Since Ashkin et al. [
Laser & Optoelectronics Progress, Volume. 61, Issue 5, 0536002(2024)
Spin of Micro-Propeller Structures Driven by High-Order Poincaré Beams
The use of light-induced micro-motors or micro-propellers, showcasing non-contact and non-damaging characteristics, is garnering increased attention in biomedical, micro-machine, and environmental fields. The High-order Poincaré (HOP) beam, as a vector beam, provides a controllable driving force with adjustable orbital angular momentum and spin angular momentum. In this study, we present the spin of a self-assembled micro-propeller structure propelled by the HOP beam, enabling flexible control over rotation velocity and direction. Our findings reveal that modifications to the total angular momentum of the driving beam field or alterations in the micro-propeller blade structure can influence rotation velocity. This research offers an efficient and versatile approach for applications in optical micromanipulation and micromachinery.
1 Introduction
Since Ashkin et al. [
Vector beams carries spin angular momentum(SAM)determined by polarization and orbital angular momentum(OAM)determined by topological charge[
In general,the driving force about rotation of micromotors or micro-propellers comes from the SAM and OAM of light. Changing the polarization state can control the SAM,which allows the spin velocity of the particle adjustable. However,the value of SAM can only be ±1,thereby imposing constrains on the velocity. By contrast,OAM is more flexible and can be extended to any integer or even fractional order,but the beam diameter is affected by the OAM. A larger OAM will yield a larger beam diameter,which may bring new challenges to the optical manipulation. Actually,the rotational motion can be divided into “spin” and “orbit” based on the rotating axis,but they are not necessarily confined to corresponding angular momentum of light. Here,we report a self-assembling propeller that is driven by a high order Poincaré(HOP)beam. We utilize the beam to assemble the micro-propeller under zero total angular momentum conditions,and to drive the micro-propeller to spin under non-zero total angular momentum conditions. By adjusting the blades of propeller and the total OAM of beam,the propeller rotating velocity can be controlled. Furthermore,since the total OAM of HOP beam depends on the optical field profile parameters instead of the topological charge,the diameter of beam keep constant,which yield the stable rotation of micro-propeller. Our work provides a flexible approach in micromanipulation and micromachinery.
2 Method
Theoretically,an arbitrary HOP beam is formed by superposition of two orthogonal conjugate circularly polarized LG beams whose orders are negative to each other [
where
where
Figure 1.(a) Experimental setup; (b)-(d) manipulated polystyrene on the loading platform with respect to two-, three- and four-blade structures
where three column Jones matrices represent the horizontal polarization,left- and right-hand circular polarization,respectively(from left to right). Next,the polarization modulated LG beam incident on vortex half wave plate(VHWP)of order
After passing through the VHWP,the right- and left-hand circular polarization will convert to each other,while the topologic charges are added
where
It is shown that the total OAM regulation of HOP beam depends on the optical field profile parameters instead of the topological charge,so the diameter of beam can be fixed in a constant.
In order to avoid not being able to clearly observe the particle rotation and calculate the rotation velocity due to high power,we set the 100× objective(MO,NA=1.25)power at 40 mW. After collimating through the two lenses,the laser beam successively passes through the HWP,the QWP,the VHWP of
3 Result
By adjusting the angle of HWP,we investigate the rotation velocity of the four-blade propeller under different total angular momentums,and the results are shown in
Figure 2.(a) Rotation of four-blade “propeller” at different α values and time. (the red rhombus denotes the entirety structure of propeller, and the red dot denotes the symmetry center); (b) different combinations of particle steering and α values angle relationship (positive is clockwise, negative is counterclockwise)
Furthermore,we measure the rotation velocities of two-,three- and four- blades “propeller” under different α values. The rotation process can be recorded as video and the rotation velocity is calculated by comparing the adjacent frames. Here,we repeated experiment for 4 times under each condition. As shown in
4 Analysis
To further explain that the rotation velocity of “propeller” is related to the quantity of blades,we conduct simulations of the interaction between different structural “propellers” and HOP beam. In general,the time average optical force acting on a particle can be obtained by considering the integral of Maxwell stress tensor surrounded by a closed surface of a particle:
where,
|
where,
When the light field interacts with the particle,it is also accompanied by the transfer of angular momentum,resulting in the particle being acted on by torque. For the particle distance from the optical axis
Six electromagnetic fields components(Ex,Ey,Ez,Hx,Hy,Hz)of HOP beam on the focal plane are imported into FDTD software. The particles with different microstructures are placed on focal plane,where the symmetry axis coincides with optical axis. Then the optical force and optical torque of the microstructures can be simulated by
Since the rotation occurs in xy-plane,the force distribution of two,three,four-blade micro-propeller with
Figure 3.Force distributions of (a) two-, (b) three- and (c) four-blade per unit volume with the same field when
Furthermore,to depict the stable spin rotation of propellers,the resistive forces caused by environment is considered. When the microstructure has size of
where
In experiments,the method to measure the rotation velocity follows the previous,so the maximum velocity,minimum velocity and average velocity can be obtained. The velocity of two-,three- and four-blade structures obtained from simulations and experiments are shown in
Figure 4.Theoretical and experimental rotational velocity of propellers self-assembled by two-, three- and four-blade (the line of experimental data denotes the range of velocity, and the dot of experimental data denotes the average velocity)
5 Conclusion
In summary,we demonstrate a light-indued self-assembled propellers to spin by a simple yet flexible method. The HOP beams,whose total angular momentum can be regulated without changing the beam diameter,is introduced to assemble and rotate particles. We found that the velocity control method for the self-assembled “propeller” is not single. Through experiments and simulations,the results reveal that the rotation velocity is controlled by HOP beam and self-assemble micro-structure simultaneously. Either changing the total angular momentum of driving field or changing the blade number of propeller can affect the rotation velocity. Our work may provide a simple and efficient approach for applications filed such as cell manipulation or micro-nano motors.
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Qian Lin, Lei Chen, Zikuan Zhuang, Jingxuan Sun, Li Zhang, Jianing Xie. Spin of Micro-Propeller Structures Driven by High-Order Poincaré Beams[J]. Laser & Optoelectronics Progress, 2024, 61(5): 0536002
Category: Letters
Received: Sep. 24, 2023
Accepted: Nov. 17, 2023
Published Online: Mar. 13, 2024
The Author Email: Zhang Li (zhangli4102@126.com), Xie Jianing (xiejianingfs@126.com)