Abstract: The configurations of an electro-optic Bragg deflector and the methods of using it as a laser Q-switch in a Q-switched laser and in a Q-switched wavelength-conversion laser are provided. As a first embodiment, the electro-optic Bragg deflector comprises an electrode-coated electro-optic material with one of a 1D and a 2D spatially modulated electro-optic coefficient. When a voltage is supplied to the electrodes, the electro-optic material behaves like a Bragg grating due to the electro-optically induced spatial modulation of the refractive index. The second embodiment relates to an actively Q-switched laser, wherein the electro-optic Bragg deflector functions as a laser Q-switch. The third embodiment of the present invention combines the Q-switched laser and a laser-wavelength converter to form a Q-switched wavelength-conversion laser, wherein the EO Bragg deflector can be monolithically integrated with a quasi-phase-matching wavelength converter in a fabrication process.

Abstract: A single-pass optical parametric amplifier is provided. The single-pass optical parametric amplifier comprises a light source emitting a fundamental wave having a wavelength range; a nonlinear material, which the fundamental wave passes therethrough to form a second harmonic generation wave having a light path; a supercontinuum generator extending the wavelength range of the fundamental wave to form a supercontinuum generation seed; and an optical parametric wavelength transformer transforming the supercontinuum generation seed and the second harmonic generation wave into a signal wave and an idler wave.

Abstract: The configurations of an electro-optic Bragg deflector and the methods of using it as a laser Q-switch in a Q-switched laser and in a Q-switched wavelength-conversion laser are provided. As a first embodiment of the present invention, the electro-optic Bragg deflector comprises an electrode-coated electro-optic material with a spatially modulated electro-optic coefficient. When a voltage is supplied to the electrodes, the electro-optic material behaves like a Bragg grating due to the electro-optically induced spatial modulation of the refractive index. The second embodiment of the present invention relates to an actively Q-switched laser, wherein the electro-optic Bragg deflector functions as a laser Q-switch. The third embodiment of the present invention combines the Q-switched laser and a laser-wavelength converter to form a Q-switched wavelength-conversion laser, wherein the EO Bragg deflector can be monolithically integrated with a quasi-phase-matching wavelength converter in a fabrication process.

Abstract: A simple and effective coherent radiation device generates laser-like radiation from an optical parametric oscillator (OPO) that is formed by a dielectric-modulation structure in a nonlinear optical material. The nonlinear optical material used in the OPO can be a birefringence phase-matched material or a quasi-phase-matched material.

Abstract: A laser system providing a laser source suitable for medical PDT (Photodynamic Therapy) and PDD (Photodynamic Diagnosis) is purposed. The laser system includes a pump laser emitting at least one wavelength to pump a wavelength converter inside a laser resonating system; a wavelength converter using QPM (Quasi-Phase-Matching) technique to convert the wavelength emitted by the pump laser to at least one wavelength suitable for the PDT and the PDD; a laser resonating system for enhancing the output intensity of the laser suitable for the PDT and the PDD generated from the wavelength converter pumped by the pump laser; and an optical transmission and output device for receiving and transmitting the output laser from the laser resonator system to its end optical output component, through which at least one specific target is illuminated.

Abstract: The invention relates to a simple and effective laser device for generating laser radiation from an optical parametric oscillator (OPO) by implementing a distributed feedback (DFB) or distributed Bragg reflector (DBR) structure, in the laser oscillator. The nonlinear crystal used in the OPO of the present invention can be a birefringence phase-matched crystal or a quasi-phase-matched crystal.