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Total external reflection

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This is an old revision of this page, as edited by Interferometrist (talk | contribs) at 16:58, 17 April 2018 (Page proposed for deletion. Phenomenon as described doesn't exist in practice (would require zero or infinite refractive index). Term never used in practice, even for X-ray reflectors (where it is true as an approximation).). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

Total external reflection is an optical phenomenon where electromagnetic radiation (e.g. visible light) can, at certain angles, be totally reflected from an interface between two media of different indices of refraction (see Snell's law). Total internal reflection occurs when the first medium has a larger refractive index than the second medium, for example, light that emerges from under water. The optically denser material (water in this case) is the "internal" medium. For visible light, water has an index of refraction of 1.33 and for air it is very close to 1. For vacuum the index of refraction is exactly 1 for all wavelengths.

For X-rays, however, all materials have indices of refraction slightly below 1. This entails that total reflection of X-rays only can occur when they travel through vacuum and impinge on a surface (at a small glancing angle). Since this kind of total reflection takes place outside of the material it is termed total external reflection.[1] This makes it possible to focus X-rays (see, for example, NASA https://imagine.gsfc.nasa.gov/science/toolbox/xray_telescopes1.html).

References

  1. ^ Attwood, D (1999). Soft X-Rays and Extreme Ultraviolet Radiation. Cambridge University Press.