P5.4.5.1 Pockels Effect in a Conoscopic Beam Path

The experiment P5.4.5.1 demonstrates the Pockels effect in a lithium niobate crystal placed in a conoscopic beam path. The crystal is illuminated with a divergent, linearly polarized light beam, and the transmitted light is viewed behind a perpendicular analyzer. The optical axis of the crystal, which is birefringent even when no electric field is applied, is parallel to the incident and exit surfaces; as a result, the interference pattern consists of two sets of hyperbolas which are rotated 90° with respect to each other. The bright lines of the interference pattern are due to light rays for which the difference Δ between the optical paths of the extraordinary and ordinary rays is an integral multiple of the wavelength λ. The Pockels effect alters the difference of the main refractive indices, n_o - n_e, and consequently the position of the interference lines. When the so-called half-wave voltage U_λ is applied, Δ changes by one half wavelength. The dark interference lines move to the position of the bright lines, and vice versa. The process is repeated each time the voltage is increased by U_λ.

COMPONENTS OF EQUIPMENT SETS:

1	472 90	Pockels cell
1	521 70	High-voltage power supply, 10 kV
1	471 830	He-Ne Laser, linearly polarised
1	460 01	Lens in frame, f=5 mm
1	460 02	Lens in frame, f=50 mm
1	472 401	Polarisation filter
1	460 32	Optical bench with standardised profile, 1 m
5	460 370	Optics rider, 60/34
1	441 53	Screen, translucent
1	300 11	Saddle base
1	500 604	Safety connecting lead, 10 cm, black
1	500 641	Safety connecting lead, 100 cm, red
1	500 642	Safety connecting lead, 100 cm, blue

EXPERIMENT INSTRUCTIONS CLICK HERE