Plasmonic optical tweezers based on nanostructures fabricated on thin metal films have been studied as an alternative system to conventional optical tweezers for nanoparticle trapping and manipulation 1-3 . The incident laser beam can be confined beyond the diffraction limit at the nano-apertures and the intensity of the local field is significantly enhanced because of the surface plasmon resonance (SPR) phenomenon. The plasmonic resonance frequency can be tuned by modifying the dimensions of the nano-structures and the period of the array. This feature is especially beneficial for trapping biological particles. To minimize photo damage to a trapped particle, the resonance frequency can be shifted into the near infrared region (NIR) 4, 5 . Besides the enhanced local field intensity, the self-induced back-action (SIBA) effect can be used to enhance the trap stiffness with a red-shifted incident frequency 6, 7 .In this work, we demonstrate a plasmonic tweezers based on an array of nano-rings connected by nano-size slits. For each nano-ring structure, a coaxial inner disk is fabricated inside a nano-hole. A cylindrical surface plasmonic (CSP) resonance is generated at the aperture of the nano-ring and a transmission peak is observed 8 . This peak becomes narrower with the presence of the nano-slit. When the size of the aperture is reduced, this peak is redshifted. The trap stiffness is compared between two nanoring arrays with different diameters of inner disks. *xue.han@oist.jp, https://groups.oist.jp/light The SIBA effect is observed for the nano-ring array under the red-shifted incident laser condition. Combined with other sensing technologies, plasmonic tweezers based on these nano-ring arrays have huge potential as components in a lab-on-a-chip system.
II ExperimentThe array of nano-apertures is fabricated on a 50 nm gold thin film using a focused ion beam (FIB). More details of the fabrication process are described in our earlier work 9, 10 . Scanning electron microscope (SEM) images of the nano-ring arrays with 147.2 ± 9.7 nm and 187.3 ± 1.9 nm inner disks are shown in Fig. 1(a) and (b), respectively. The average diameter of the nano-hole is 293.3 ± 13.3 nm, the period is 361.2 ± 3.1 nm, and the width of the connecting slit is 39.6 ± 4.6 nm. The connecting slits are only fabricated along the vertical direction and horizontally polarized incident light is used for experiments.A finite-difference time-domain (FDTD) simulation is used to obtain the transmission spectra. Dimensions from SEM images are used for the simulation. As shown in Fig. 1(c), the CSP resonance peak is narrower for nano-ring arrays with 147.2 nm inner disks when connecting slits are present. With bigger inner disks, the CSP resonance peak is shifted towards the red. A Ti: Sapphire laser at 980 nm, which is red shifted for the nano-ring array with 147.2 nm inner disks and close to the resonance for the nano-ring array with 187.3 nm inner disks, is used for
AbstractPlasmonic tweezers based on nano-ring arrays on gold thin film are demonstrate...