Acousto- and electro-optics

Acousto-optical modulators

Acousto-optic modulators (AOM or Bragg cells) consist of a crystal that is transparent to laser light, a piezoelectric transducer and a sound absorber that prevents standing waves from forming in the crystal. When an electric field is applied to the piezoelectric transducer, sound waves are generated in the crystal which modulate the refractive index. This allows the power, direction and frequency of the laser beam to be controlled. AOMs are used for the following applications, among others: Q-switching of solid-state lasers Generation of ns pulses and ultrashort pulses Active mode locking As external modulators, e.g. for laser communication systems Pulse picker for increasing the pulse energy while reducing the pulse repetition rate Continuous power modulation or switches Noise suppression For AOMs, we offer crystals made of TeO2, crystalline quartz and fused silica.

Electro-optical modulators

An electro-optic modulator (EOM) consists of a Pockels cell and other optical components such as polarizers. A Pockels cell is a non-linear crystal and can change the refractive index when an electric field is applied. This allows the power, phase and polarization of the laser beam to be controlled. EOMs are used for the following applications, among others: Power modulator (e.g. for laser printing and optical communication) Laser frequency stabilization Q-switching of solid-state lasers Active mode locking Fast optical switch We offer KDP, KTP, BBO, LiNbO3 and LiTaO3 crystals for EOMs.