Radiation Boundaries
When solving radiating and scattering structures in an unbounded, infinite domain, HFSS truncates the problem into a bounded domain and prescribes the appropriate truncation condition. This is generally known as the "radiation boundary condition". Theoretically, the radiation boundary condition should be a "transparent" condition. In other words it should not produce any unphysical reflection as a result of the artificial truncation. HFSS offers three types of radiation boundaries: first-order absorbing boundary condition (ABC), perfectly matched layers (PML), and boundary integral equations (IE).
ABC and PML Boundaries
Both the ABC and PML boundaries attempt to minimize reflections by absorbing all outgoing waves at the truncation boundary. Because of this, they can only be prescribed at convex surfaces. This is because for concave surfaces, outgoing waves will re-enter the problem domain and should therefore not be completely eliminated. While PMLs absorb any kind of waves including guided waves, ABC imitates radiation to homogeneous background space.
ABCs only absorbs normal or near normal incident waves. Thus in order to produce accurate results, it must be placed sufficiently far away from structures. The typical recommendation is at least a quarter wavelength from the radiating source, although in some cases the radiation boundary may be located closer than one-quarter wavelength, such as portions of the radiation boundary where little radiated energy is expected. ABC is a local condition and thus preserving the sparse nature of the FEM formulation.
PMLs absorb all outgoing waves by adding artificial material layers that are designed such that all of the incident waves impinging upon them are completely transmitted with minimal reflections. Thus PMLs can be placed closer than ABCs. Furthermore, the PML absorbs a much wider range of waves in terms of frequency and direction whereas ABC absorbs only normally incident waves accurately. However, PMLs in general makes it more difficult for the iterative solver to reach convergence compared to ABCs. PMLs also preserves the sparse nature of the FEM formulation.
Radiating BCs and PMLs are local boundary conditions and inherit the Global Environment Material from the computational domain. They work as if the material of the computational domain were continued to infinity. FE-BI uses the user defined Global Environment material which may or may not be the same as the material of the computational domain. If they are the same, PMLs and FE-BI give the same results. If the materials are different, there is a jump in the materials which can be modeled by FE-BI, but not by PMLs.