Abstract

In this work, we demonstrate trapping of microparticles using plasmonic tweezers based on arrays of annular apertures. The transmission spectra and the electric-field distribution are simulated to calibrate the arrays. Theoretically, we observe sharp peaks in the transmission spectra for dipole resonance modes and these are red-shifted as the size of the annular aperture is reduced. We also expect an absorption peak at approximately 1115 m for the localised plasmon resonance. Using a laser frequency between the two resonances, multiple plasmonic hot spots are created and used to trap and transport micron and submicron particles. Experimentally, we demonstrate trapping of individual 0.5 μm and 1 μm polystyrene particles and the feasibility of particle transportation over the surface of the annular apertures using less than 1.5 mW μm−2 incident laser intensity at 980 nm.

Highlights

  • To address the problems associated with conventional optical tweezers for trapping objects in the Rayleigh regime, plasmonic tweezers (PTs) - which can confine the incident laser beam to the nm-scale - have been developed

  • The transmission of the trapping laser through the array was collected by a condenser (50 X, N.A = 0.55) and measured by an avalanche photodetector (APD) at 1 kHz frequency

  • The above hypothesis of trap stiffness self-adjustment with lower laser intensity excitation for S2 when compared to S1 and S3 is very similar to previous reports on the self-induced back action (SIBA) effect [13,14]

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Summary

Introduction

To address the problems associated with conventional optical tweezers for trapping objects in the Rayleigh regime, plasmonic tweezers (PTs) - which can confine the incident laser beam to the nm-scale - have been developed. These devices provide an alternative and robust technique for scaling optical trapping down to subwavelength particles [1,2,3,4,5,6]. Polystyrene beads with a minimum diameter of 200 nm have been successfully transported using a nano-optical conveyor belt [17, 18] Another major advantage of PTs is the tunability of the resonance frequency towards the near-infrared (NIR) region. While heating could be helpful, it should, be avoided for most PTs applications

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