HOW A CIRCULAR POLARIZER FUNCTIONS

Unpolarized ambient light entering the display from the outside first passes through a linear polarizer (the first layer of the circular polarizer). When the light ray, now linearly polarized, passes through the ¼ wave retarder, it is separated into two equal component light rays that are ¼ wavelength out of phase with one another (i.e., the phase relationship such that the leading ray is ¼ wavelength ahead of the lagging ray). When these light rays strike a specularly reflecting surface (e.g., the front of a display or internal layer of a resistive touch panel) and are reflected, the phase relationships between the two rays are reversed. Now the previously lagging ray is ¼ wavelength in front. It then re-enters the retarder. The retarder realigns the two rays, and the resultant ray is oriented 90 degrees from the original ray. Thus, by next passing through the linear polarizer again, this ray is blocked. In this way, unwanted reflected ambient light originating outside the display is separated from the desired light emitted by the display, thereby reducing glare and internal reflections, and increasing contrast. The level of blocking is characterized by the polarizer efficiency of the linear polarizer or the extinction coefficient of the circular polarizer.

A “perfect” linear polarizer would transmit 50% of an unpolarized input beam. Two perfect polarizers with their transmission axes crossed will totally extinguish an incident beam and have a polarizing efficiency of 100%. Note the vibration direction of a transmitted wave through a LP is always 90 degrees with respect to the LP transmission axis. Dontech standard linear polarizers have a total luminous transmittance between 40 to 46% of unpolarized light.

The retarder has two principal axes, slow and fast, and it resolves a light beam into two polarized components. The beam parallel to the slow axis lags the one parallel to the fast axis. The “retardance” of a material depends on its birefringence. Birefringence is an intensive quantity and is specifically the difference between the two principal refractive indices or the speeds of the propagation of light within the substrate depending on vibration direction. Note: refractive index (n) is the ratio of the speed of light in a vacuum to the normal speed in a medium. The extreme Δn in a material due to the change in vibration direction is the measure of its birefringence. The birefringence of a material remains constant no matter what the size or orientation of the material. Retardance is similar but it is an extensive quantity. For example, if you double a retarder’s thickness the retardance is doubled. Note, a retarder has no effect on an unpolarized beam of light. 

Circular polarizers are expressed as having handedness or helicity, which is determined by the position of the slow axis of the retarder being to the right or left of the linear polarizer as viewed from the retarder side of the filter. Dontech standard circular polarizers are left-handed. However, Dontech can configure a CP to either handedness.