. Ed. 54, 1414–1444 (2015)

  31. [31]

    Ebbens, S., Jones, R. A. L., Ryan, A. J., Golestanian, R. & Howse, J. R. Self-assembled autonomous runners and tumblers.Phys. Rev. E82, 015304 (2010)

  32. [32]

    & Poon, W

    Brown, A. & Poon, W. Ionic effects in self-propelled pt-coated janus swimmers.Soft Matter10, 4016–4027 (2014)

  33. [33]

    Moran, J. L. & Posner, J. D. Phoretic self-propulsion. Annu. Rev. Fluid Mech.49, 511–540 (2017)

  34. [34]

    R., Bet, B., van Roij, R., Dijkstra, M

    Vutukuri, H. R., Bet, B., van Roij, R., Dijkstra, M. & Huck, W. T. S. Rational design and dynamics of self- propelled colloidal bead chains: from rotators to flagella. Sci. Rep.7, 16758 (2017)

  35. [35]

    & Villa, K

    Ferrer Campos, R., Bachimanchi, H., Volpe, G. & Villa, K. Bubble-propelled micromotors for ammonia genera- tion.Nanoscale15, 15785–15793 (2023)

  36. [36]

    & Sen, A

    Illien, P., Golestanian, R. & Sen, A. ‘Fuelled’ motion: phoretic motility and collective behaviour of active col- loids.Chem. Soc. Rev.46, 5508–5518 (2017)

  37. [37]

    & Zhang, X

    Xu, T., Xu, L.-P. & Zhang, X. Ultrasound propulsion of micro-/nanomotors.Appl. Mater. Today9, 493–503 (2017)

  38. [38]

    & Fischer, P

    Ghosh, A. & Fischer, P. Controlled propulsion of artificial magnetic nanostructured propellers.Nano Lett.9, 2243– 2245 (2009)

  39. [39]

    Palacci, J., Sacanna, S., Vatchinsky, A., Chaikin, P. M. & Pine, D. J. Photoactivated colloidal dockers for cargo transportation.J. Am. Chem. Soc.135, 15978–15981 (2013)

  40. [40]

    & Sitti, M

    Yigit, B., Alapan, Y. & Sitti, M. Programmable collec- tive behavior in dynamically self-assembled mobile mi- crorobotic swarms.Adv. Sci.6, 1801837 (2019)

  41. [41]

    & Sitti, M

    Gardi, G., Ceron, S., Wang, W., Petersen, K. & Sitti, M. Microrobot collectives with reconfigurable morphologies, behaviors, and functions.Nat. Commun.13, 2239 (2022)

  42. [42]

    Adv.6, eaba5855 (2020)

    Magdanz, V.et al.Ironsperm: Sperm-templated soft magnetic microrobots.Sci. Adv.6, eaba5855 (2020)

  43. [43]

    & Volpe, G

    Gentili, A., Klages, R. & Volpe, G. Anomalous dynamics of superparamagnetic colloidal microrobots with tailored statistics.Small21, e06538 (2025)

  44. [44]

    Barroso, A.et al.Optical assembly of bio-hybrid micro- robots.Biomedical Microdevices17, 26 (2015)

  45. [45]

    & Isa, L

    van Baalen, C., Ketzetzi, S., Tintor, A., Gabay, I. & Isa, L. Gating and tunable confinement of active colloids within patterned environments.Soft Matter21, 3850– 3858 (2025)

  46. [46]

    & Isa, L

    van Kesteren, S., Alvarez, L., Arrese-Igor, S., Alegria, A. & Isa, L. Self-propelling colloids with finite state dy- namics.Proc. Natl. Acad. Sci. U.S.A.120, e2213481120 (2023)

  47. [47]

    Ketzetzi, S.et al.Self-reconfiguring colloidal active mat- ter (2025)

  48. [48]

    Tanuku, V. M. S. G., Vogel, P., Palberg, T. & Buttinoni, I. Island hopping of active colloids.Soft Matter19, 5452–5458 (2023)

  49. [49]

    & Volpe, G

    Rey, M., Volpe, G. & Volpe, G. Light, matter, action: Shining light on active matter.ACS Photonics10, 1188– 1201 (2023). 14

  50. [50]

    & K¨ all, M

    ˇS´ ıpov´ a-Jungov´ a, H., Andr´ en, D., Jones, S. & K¨ all, M. Nanoscale inorganic motors driven by light: Principles, realizations, and opportunities.Chem. Rev.120, 269– 287 (2020)

  51. [51]

    Active colloids moving by critical demix- ing

    Schmidt, F. Active colloids moving by critical demix- ing. InActive Colloids: From Fundamentals to Frontiers (Royal Society of Chemistry, Cambridge, 2024)

  52. [52]

    Yang, W., Wang, X., Wang, Z., Liang, W. & Ge, Z. Light-powered microrobots: Recent progress and future challenges.Opt. Lasers Eng.161, 107380 (2023)

  53. [53]

    K., Kumar, M

    Vardhan, R. K., Kumar, M. & Xavier, J. Light-driven micro/nanobots.Nanophotonics14, 4821–4874 (2025)

  54. [54]

    & Cichos, F

    Khadka, U., Holubec, V., Yang, H. & Cichos, F. Active particles bound by information flows.Nat. Commun.9, 3864 (2018)

  55. [55]

    & Yang, H

    Qian, B., Montiel, D., Bregulla, A., Cichos, F. & Yang, H. Harnessing thermal fluctuations for purposeful activities: the manipulation of single micro-swimmers by adaptive photon nudging.Chem. Sci.4, 1420 (2013)

  56. [56]

    K¨ ummel, F.et al.Circular motion of asymmetric self- propelling particles.Phys. Rev. Lett.110, 198302 (2013)

  57. [57]

    Buttinoni, I.et al.Dynamical clustering and phase sepa- ration in suspensions of self-propelled colloidal particles. Phys. Rev. Lett.110, 238301 (2013)

  58. [58]

    & Grelet, E

    Truong, H., Moretti, C., Buisson, L., Ab´ ecassis, B. & Grelet, E. Light-activated self-thermophoretic Janus nanopropellers.Nanoscale(2026)

  59. [59]

    & Bechinger, C

    Heuthe, V.-L., Iyer, P., Gompper, G. & Bechinger, C. Tunable colloidal swarmalators with hydrodynamic cou- pling.Nat. Commun.16, 10984 (2025)

  60. [60]

    & Bechinger, C

    Knippenberg, T., Bebon, R., Speck, T. & Bechinger, C. Negative drag force on beating flagellar-shaped bodies in active fluids.Phys. Rev. Lett.135, 118301 (2025)

  61. [61]

    Mater.15, 647–653 (2016)

    Palagi, S.et al.Structured light enables biomimetic swimming and versatile locomotion of photoresponsive soft microrobots.Nat. Mater.15, 647–653 (2016)

  62. [62]

    P., Pine, D

    Palacci, J., Sacanna, S., Steinberg, A. P., Pine, D. J. & Chaikin, P. M. Living crystals of light-activated colloidal surfers.Science339, 936–940 (2013)

  63. [63]

    R., Lisicki, M., Lauga, E

    Vutukuri, H. R., Lisicki, M., Lauga, E. & Vermant, J. Light-switchable propulsion of active particles with re- versible interactions.Nat. Commun.11, 2628 (2020)

  64. [64]

    & Simmchen, J

    Wang, L., Kaeppler, A., Fischer, D. & Simmchen, J. Pho- tocatalytic tio 2 micromotors for removal of microplastics and suspended matter.ACS Appl. Mater. Interfaces11, 32937–32944 (2019)

  65. [65]

    G., Pagonabarraga, I

    Boniface, D., Leyva, S. G., Pagonabarraga, I. & Tierno, P. Clustering induces switching between phoretic and os- motic propulsion in active colloidal rafts.Nat. Commun. 15, 5666 (2024)

  66. [66]

    Express21, 581–593 (2013)

    Palima, D.et al.Optical forces through guided light deflections.Opt. Express21, 581–593 (2013)

  67. [67]

    A., Peterson, T

    Swartzlander, G. A., Peterson, T. J., Artusio-Glimpse, A. B. & Raisanen, A. D. Stable optical lift.Nat. Pho- tonics5, 48–51 (2011)

  68. [68]

    B´ uz´ as, A.et al.Light sailboats: Laser driven autonomous microrobots.Appl. Phys. Lett.101, 041111 (2012)

  69. [69]

    Y.et al.Plasmonic linear nanomotor using lateral optical forces.Sci

    Tanaka, Y. Y.et al.Plasmonic linear nanomotor using lateral optical forces.Sci. Adv.6, eabc3726 (2020)

  70. [70]

    Nan- otechnol.16, 970–974 (2021)

    Andr´ en, D.et al.Microscopic metavehicles powered and steered by embedded optical metasurfaces.Nat. Nan- otechnol.16, 970–974 (2021)

  71. [71]

    Nanotech- nol.17, 477–484 (2022)

    Wu, X.et al.Light-driven microdrones.Nat. Nanotech- nol.17, 477–484 (2022)

  72. [72]

    & K¨ all, M

    Shanei, M., Wang, G., Johansson, P., Volpe, G. & K¨ all, M. Harnessing photon recoil for enhanced torque on light- driven metarotors.Nano Lett.25, 4832–4837 (2025)

  73. [73]

    Appl.14, 38 (2025)

    Engay, E.et al.Transverse optical gradient force in un- tethered rotating metaspinners.Light Sci. Appl.14, 38 (2025)

  74. [74]

    Commun.16, 7767 (2025)

    Wang, G.et al.Microscopic geared metamachines.Nat. Commun.16, 7767 (2025)

  75. [75]

    M., Engay, E

    Shanei, M. M., Engay, E. & K¨ all, M. Light-driven trans- port of microparticles with phase-gradient metasurfaces. Opt. Lett.47, 6428–6431 (2022)

  76. [76]

    & Basak, M

    Mitra, S. & Basak, M. Recent trends in non-reactive light driven micro/-nano propellers and rotors.Appl. Mater. Today31, 101748 (2023)

  77. [77]

    Man, W.et al.Optical nonlinearities and enhanced light transmission in soft-matter systems with tunable polar- izabilities.Phys. Rev. Lett.111, 218302 (2013)

  78. [78]

    Wensink, H. H. & L¨ owen, H. Emergent states in dense systems of active rods: from swarming to turbulence.J. Phys.: Condens. Matter24, 464130 (2012)

  79. [79]

    & Gompper, G

    Yang, Y., Marceau, V. & Gompper, G. Swarm behavior of self-propelled rods and swimming flagella.Phys. Rev. E82, 031904 (2010)

  80. [80]

    Cohen, J. A. & Golestanian, R. Emergent cometlike swarming of optically driven thermally active colloids. Phys. Rev. Lett.112, 068302 (2014)

Showing first 80 references.