2021
DOI: 10.1103/physrevlett.127.186803
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Toward Lossless Infrared Optical Trapping of Small Nanoparticles Using Nonradiative Anapole Modes

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Cited by 25 publications
(33 citation statements)
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“…The trapping energy was calculated using a line integral path of the optical force along the z -axis, defining U z = 0 at z = 160 nm (see Figure c). As demonstrated numerically in ref , the optical potentials depend on the nanoparticle refractive index and height above the nanodisk. Hence, the distance between two nanoparticles and the stiffness of their optical trapping can be manipulated.…”
Section: Resultsmentioning
confidence: 70%
See 1 more Smart Citation
“…The trapping energy was calculated using a line integral path of the optical force along the z -axis, defining U z = 0 at z = 160 nm (see Figure c). As demonstrated numerically in ref , the optical potentials depend on the nanoparticle refractive index and height above the nanodisk. Hence, the distance between two nanoparticles and the stiffness of their optical trapping can be manipulated.…”
Section: Resultsmentioning
confidence: 70%
“…Anapole states with orders higher than the first exhibit sharper resonances with stronger energy concentration, as observed experimentally . Although the electromagnetic hotspots from anapole resonances are normally found inside the elementary scatterers, recent research indicated localization at the external region using small slots in dielectric nanodisks. , This finding is the basis for lossless trapping of small nanoparticles using anapole modes, with optical forces to trap nanoparticles with radii as small as 15 nm …”
Section: Introductionmentioning
confidence: 71%
“…The defining nonradiating condition of the anapole relies on the fine balance between the constituent electric dipole and toroidal dipole excitations. Consequently, such excitations are expected to be highly sensitive to external perturbations including variations in the ambient refractive index [30][31][32]. Compared with conventional dipole modes with low transmission, anapole modes can acquire the effective transmission channel due to the nonradiative property, which is beneficial to practical low-loss sensors [25,33].…”
Section: Introductionmentioning
confidence: 99%
“…Under certain conditions, the destructive interference between dipole and toroidal moments may result in suppressed scattering accompanied by strongly enhanced near fields. The corresponding practically radiationless states are called anapole states. , The unique properties of anapole states reveal an exciting potential in many applications such as cloaking, , nanoscale lasers, field enhancements, , energy guiding, , harmonic generations, metamaterials, , and optical trapping …”
mentioning
confidence: 99%
“…3,4 The unique properties of anapole states reveal an exciting potential in many applications such as cloaking, 5,6 nanoscale lasers, 7 field enhancements, 8,9 energy guiding, 10,11 harmonic generations, 12−14 metamaterials, 1,15−17 and optical trapping. 18 It is important to emphasize that the far-field excitation of a pure nonradiating anapole state is problematic due to the reciprocity principle unless some specially designed illumination is used as, for instance, a combination of counterpropagating strongly focused radially polarized beams. 6,19 In practice, the formation of an anapole state is usually referred to when the suppression of a dominant (radiative) multipole moment is achieved.…”
mentioning
confidence: 99%