Editing Polarization (waves) (section)

==== Dichroism ====
Media in which transmission of one polarization mode is preferentially reduced are called ''[[dichroism|dichroic]]'' or ''diattenuating''. Like birefringence, diattenuation can be with respect to linear polarization modes (in a crystal) or circular polarization modes (usually in a liquid).

Devices that block nearly all of the radiation in one mode are known as ''{{dfn|polarizing filters}}'' or simply "[[polarizer]]s". This corresponds to {{math|1= ''g''{{sub|2}} = 0}} in the above representation of the Jones matrix. The output of an ideal polarizer is a specific polarization state (usually linear polarization) with an amplitude equal to the input wave's original amplitude in that polarization mode. Power in the other polarization mode is eliminated. Thus if unpolarized light is passed through an ideal polarizer (where {{math|1= ''g''{{sub|1}} = 1}} and {{math|1= ''g''{{sub|2}} = 0}}) exactly half of its initial power is retained. Practical polarizers, especially inexpensive sheet polarizers, have additional loss so that {{math|''g''{{sub|1}} < 1}}. However, in many instances the more relevant figure of merit is the polarizer's [[degree of polarization]] or [[extinction ratio]], which involve a comparison of {{math|''g''{{sub|1}}}} to {{math|''g''{{sub|2}}}}. Since Jones vectors refer to waves' amplitudes (rather than [[Irradiance|intensity]]), when illuminated by unpolarized light the remaining power in the unwanted polarization will be {{math|(''g''{{sub|2}}/''g''{{sub|1}}){{sup|2}}}} of the power in the intended polarization.