"scattering field" is a correct and usable phrase in written English.
It is typically used in the context of physics or electromagnetic field theory. "Scattering field" refers to the pattern of scattered energy or particles that result from the interaction of a wave or particle with an obstacle or medium. Example: In the experiment, the researchers observed how the scattering field changed when a different material was placed in front of the light source.
Various short-term fading distributions like Nakagami-m, Ricean and Rayleigh assume a resultant homogenous diffuse scattering field, from randomly distributed scatters.
The transition matrix relating the scattering field by a single subscatterer and an incident field is utilized for the multiple scattering analysis, but near-field interactions among subscatterers must be considered because of the closely packed arrangement of subscatterers.
Using this technique, the incident light can be effectively introduced by modifying the electromagnetic components in an inserted connecting region between the total field and the scattering field region with incident terms, where the incident terms are obtained by weighting the incident field by a window function.
Amplitudes of scattering field, E s, from positive and negative metasurfaces are shown in (c) and (d).
Since SAR sensors returns can be related to the spatial frequency domain projections of the scattering field, we exploit insights from compressed sensing theory to show that moving targets can be effectively imaged with a small number of transmitters and receivers randomly dispersed within a narrow forward cone around the scene of interest.
The scattering field of the target is denoted as L. And, the instantaneous rotational angle of target is defined as θ(t) = ωeff· t, and t is the slow time with 0 ≤ t ≤ T a, where T a is the CPI.
Once the scattering fields from dipole and slot antennas constituting metasurfaces are identified, we calculate transmission and reflection spectra.
After a discussion on Babinet principle to compare scattering fields from dipole and slot antennas constituting metasurface, a fabrication of metasurface and construction of MSLC cell are introduced.
From the scalar form of Maxwell's equations, the incident and scattering fields are analyzed first, and then the general SAR echo model [20] is derived according to the antenna theory.
The capacity of the multilayer system (C) can be found as the sum of three partial capacitances C = C1 + C2 + C3, where C1, C2, and C3 are the capacitances of the parts of the planar capacitor, which are scattering fields in (1) the substrate, (2) the inner parallelepiped of the film, and (3) the outer parallelepiped of the film.
Light scattering by each sample particle is computed for only one random orientation of the incident electromagnetic wave, but we average the scattered field over 100 scattering planes, evenly distributed around the propagation direction of the incident light.
