Rotate the laser and position a polarizer in the laser beam so as to create a beam that is linearly polarized in the horizontal direction. (To do this, utilize the reflection null at Brewster angle for horizontal polarization.) Mount a large aperture polarizer on a rotation stage to be used for analyzing the polarization, and cross this with the horizontally polarized laser beam.
Mount the quarter-wave plate on a rotation stage and position it
between the polarizers. Rotate the quarter-wave plate so that its
fast axis is vertical. Determine the polarization state after the
wave plate by using the second polarizer. To this end, measure the
degree of linear polarization using the optical power meter.
Rotate the quarter-wave plate so that its fast axis is making a
20 angle with the vertical. Repeat the same measurements. What
is the polarization state of the beam?
Rotate the quarter-wave plate so that its fast axis is making a
45 angle with the vertical. Repeat the same measurements. What
is the polarization state of the beam?
Obtain a circularly polarized beam. Remove the second polarizer. Position a flat mirror after the wave plate to reflect the beam back through the plate and the linear polarizer almost back into the laser. The reflection at the mirror flips the handedness of the the circularly polarized beam (LHC becomes RHC and vice versa, see problem 6.1-5). What should you see after the reflected beam passes back through the retarder and the linear polarizer? What do you observe?
Prepare a horizontally polarized beam with a polarizer and pass it through the half-wave plate. Use a polarizer after the half-wave plate to determine the polarization state. Rotate the half-wave plate and measure the rotation of the output polarization.