Fig. 1. Schematic diagram of time-reversal theory

Fig. 2. Polarization state schematic within the tight focusing field. (a) Normalized intensity distribution within the tightly focused focal field; (b) schematic of the polarization orientation angle of vector beam, asterisk denotes the coordinate origin

Fig. 3. Illustration of ellipsoidal particle rotation parameters

Fig. 4. Normalized intensity distributions of vector beams with different polarization directions within the focal field range. (a) θ₀=0°, φ₀=0°; (b) θ₀=45°, φ₀=45°; (c) θ₀=90°, φ₀=0°; (d) θ₀=-30°, φ₀=-70°

Fig. 5. Three-dimensional projection distributions of vector beams with different polarization directions within the focal field range. (a) θ₀=0°, φ₀=0°; (b) θ₀=45°, φ₀=45°; (c) θ₀=90°, φ₀=0°; (d) θ₀=-30°, φ₀=-70°

Fig. 6. Light force distributions experienced by the ellipsoidal particles within the focal field range when vector beams with different polarization directions capture ellipsoidal particles. (a) θ₀=0°, φ₀=0°; (b) θ₀=45°, φ₀=45°; (c) θ₀=90°, φ₀=0°; (d) θ₀=-30°, φ₀=-70°

Fig. 7. Distributions of gradient force F_grad, radiation force F_radi and total force F_total in different when the ellipsoidal particle is trapped by vector beams polarized along direction θ₀=0°, φ₀=0°. (a) xy plane; (b) xz plane;(c) yz plane

Fig. 8. Trapping potential distributions in focal plane of optical forces exerted on ellipsoidal particles when trapped by vector beams polarized along directions. (a) θ₀=0°, φ₀=0°; (b) θ₀=45°, φ₀=45°; (c) θ₀=90°, φ₀=0°; (d) θ₀=-30°, φ₀=-70°

Fig. 9. Relationship between trapping potential and polar angle Θ0 and azimuthal angle Φ0 of ellipsoidal particles stably trapped by vector beams polarized along directions. (a) θ₀=0°, φ₀=0°; (b) θ₀=45°, φ₀=45°; (c) θ₀=90°, φ₀=0°; (d) θ₀=-30°, φ₀=-70°; (e) schematic diagram of the relationship between the spatial orientation of the ellipsoidal particle and the polarization state

Fig. 10. Distributions of torques and the directions of rotation of ellipsoidal particles stably trapped by vector beams polarized along directions. (a) θ₀=0°, φ₀=0°; (b) θ₀=45°, φ₀=45°; (c) θ₀=90°, φ₀=0°; (d) θ₀=-30°, φ₀=-70°

Fig. 11. Spatial orientation diagrams of ellipsoidal particles when trapped by vector beams with different polarization directions