米氏散射 Mie scattering
（重定向自MIE theory）
米式散射（Mie scattering），是一种光学现象，属于散射的一种情况。米式散射理论是由德国物理学家古斯塔夫·米于1908年提出的。
MIE theory
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Mie scattering 米氏散射
（重定向自MIE theory）
![Monostatic radar cross section [RCS] of a perfectly conducting metal sphere as a function of frequency (calculated by Mie theory). In the low frequency Rayleigh scattering limit where the circumference is less than the wavelength, the normalized RCS is σ/(πR2) ~ 9(kR)4. In the high frequency optical limit σ/(πR2) ~ 1](/uploads/202501/27/Radar_cross_section_of_metal_sphere_from_Mie_theory.svg2326.png)
The Mie solution to Maxwell's equations (also known as the Lorenz–Mie solution, the Lorenz–Mie–Debye solution or Mie scattering) describes the scattering of an electromagnetic plane wave by a homogeneous sphere. The solution takes the form of an infinite series of spherical multipole partial waves. It is named after Gustav Mie.
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