A transverse static electric field can induce linear birefringence through the electro-optic Kerr effect. Define its coefficient by , with the principal axes parallel and perpendicular to the applied field. A length then gives .
For input polarized at to those axes, switching from zero retardation to switches linear to circular polarization. Other input angles generally become elliptical, and axis-aligned input stays linear. The required field magnitude for the lowest-order setting isA Kerr cell is suitable as a switchable quarter-wave plate. The field can be changed electronically without mechanically rotating the axes; actual switching time depends on the material response and driving circuit. This is induced linear birefringence, not polarization-selective absorption.[ref]
The Feynman Lectures on Physics, Volume I by Richard Feynman and others. §33–3, final paragraphs: an applied electric field produces birefringence and electrical light switching in a Kerr cell
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