z-logo
open-access-imgOpen Access
Double-Glazing Interferometry
Author(s) -
Vincent Toal,
Emilia Mihaylova
Publication year - 2009
Publication title -
the physics teacher
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.411
H-Index - 38
eISSN - 1943-4928
pISSN - 0031-921X
DOI - 10.1119/1.3116841
Subject(s) - optics , interferometry , michelson interferometer , white light interferometry , physics , monochromatic color , optical path length , interference (communication) , white light , coherence (philosophical gambling strategy) , interferometric visibility , light source , astronomical interferometer , channel (broadcasting) , electrical engineering , quantum mechanics , engineering
This note describes how white light interference fringes can be seen by observing the Moon through a double-glazed window. White light interferometric fringes are normally observed only in a well-aligned interferometer whose optical path difference is less than the coherence length of the light source, which is approximately one micrometer for white light. Obtaining such fringes in a Michelson interferometer is not a trivial task.1 The interferometer is typically illuminated with a monochromatic source and the path length difference adjusted with a wedge angle between the interferometer mirrors so that five or six vertical fringes are visible, indicating nearly equal paths. Then the mirrors are adjusted until the fringes are almost perfectly straight. Finally we use a white light source and carefully scan through the approximately equal path range until five or six white light fringes are seen to sweep rapidly by.

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom