Optical path length

In optics, optical path length (OPL) is the product of the geometric length of the path light follows through the system, and the index of refraction of the medium through which it propagates. A difference in optical path length between two paths is often called the optical path difference (OPD). Optical path length is important because it determines the phase of the light and governs interference and diffraction of light as it propagates.

Details

In a medium of constant refractive index, n, the OPL for a path of physical length d is just

$\mathrm{OPL} = nd .\,$

If the refractive index varies along the path, the OPL is given by

$\mathrm{OPL} = \int_C n(s) \mathrm d s,\quad$

where n(s) is the local refractive index as a function of distance, s, along the path C.

An electromagnetic wave that travels a path of given optical path length arrives with the same phase shift as if it had traveled a path of that physical length in a vacuum. Thus, if a wave is traveling through several different media, then the optical path length of each medium can be added to find the total optical path length. The optical path difference between the paths taken by two identical waves can then be used to find the phase change. Finally, using the phase change, the interference between the two waves can be calculated.

Fermat's principle states that the path light takes between two points is the path that has the minimum optical path length.

References

This article incorporates public domain material from the General Services Administration document "Federal Standard 1037C" (in support of MIL-STD-188).
Jenkins, F.; White, H. (1976). Fundamentals of Optics (4th Edition ed.). McGraw-Hill. ISBN 0-07-032330-5.

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