“…In many cases, it is not practical to fully calculate such an interaction. In classical electromagnetism, several approximations have been established and are now widely used [32], e.g., the physical optics approximation [33] and the discrete dipole approximation [34,35]. In particular, the perfect conductor approximation [36] for a mirror surface is essential because it enables us to perform an analytic calculation and decrease the amount of numerical calculation.…”