High resolution optical waveform shaping device having phase shift compensation associated with optical intensity modulation

An optical waveform shaping device comprising:

• a polarization separator for polarizing/separating the light beam from a light source;
• a ½ wavelength plate for joining the polarization planes of a first lightwave and a second lightwave polarized/separated by the polarization separator;
• a polarization beam splitter where the light beams having passed through the ½ wavelength plate are incident;
• a Faraday rotator for rotating in a predetermined amount the polarization planes of the first lightwave and the second lightwave having passed through the polarization beam splitter;
• a first collimator where the lightwave having passed through the Faraday rotator is incident;
• a second collimator where the lightwave having passed through the Faraday rotator is incident;
• a 2-axis polarization-preserving fiber where the lightwaves from the first collimator and the second collimator are incident;
• a third collimator where the light beams having passed through the 2-axis polarization-preserving fiber;
• a branching filter for branching the light beam from the third collimator into the light beams of each frequency;
• a condensing lens for condensing the plurality of light beams branched by the branching filter;
• a polarization separation means for adjusting the polarization planes of the light beams having passed through the condensing lens;
• a spatial light modulator having a phase modulation part and an intensity modulation part where the light beams having passed through the polarization separation means are incident, the phase modulation part and the intensity modulation part each having a plurality of liquid crystal cells in a line or in a matrix existing in the corresponding spatial positions, the orientation of liquid crystals of the phase modulation part being parallel to the polarization plane adjusted by the polarization separation means, the orientation of liquid crystal of the intensity modulation part being 45 degrees offset from the orientation of liquid crystals of the phase modulation part;
• a prism-type folded reflector where the light beams having passed through the liquid crystal spatial phase modulation and liquid crystal spatial intensity modulation part are incident;
• a ½ wavelength plate for adjusting the polarization planes of the lightwaves output from the polarization beam splitter after having passed through the folded reflector;
• and
• a forth collimator where the light beams having passed through the ½ wavelength plate are incident,
• wherein the light beam from the third collimator is frequency separated and is dispersed spatially by the branching filter,
• wherein the spatially dispersed and frequency separated light beams are condensed by the condensing lens,
• wherein the polarization planes of the condensed light beams are adjusted by the polarization separation means,
• wherein the light beams with the polarization planes adjusted are subjected to either or both of separately controlled phase modulation and intensity modulation by the spatial light modulator,
• wherein the light beams are folded by the folded reflector,
• wherein the light beams are condensed through the condensing lens,
• wherein the frequency separated light beams are multiplexed by the branching filter,
• wherein the lightwave derived from the first lightwave is incident on the Faraday rotator through the second collimator,
• wherein the lightwave derived from the second lightwave is incident on the Faraday rotator through the first collimator,
• wherein the traveling direction of the lightwave derived from the first lightwave and the lightwave derived from the second lightwave having passed through the Faraday rotator are adjusted by the polarization beam splitter,
• wherein the polarization planes of the two lightwaves with the traveling direction adjusted are adjusted by the ½ wavelength plate so that the polarization planes are orthogonal to each other,
• and wherein the lightwaves with the polarization planes adjusted are output through the forth collimator.