Resonant bending of silicon nanowires by light

Abstract

Coupling of two dielectric wires with rectangular cross-section gives rise to bonding and anti-bonding resonances. The latter is featured by extremal narrowing of the resonant width for variation of the aspect ratio of the cross-section and distance between wires when the morphology of the anti-bonding resonant mode approaches to the morphology of the Mie resonant mode of effective circular wire with high azimuthal index. Then plane wave resonant to this anti-bonding resonance gives rise to unprecedent enhancement of the optical forces up to several nano Newtons per micron length of wires. The forces oscillate with angle of incidence of plane wave but always try to repel the wires. If the wires are fixed at the ends the optical forces result in elastic deflection of wires of order $100nm$ for wires's length $50\mu m$ and the light power $1.5mW/\mu m^2$.

5 pages, 5 figures. arXiv admin note: text overlap with arXiv:2007.08721

References in corpus (5)

• High-Q supercavity modes in subwavelength dielectric resonators
• Formation of long-lived, scarlike modes near avoided resonance crossings in optical microcavities
• Pushing the Limit of High-Q Mode of a Single Subwavelength Dielectric Nanocavity
• Engineering of the extremely high Q factor in two subwavelength dielectric resonators
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Cited by in corpus (1)

• Enhancement of optical forces at bound state in the continuum