Deep sub-wavelength size non-reciprocal emission/absorption device construction method and system
A deep subwavelength, non-reciprocal technology, used in nonlinear optics, instruments, optics, etc., can solve problems such as performance needs to be improved, and achieve the effect of reducing the geometric size of the structure, solving the larger size, and reducing the size of the structure
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Embodiment example 1
[0087] In the presence of an external magnetic field, Kirchhoff's law of thermal radiation is broken, and at the same incident angle, the absorption ratio and emissivity are no longer equal. The invention proposes to completely break Kirchhoff's law by exciting the Berreman mode of the near-zero material layer and increasing the difference between the absorption ratio and the emissivity. Figure 4 for the invention figure 1 The emissivity and absorptivity of the near-zero material with different thicknesses as a function of incident angle and operating angular frequency of the double-layer structure when the applied magnetic field is 1T. For a specific implementation case, when the thickness of the near-zero material is 200nm and the incident angle is 40°, the difference between the absorption ratio and the emissivity can reach |Δ|=0.59; when the thickness of the near-zero material is 450nm, when the incident angle is 22.5°, The difference between the absorption ratio and the...
Embodiment example 2
[0091] According to the design principles proposed in the present invention, a sub-wavelength dielectric grating is added, and the design structure can support asymmetric Berreman mode and Epsilon-near-zero mode at the same time, which can realize multi-peak non-reciprocal emission. The thickness of the grating is 1.75 μm, width 3 μm, period 4.5 μm. For specific implementation cases, by using a grating structure to excite an asymmetric Epsilon-near-near mode, such as Figure 7 As shown, high emission and low absorption characteristics can be achieved under the same incident angle, and the position of the absorption peak is insensitive to the incident angle, and the angle condition only changes the height of the absorption peak. Figure 8 for the invention image 3 The change of the emission / absorption spectrum with the period size after adding the grating structure, the non-reciprocal emission and absorption characteristics realized by using the asymmetric Berreman mode are n...
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