2000
DOI: 10.1063/1.126232
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Manipulation of colloidal gold nanoparticles in the evanescent field of a channel waveguide

Abstract: Colloidal gold spheres of radius 10 nm are reported to move forward in water, under the influence of radiation pressure forces, due to the evanescent field at the surface of an optical channel waveguide. The velocity is linearly dependent upon the optical power in the waveguide, acquiring a maximum velocity of 4 μm/s for modal power of 500 mW in the TM polarization at a wavelength of λ=1.047 μm.

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Cited by 65 publications
(38 citation statements)
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“…Here we use the lower value as it is the most often cited value. The agreement between theory and experiment (speeds up to 384µm/s predicted, with speeds of 500µm/s observed) is much improved on previous calculations [4].…”
Section: Resultssupporting
confidence: 71%
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“…Here we use the lower value as it is the most often cited value. The agreement between theory and experiment (speeds up to 384µm/s predicted, with speeds of 500µm/s observed) is much improved on previous calculations [4].…”
Section: Resultssupporting
confidence: 71%
“…In order to compare this to theory we equate the Rayleigh optical forces to the Stokes' drag forces to predict the velocity [4]. The peak intensity in the evanescent field of the waveguide was estimated to be 9GW m −2 per Watt of propagating modal power, using beam propagation analysis (RSoft), for which the refractive index distribution was taken from slab waveguides formed under the same conditions, and knowledge of the waveguide diffusion width.…”
Section: Resultsmentioning
confidence: 99%
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“…Figure 3a,c shows the schematic of the corresponding experiment using the total internal reflection at a glass prism. For this numerical experiment, we use parameters corresponding to real experiments manipulating particles with evanescent fields (for example see refs [57][58][59][60][61][62]. Namely, we consider radiation with the wavelength l ¼ 650 nm, a gold particle (e p ¼ À 12.2 þ 3i, m p ¼ 1) in water (e ¼ 1.77, m ¼ 1), and near-critical total internal reflection (the angle of incidence is y ¼ 51°¼ y c þ 1.5°) from the interface between heavy flint glass (e 1 ¼ 3.06, m 1 ¼ 1) and water.…”
Section: Article Nature Communications | Doi: 101038/ncomms4300mentioning
confidence: 99%