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Resonant binding of dielectric particles to a metal surface without plasmonics

Evgeny Bulgakov1,2, Konstantin Pichugin1, and Almas Sadreev1

  • 1Kirensky Institute of Physics Federal Research Center KSC SB RAS, 660036 Krasnoyarsk, Russia
  • 2Reshetnev Siberian State University of Science and Technology, 660037 Krasnoyarsk, Russia

Phys. Rev. A 103, L051501 – Published 26 May, 2021

DOI: https://doi.org/10.1103/PhysRevA.103.L051501

Abstract

A high index dielectric spherical particle supports the high-Q resonant Mie modes that result in a regular series of sharp resonances in the radiation pressure. The presence of a perfectly conducting metal surface transforms the Mie modes into extremely high-Q magnetic bonding or electric antibonding modes for the close approach of a sphere to a surface. We show that an electromagnetic plane wave with normal incidence results in repulsive or attractive resonant optical forces relative to a metal for the excitation of electric bonding or magnetic antibonding resonant modes, respectively. A magnitude of resonant optical forces reaches the order of 1 nN of magnitude for micron-sized silicon particles and a power of light 1mW/μm2 that exceeds the gravitational force by four orders. However, what is the most remarkable is there are steady positions for a sphere between the pulling and pushing forces that give rise to the resonant binding of the sphere to a metal surface.

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