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{{Short description|Electromagnetic radiation special case}}
{{Use American English|date=March 2021}}
{{Use mdy dates|date=March 2021}}
{{More footnotes|date=May 2020}}
[[File:Linear polarization schematic.png|162px|thumb|right|Diagram of the electric field of a light wave (blue), linear-polarized along a plane (purple line), and consisting of two orthogonal, in-phase components (red and green waves)]]
In [[electrodynamics]], '''linear polarization''' or '''plane polarization''' of [[electromagnetic radiation]] is a confinement of the [[electric field]] vector or [[magnetic field]] vector to a given plane along the direction of propagation. The term ''linear polarization'' (French: ''polarisation rectiligne'') was coined by [[Augustin-Jean Fresnel]] in 1822.<ref name=fresnel-1822z>A. Fresnel, "Mémoire sur la double réfraction que les rayons lumineux éprouvent en traversant les aiguilles de cristal de roche suivant les directions parallèles à l'axe", read 9 December 1822; printed in H. de Senarmont, E. Verdet, and L. Fresnel (eds.), ''Oeuvres complètes d'Augustin Fresnel'', vol. 1 (1866), pp.{{nnbsp}}731–51; translated as "Memoir on the double refraction that light rays undergo in traversing the needles of quartz in the directions parallel to the axis", {{Zenodo|4745976}}, 2021 (open access); §9.</ref> See ''[[Polarization (waves)|polarization]]'' and ''[[plane of polarization]]'' for more information.
The orientation of a linearly polarized electromagnetic wave is defined by the direction of the [[electric field]] vector.<ref name="Shapira,">{{cite book
| last = Shapira
| first = Joseph
|author2=Shmuel Y. Miller
| title = CDMA radio with repeaters
| publisher = Springer
| date = 2007
| pages = 73
| url =
| isbn = 978-0-387-26329-
▲ | isbn = 0-387-26329-2}}</ref> For example, if the electric field vector is vertical (alternately up and down as the wave travels) the radiation is said to be vertically polarized.
==Mathematical description
The [[Classical physics|classical]] [[sinusoidal]] plane wave solution of the [[electromagnetic wave equation]] for the [[Electric field|electric]] and [[Magnetic field|magnetic]] fields is (cgs units)
:<math> \mathbf{E} ( \mathbf{r} , t ) =
:<math> \mathbf{B} ( \mathbf{r} , t ) = \hat { \mathbf{z} } \times \mathbf{E} ( \mathbf{r} , t )/c </math>
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**[[Circular polarization]]
**[[Elliptical polarization]]
**[[Plane of polarization]]
*[[Photon polarization]]
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==External links==
*[
*[
{{FS1037C}}
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[[ja:直線偏光]]
[[pl:Polaryzacja_fali#Polaryzacja_liniowa]]
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