Lummer–Gehrcke interferometer

From Wikipedia, the free encyclopedia
Jump to: navigation, search

The Lummer–Gehrcke interferometer or Lummer–Gehrcke plate is a multiple-beam interferometer similar to the Fabry–Perot etalon, but using light at a steep angle of incidence. The interferometer consists of a long plate of glass or quartz, with faces that are polished accurately flat and parallel.[1] Light bounces back and forth inside the plate, striking the faces at an angle just below the critical angle as it propagates along. Because of the steep angle of incidence, nearly all of the light is reflected, but a tiny fraction leaks out on each bounce. As in a Fabry–Perot interferometer, the light that leaks out has phase that depends on how many times it has bounced inside the plate. A lens is used to overlap light that has emerged after varying numbers of bounces, producing an interference pattern. A key difference from a Fabry–Perot etalon is that input light that reflects off of the surface of the plate does not contribute to the interference.[1]

Lummer–Gehrcke interferometers are now rarely used, having been largely replaced by Fabry–Perot interferometers using modern dielectric reflective coatings.[1]

See also[edit]

References[edit]

  1. ^ a b c Born, Max; Wolf, Emil (1999). "7.6.5 The Lummer–Gehrcke interferometer". Principles of Optics (7th ed.). Cambridge University Press. pp. 380–386. ISBN 0-521-64222-1.