Figures & data
Figure 1 Basic principles of optical tweezers.
Note: A particle is trapped in the potential well formed by dark solitons at the center wavelength, λ0.
![Figure 1 Basic principles of optical tweezers.Note: A particle is trapped in the potential well formed by dark solitons at the center wavelength, λ0.](/cms/asset/b3247d8e-ce33-433e-8513-214c1b08abe1/dijn_a_27417_f0001_c.jpg)
Figure 3 Results of dynamic optical tweezers generated at four different center wavelengths, where E1, E2, E3, and E4 are circulated in optical fields within the center ring resonator shown in (A), (B), (C), and (D), respectively. Et and Ed are output optical fields generated at the throughput and drop ports of the PANDA ring as shown in (E) and (F), respectively.
![Figure 3 Results of dynamic optical tweezers generated at four different center wavelengths, where E1, E2, E3, and E4 are circulated in optical fields within the center ring resonator shown in (A), (B), (C), and (D), respectively. Et and Ed are output optical fields generated at the throughput and drop ports of the PANDA ring as shown in (E) and (F), respectively.](/cms/asset/a12aad67-6d8e-41fa-beb5-fe9ceec1574e/dijn_a_27417_f0003_c.jpg)