Method for controlling optical force which radial isotropic nanowire is subjected to
An anisotropic, nanowire technology, applied in the field of light manipulation, which can solve problems such as the study of optical power that does not involve anisotropic materials
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Embodiment 1
[0035] This embodiment provides a normal Rayleigh scattering, with ε r =ε t The nanowire with =5 is a comparative example, the nanowire with a radius of 100nm and a relative magnetic permeability of 1 is placed in a vacuum medium, and the wave vector k 1 =10 3 The plane wave excites the nanowire along the radial direction, and the acceleration of the particle at this time is measured, and then the wave vector k 1 =10 4 The plane wave excites the nanowire, the acceleration of the particle is measured at this time, and the acceleration change in this case is recorded. Mathematica software can also be used for numerical calculation, and the obtained data can be drawn with Origin software to intuitively summarize the law of light manipulation.
[0036] See attached figure 1 , it is the function relationship diagram between the acceleration of the isotropic nanowire and the wave vector provided by this embodiment, when the wave vector k 1 =10 3 (At this time Log...
Embodiment 2
[0041] In this example, an anisotropic nanowire under non-Rayleigh superscattering is taken as the research object, and the radius size r 0 is 100nm, the relative permeability is 1, and the permittivity satisfies (such as ε r =-5,ε t =-0.2) the nanowire is placed in a vacuum medium, the magnetic field is polarized along the axial direction, and the wave vector in the medium is k 1 The transverse magnetic wave is incident on the nanowire along the radial direction, when satisfying k 1 r 0 =10 -4 ~10 -3 Under the quasi-static approximation of , changing the wave vector k of the incident wave 1 ,
[0042] Press
[0043] a = F m = k 0 2 m Im [ α e + α m ] - k ...
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