RP Photonics logo
RP Photonics
Technical consulting services on lasers, nonlinear optics, fiber optics etc.
Profit from the knowledge and experience of a top expert!
Powerful simulation and design software.
Make computer models in order to get a comprehensive understanding of your devices!
Success comes from understanding – be it in science or in industrial development.
The famous Encyclopedia of Laser Physics and Technology – available online for free!
The ideal place for finding suppliers for many photonics products.
Advertisers: Make sure to have your products displayed here!
… combined with a great Buyer's Guide!
VLib part of the


<<<  |  >>>

Definition: optical filters where the light transmission depends strongly on the direction of polarization

German: Polarisatoren

Category: general optics

How to cite the article; suggest additional literature

A polarizer is a kind of optical filter where the light transmission depends strongly on the polarization state. Normally, light with linear polarization in a certain direction is passed, and light polarized in an orthogonal direction is blocked: it may be absorbed or sent to a different direction.

One can also construct devices passing light with a certain circular polarization, usually using one or more quarter waveplates in conjunction with a linear polarizer.

Note that a polarizer can not convert any polarization of input light into the wanted polarization; this is physically not possible. It can only remove light with the unwanted polarization.

Ideal versus Real Polarizers

An ideal polarizer would have the following properties:

In practice, polarizers are not ideal. In particular, they absorb or reflect some part of the optical power, and the absorbed part may lead to thermal effects such as beam distortions. The performance depends very much on the used type of polarizer (see below).

When using a polarizer, the actual goal is not always exactly the same:

Types of Optical Polarizers

Absorptive Polarizers (= Dichroic Polarizers)

For low-power applications, Polaroid filters (polarizing sheets, sheet polarizers) are often used. These consist of a special doped plastic sheet (a polymer materials), which has been stretched in one direction, such that the polymer chains are more or less aligned along one axis. Light a polarization direction along the chains is strongly absorbed, whereas the absorption is weak for light with a polarization direction perpendicular to these. The polymer sheet is usually mounted in some solid holder, which may have marks indicating the direction of polarization for maximum transmission.

Similar sheets are used for polarizing glasses (also called polarized glasses). In case of sunglasses, only vertically polarized light is transmitted. This reduces glare from water surfaces, for example, as horizontally polarized light experiences stronger reflection at such surfaces. In case of polarizing glasses for 3D viewing, one eye gets the vertical polarization and the other eye the horizontal one. In this way, a 3D display can transmit separate images for the eyes.

Polymer sheet polarizers can be made quite large, and usually they are quite cheap.

A more modern type of absorptive polarizer is based on silver or copper nanoparticles embedded in a thin glass plate. These glass polarizers are much more expensive and not available in very large sizes, but offer a substantial better performance in terms of polarization extinction ratio. Laminated versions are mechanically more robust and cause lower wavefront distortions.

Absorptive filters can handle only quite limited optical powers (have a low optical damage threshold), because the absorbed power is converted to heat, and the sheet can easily be damaged by overheating it. In case of simple polymer sheet polarizers, an optical intensity of only 1 W/cm2 may already be critical.

Polarizing Beam Splitters Based on Birefringence

Much higher optical powers can be handled by polarizers where light with the “rejected” polarization state is not absorbed but only sent to some other direction. (If it needs to absorbed later on, a beam dump can stand much higher powers than an optical element.) The most common type of polarizing beam splitters exploit birefringence of a transparent crystalline material such as quartz (SiO2), calcite (CaCO3), yttrium vanadate (YVO4), beta barium borate (BBO) or magnesium fluoride (MgF2). Often, two pieces of such material with different orientations of the optical axis are cemented together (or joined with a small air space). The device is often mounted in a polymer housing, which may also contain a beam dump for light with the rejected polarization direction.

Different physical principles of birefringent polarizers are used:

Glan–Taylor prism

Figure 1: A Glan–Taylor prism. total internal reflection occurs for the s polarization, whereas there is little reflection for p polarization due to operation close to Brewster's angle.

  • In some types of polarizers, such as the Nicol prism, the Glan–Thompson prism, the Glan–Taylor prism and the Glan–Foucault prism, total internal reflection occurs for one polarization state, but not for the other, so that one obtains completely different beam directions for these outputs.
  • Other types of polarizers, such as the Wollaston prism, the Nomarski prism, the Rochon prism and the Sénarmont prism, only exploit somewhat different refraction angles due to birefringence, and not any reflection. Here, the two output beams are less strongly separated.

Such birefringent crystalline polarizers differ in various respects:

  • For true polarizing beam splitters such as the Wollaston prism, both output beams are completely polarized. This is not the case for some other designs, such as the Glan-Thompson prism, the Glan-Foucault prism and the Glan-Taylor prism (even though these can be more or less optimized in that respect). Note that for many applications only one output is used, so that this aspect is not always relevant.
  • For some designs (e.g., the Glan–Taylor prism, the Glan–Foucault prism, the Rochon prism and the Sénarmont prism), one of the involved rays is not deflected, i.e., continuous to propagate after the polarizers in the same direction as the incident beam.
  • Some designs work properly only for a narrow range of incidence angles, whereas others have a wider angular acceptance range. For example, the Glan–laser prism is a variant of the Glan–Taylor prism which works only in a narrow range of angles (which is usually no problem when working with low-divergence laser beams), but has lower optical losses and a higher optical damage threshold.
  • Those designs using a cement rather than an air gap tend to have lower optical damage threshold.
  • Many polarizers have anti-reflection coatings, which function well only in a limited wavelength range.
  • Some crystal materials such as BBO allow for operation at particularly short wavelengths in the ultraviolet spectral region, whereas others are well suited for infrared light.

The reason for the use of many different designs of birefringent polarizer designs is that different applications can have quite different requirements on the polarizers, and no design can meet all requirements.

Thin-Film Polarizers

polarizing plate

Figure 2: A thin-film plate polarizer.

There are different kinds of thin-film polarizers. Thin-film plate polarizers (Figure 2) consist of a dielectric coating on some glass substrate. (Note that the substrate does not need to be birefringent.) For non-normal incidence (in a certain range of incidence angles), the reflectivity of the coating can be strongly polarization-dependent. It is possible to have the “rejected” beam at a deflection angle of 90°, which is often convenient. However, many thin-film plate polarizers are operated at Brewster's angle, so that no anti-reflection coating is required on one side.

There are polarizing cube beam splitters where the dielectric coating is applied to one 45° prism and another 45° prism is cemented to the coating, such that overall one obtains a cube.

Note that they can work only in a limited wavelength range, since the interference effects in the multilayer coating are of course wavelength-dependent. However, operation in a range of few hundred nanometers is possible.

An advantage of thin-film polarizers is that they can be made with rather large dimensions, which is more difficult with crystalline (birefringent) polarizers.

The article on thin-film polarizers gives more details.

Wire Grid Polarizers

Wire grid polarizers are made by fabricating very narrow (sub-wavelength) metal stripes on a glass substrate (using a lithographic technique) or in a free-standing arrangement (for longer wavelengths). Such devices reflect s-polarized light, while p-polarized light is transmitted. They can be used at very high average power levels.

Essential Specifications for Polarizers

The performance of a polarizer is characterized by various specifications:

Note that a high performance of a polarizer is more difficult to achieve in extreme wavelength regions, in particular in the ultraviolet spectral region.

Selection of a polarizer for an application can be a relatively complex task, as many different aspects have to be taken into account. The different requirements for different applications are also the reason why so many polarizer designs are in use.

Applications of Optical Polarizers

Polarizers have many different applications. Some examples:

See also: thin-film polarizers, beam splitters, polarization beam combining, prisms
and other articles in the category general optics

In the RP Photonics Buyer's Guide, 99 suppliers for polarizers are listed.

If you like this article, share it with your friends and colleagues, e.g. via social media: