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🗒ïļ Note: the polarization direction is the same as the direction of the electric field

Light can be converted from random to linear using a linear polarizer, for example a dichroic sheet

Generally a polaroid sheet which consists of PVA doped with iodine

Generally a polaroid sheet which consists of PVA doped with iodine

Circular polarized light

<aside> <img src="https://prod-files-secure.s3.us-west-2.amazonaws.com/369dfa6b-d4d9-4cf2-a446-e369553b6347/cca6ec0c-18e8-4ce8-bc05-8a3ddbacb05e/Circular_polarized_light.gif" alt="https://prod-files-secure.s3.us-west-2.amazonaws.com/369dfa6b-d4d9-4cf2-a446-e369553b6347/cca6ec0c-18e8-4ce8-bc05-8a3ddbacb05e/Circular_polarized_light.gif" width="40px" /> Circular polarized light: the electric vector rotates at a constant rate, $\omega$, the same as the oscillation frequency, and at constant amplitude

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Both linear and circular are cases of the general form that is elliptical

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We see that $\vec E$ rotates at constant rate $\omega$, with a major axis that is tilted at an angle $\Psi$. Unit vector $\xi$ is plane vector, and $\eta$ is the ellipticity

💃 Examples:

🗒ïļ Note: The electric vector can rotate in either direction LHC and RHC

ðŸĶī Convention: When viewed along the propagation direction, if the electric vector rates anticlockwise this is the LHC and vice versa

Light in a medium

$$ \vec E=\left [\left |\vec E\right | \sin(\theta)\,\hat i+\left |\vec E\right |\cos(\theta)\,\hat j \right ]\exp[i(\omega t-kz+\phi)] $$

Absorbers

Circular polarized light through a linear polarizer gives linearly polarized light at half intensity no matter the orientation

Types of linear absorbing polarizers