Optics And Photonics Codexery

Physical optics

Branch of optics studying wave phenomena beyond ray approximation.

Physical optics

Physical optics, often called wave optics, constitutes a fundamental branch of optics that examines phenomena where the ray-based simplifications of geometric optics break down. This field specifically addresses interference, diffraction, and polarization effects, which arise from the wave nature of light. Notably, this definition typically excludes topics such as quantum noise in optical communications, as those are handled within the separate sub-field of coherence theory. Beyond its role as a descriptive science, the term "physical optics" also denotes a specific approximation technique widely employed in optics, electrical engineering, and applied physics. This method serves as a practical intermediate step between the purely ray-based geometric optics and the more rigorous full-wave solutions of electromagnetism. The approximation works by first using ray optics to estimate the electromagnetic field on a given surface—such as a lens, mirror, or aperture—and then integrating that estimated field across the surface to calculate the resulting transmitted or scattered field. This approach is conceptually similar to the Born approximation, treating the detailed structure of the problem as a perturbation. In optical contexts, it is a standard technique for estimating diffraction effects, while in radio engineering it models certain optical-like phenomena. However, the approximation has limitations: it can model interference, diffraction, and polarization but does not capture the dependence of diffraction on polarization. Because it is a high-frequency approximation, it tends to be more accurate for optical wavelengths than for radio waves. In radar scattering applications, the method involves assuming that the current on the illuminated front of a scatterer is the same as that on a tangent plane of similar material, while setting the current on shadowed parts to zero. The scattered field is then approximated by integrating these currents. This technique works well for large, smooth, convex bodies and lossy surfaces, but it becomes inaccurate near edges or shadow boundaries unless supplemented by additional calculations for diffraction and creeping waves. The standard physical optics theory also has known defects in evaluating scattered fields, leading to reduced accuracy away from the specular direction, though an improved theory introduced in 2004 provides e

field
Physics, optics, electrical engineering, applied physics
known_for
Studying interference, diffraction, polarization; providing an approximation method between geometric optics and full wave electromagnetism
type
Branch of optics and approximation method
applications
Estimating diffraction effects in optics; modeling interference, diffraction, and polarization effects in radio; radar scattering analysis

Lore & Background

Physical optics is defined as the branch of optics that examines interference, diffraction, polarization, and other phenomena where the ray approximation of geometric optics is invalid. This definition excludes quantum noise in optical communication, which falls under coherence theory. The term also names an approximation used in optics, electrical engineering, and applied physics, positioned as an intermediate method between geometric optics and precise full wave electromagnetism. The word 'physical' indicates it is more physical than geometric or ray optics, not that it is an exact physical theory.

Reader's Guide

The physical optics approximation involves using ray optics to estimate the field on a surface, then integrating that field over the surface to calculate the transmitted or scattered field. This approach resembles the Born approximation, treating details as a perturbation. In optics, it is a standard way to estimate diffraction effects, typically by integrating ray-estimated field over a lens, mirror, or aperture. In radio, it models some interference, diffraction, and polarization effects but not the dependence of diffraction on polarization. As a high-frequency approximation, it is often more accurate in optics than for radio. In radar scattering, it involves taking the current found on a tangent plane of similar material at each point on the geometrically illuminated part of a scatterer, with current on shadowed parts set to zero, then integrating to obtain the approximate scattered field. This is useful for large smooth convex bodies and lossy surfaces. The ray-optics field or current is generally inaccurate near edges or shadow boundaries unless supplemented by diffraction and creeping wave calculations.

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