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[[Image:Faraday-effect.svg|thumb|right|250px|Polarization mechanism due to the Faraday effect. The field lines are usually closed through a [[permanent magnet]] around the rotator.]] | |||
A '''Faraday rotator''' is an optical device that rotates the [[polarization of light]] due to the [[Faraday effect]], which in turn is based on a [[magneto-optic effect]]. | |||
The Faraday rotator works because one polarization of the input light is in [[ferromagnetic]] [[resonance]] with the material which causes its [[phase velocity]] to be higher than the other. | |||
The plane of linearly polarized light is rotated when a [[magnetic field]] is applied [[Parallel (geometry)|parallel]] to the [[wave propagation|propagation]] direction. The empirical [[angle of rotation]] is given by: | |||
:<math> \beta = VBd \!</math> | |||
Where <math>\beta</math> is the angle of rotation (in [[radian]]s).<br /> | |||
<math>B</math> is the magnetic flux density in the direction of propagation (in [[tesla (unit)|tesla]]s).<br> | |||
<math>d</math> is the length of the path (in metres) where the light and magnetic field interact.<br> | |||
Then <math>V</math> is the [[Verdet constant]] for the material. This empirical proportionality constant (in units of radians per tesla per metre, rad/(T·m)) varies with wavelength and temperature and is tabulated for various materials. | |||
Faraday rotation is an example of non-reciprocal optical propagation. Unlike what happens in an [[optical activity|optically active]] medium such as a sugar solution, reflecting a polarized beam back through the same Faraday medium does not undo the polarization change the beam underwent in its forward pass through the medium. This allows Faraday rotators to be used to construct devices such as [[optical isolator]]s to prevent undesired back propagation of light from disrupting or damaging an optical system. | |||
The geometry of nonreciprocal propagation may at first appear paradoxical. In an optically active medium, the polarization direction twists in the same sense (e.g. like a right-handed screw) during the forward and backward passes, whereas in a Faraday medium, because the light reverses its propagation direction with respect to the magnetic field, the helicity of the propagation also reverses. But because the propagation axis has also reversed, this reversal of helicity is just what is needed to cause the back-reflected light to have different polarization from the incident light. If the Faraday medium is of such thickness as to cause a 45 degree rotation on the way in, the back-reflected beam will have polarization perpendicular to the incident beam, allowing it to be cleanly blocked by the light source's polarizer. | |||
Faraday rotators may be enhanced by the [[Zeeman effect]].<ref>{{cite journal| last=Popescu| first=Alexandru| coauthors=Walther, Thomas| title=On the potential of Faraday anomalous dispersion optical filter as high-resolution edge filters| journal=Laser physics| year=2005| volume=15| issue=1| pages=55–60| url=http://www.physik.tu-darmstadt.de/lqo/cgi-bin/Download/Downloadmgr.cgi?user=anonymous&file=lasphys_popescu_fadof.ps&type=ps| accessdate=2007-03-13}}</ref> | |||
==See also== | |||
*[[Optical isolator]] | |||
*[[Atomic line filter]] | |||
==References== | |||
<references/> | |||
{{DEFAULTSORT:Faraday Rotator}} | |||
[[Category:Optical devices]] | |||
[[Category:Michael Faraday]] | |||
Revision as of 07:10, 26 January 2014
A Faraday rotator is an optical device that rotates the polarization of light due to the Faraday effect, which in turn is based on a magneto-optic effect.
The Faraday rotator works because one polarization of the input light is in ferromagnetic resonance with the material which causes its phase velocity to be higher than the other.
The plane of linearly polarized light is rotated when a magnetic field is applied parallel to the propagation direction. The empirical angle of rotation is given by:
Where is the angle of rotation (in radians).
is the magnetic flux density in the direction of propagation (in teslas).
is the length of the path (in metres) where the light and magnetic field interact.
Then is the Verdet constant for the material. This empirical proportionality constant (in units of radians per tesla per metre, rad/(T·m)) varies with wavelength and temperature and is tabulated for various materials.
Faraday rotation is an example of non-reciprocal optical propagation. Unlike what happens in an optically active medium such as a sugar solution, reflecting a polarized beam back through the same Faraday medium does not undo the polarization change the beam underwent in its forward pass through the medium. This allows Faraday rotators to be used to construct devices such as optical isolators to prevent undesired back propagation of light from disrupting or damaging an optical system.
The geometry of nonreciprocal propagation may at first appear paradoxical. In an optically active medium, the polarization direction twists in the same sense (e.g. like a right-handed screw) during the forward and backward passes, whereas in a Faraday medium, because the light reverses its propagation direction with respect to the magnetic field, the helicity of the propagation also reverses. But because the propagation axis has also reversed, this reversal of helicity is just what is needed to cause the back-reflected light to have different polarization from the incident light. If the Faraday medium is of such thickness as to cause a 45 degree rotation on the way in, the back-reflected beam will have polarization perpendicular to the incident beam, allowing it to be cleanly blocked by the light source's polarizer.
Faraday rotators may be enhanced by the Zeeman effect.[1]
See also
References
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