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Plane Waves in Materials with Optical Rotation

2 Plane Waves in Materials with Optical Rotation [Pg.8]

In this case the material is characterized by e - = e8, py = jj.8-, - = tM jiyS. and Q, j = 0. The parameter y is the rotary power. This material couples the electric and magnetic fields, and the Maxwell curl equations are [Pg.8]

The time dependence of the electric field is still e mt, so that its spatial dependence is described by [Pg.8]

For light propagating along the z axis, this leads to the following equations for the components of the electric vector  [Pg.8]




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In-plane

Optical material

Optical rotation

Plane waves

Rotating waves

Rotations in

Wave optics

Waves in

With rotation

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