A Tunable Optical Switch Based on Array Plasma Columns
A plasma and plasma technology, applied in the field of tunable optical switches, can solve the problems of small adjustable degree of freedom and uncontrollable Fano resonance frequency
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Embodiment 1
[0023] This embodiment provides a tunable optical switch based on an array plasma column, such as figure 1 , including: a metasurface with a thickness smaller than the working wavelength, the metasurface is a regular geometric shape, and at least 3 plasma columns are distributed in parallel and equidistantly in the metasurface;
[0024] The Mie scattering coefficient of a single plasma column is obtained by using the Mie scattering theory, and the interference between the Mie scattering of a single plasma column and the Bragg scattering generated by the array plasma column produces a Fano resonance phenomenon;
[0025] The material of the metasurface is cladding quartz tube and plasma column.
[0026] Specifically, the metasurface is rectangular, and the geometric parameters of all plasma columns are exactly the same.
[0027] Specifically, the geometric parameters of the metasurface, the radius r of the quartz tube 1 =1.0mm plasma radius r 1 =0.66mm metasurface period p = ...
Embodiment 2
[0041] This embodiment is based on implementation 1, and the established parameters are d=3.9mm, r 1 =1.0mm,r 2 =0.66mm,n e =2.0×10 12 cm -3 At the same time, the simulation software based on the finite element method is used for numerical and analytical calculation of the period p, and the results are as follows Figure 5 , is the relationship between the transmission coefficient and the frequency when the parameter p changes.
[0042] Figure 5 It shows that when 10.0mm
Embodiment 3
[0044] This example is based on Example 1, and establishes parameters p=18.0mm, r 1 =1.0mm,r 2 =0.66mm,n e =2.0×10 12 cm -3 At the same time, the simulation software based on the finite element method is used for numerical and analytical calculation of d. The results are as follows Image 6 , is the relationship between the transmission coefficient and the frequency when the parameters are changed.
[0045] Image 6 It shows that with the increase of d, the resonance frequency redshifts, but the redshift trend of 2.0mm
[0046] It can be seen from the above embodiments that the resonance frequency of the Fano resonance can be tuned by changing the geometric parameters, but the tuning frequency range is far less than the tuning frequency range obtained by changing the plasma density, which is convenient.
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