A Device Realizing the Inverse Doppler Effect
A Doppler effect and device technology, applied in the field of electromagnetic wave devices, can solve problems such as limited frequency band, complex structure, difficult experimental detection, etc., and achieve a wide range of applications.
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[0028] Such as figure 1 As shown, the whole device is composed of a cylindrical inner sleeve (1) with a radius a and a cylindrical outer sleeve (2) with a radius b. The area between the inner sleeve (1) and the outer sleeve (2) is filled with an anisotropic inhomogeneous electromagnetic medium related to the geometric size of the device, and its relative permittivity and permeability are both second-order tensors . In the cylindrical coordinate system, it can be described by a matrix
[0029] ε=[ε rr ,ε rθ ,ε rz ;ε θr ,ε θθ ,ε θz ;ε zr ,ε zθ ,ε zz ],μ=[μ rr ,μ rθ ,μ rz μ θr ,μ θθ ,μ θz μ zr ,μ zθ ,μ zz ]. To implement our device, these parameter components are specifically required as follows:
[0030] ε rr =μ rr =ε zz =μ zz = 1,
[0031] ε rθ =μ rθ =ε θr =μ θr =rπ / (a-b),
[0032] ε θθ =μ θθ =1+r 2 π 2 / (b-a) 2 ,
[0033] ε rz =μ rz =ε zr =μ zr =ε θz =μ θz =ε zθ =μ zθ =0.
[0034] Wherein, a is the radius of the inner sleeve (1), b...
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