Terahertz broadband absorber based on doped semiconductor with coating film
A semiconductor and terahertz technology, applied in the field of terahertz broadband absorbers, can solve the problems of size and bandwidth process complexity that are difficult to achieve a good balance, and there are few terahertz broadband absorbers, and achieve near-perfect anti-reflection and strong The effect of absorbing properties
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Embodiment 1
[0045] For the terahertz broadband absorber based on coating doped semiconductor of this embodiment, please refer to image 3(a) includes doped GaAs and PS (Polystyrene) coating, and the PS coating is arranged above the doped GaAs.
[0046] In the present embodiment, each parameter of doping GaAs is: ε GaAs =12.9+7.9×10 -28 ω 2 ;m * =0.079m 0 , m 0 is the free electron mass; τ=μm * / e, μ is the DC electron mobility, and μ changes with the carrier concentration n; n=10.3×10 16 cm -3 (mobility μ = 4000cm 2 V -1 the s -1 , n-type doping); the thickness is 300 μm.
[0047] see figure 2 (a), which is the refractive index dispersion curve of the doped GaAs of the present embodiment (wherein, n represents the real part, and k represents the imaginary part), it can be seen that the refractive index of the doped GaAs is shown as Drude dispersion, and a certain In the wavelength band, the condition of anomalous reflection phase dispersion is satisfied. see figure 2 (b),...
Embodiment 2
[0051] The frequency range of broadband absorption can be adjusted by changing the doping concentration of the semiconductor and the coating thickness. Changing the doping concentration of the semiconductor will change its refractive index, and at the same time, the reflection phase, reflection coefficient, and frequency range of the abnormal dispersion of the reflection phase will also change accordingly. Coatings with different thicknesses are designed to compensate for the reflection phase of doped semiconductors. Anomalous dispersion, so that the corresponding broadband anti-reflection can be realized.
[0052] The terahertz broadband absorber based on coating doped semiconductor in this embodiment is basically the same as that in Embodiment 1, except that the doping concentration of doped GaAs and the thickness of the PS coating are different.
[0053] Figure 4 (a) shows the doping concentration of doped GaAs was 3.1×10 16 cm -3 (μ=5500cm 2 V -1 the s -1 , n-type d...
Embodiment 3
[0055] For the terahertz broadband absorber based on coating doped semiconductor of this embodiment, please refer to Figure 5 (a) includes doped Si and PE (Polyethylene) coating, and the PE coating is arranged on the doped Si.
[0056] In the present embodiment, each parameter of doping Si is: ε Si =(3.415) 2 ; m * =0.26m 0 , m 0 is the mass of free electrons; doping concentration n=4×10 16 cm -3 (mobility μ = 4000cm 2 V -1 the s -1 , n-type doping); the thickness is 300 μm.
[0057] see figure 2 (c), which is the refractive index dispersion curve of the doped Si of the present embodiment (wherein, n represents the real part, and k represents the imaginary part), it can be seen that the refractive index of the doped Si is shown as Drude dispersion, and a certain In the wavelength band, the condition of anomalous reflection phase dispersion is satisfied. see figure 2 (d), which shows the reflectance and reflection phase of the terahertz wave from the air to the ...
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