Glan–Foucault prism: Difference between revisions

Content deleted Content added
m CS1 maint: Explicit use of et al. -> display-authors/editors=etal using AWB
refs
Line 1:
[[Image:Glan-foucault.png|frame|right|A Glan–Foucault prism deflects ''p''-polarized light, transmitting the ''s''-polarized component. The optical axis of the prism material is perpendicular to the plane of the diagram.]]
 
A '''Glan–Foucault prism''' (also called a '''Glan–air prism''') is a type of [[prism (optics)|prism]] which is used as a [[polarizer]]. It is similar in construction to a [[Glan–Thompson prism]], except that two right-angled [[calcite]] prisms are spaced with an air-gap instead of being cemented together.<ref>{{cite book |last=Bennett |first=Jean M . |editor=Bass, Michael, Ed. |title=Handbook of Optics Volume II |edition=2nd |date=1995 |publisher=McGraw-Hill |isbn=0-07-047974-7 |pages=3.11–3.12 |chapter=Polarizers }}</ref> [[Total internal reflection]] of ''p''-[[polarization (waves)|polarized]] light at the air gap means that only ''s''-polarized light is transmitted straight through the prism.
 
Compared to the Glan–Thompson prism, the Glan–Foucault has a narrower acceptance angle over which it will work, but because it uses an air-gap rather than cement, much higher [[irradiance]]s can be used without damage. The prism can thus be used with [[laser]] beams. The prism is also shorter (for a given usable aperture) than the Glan–Thompson design, and the deflection angle of the rejected beam can be made close to 90°, which is sometimes useful. Glan–Foucault prisms are not typically used as polarizing beamsplitters because while the transmitted beam is 100% polarized, the reflected beam is not.