A device for moving a nonlinear crystal or a saturable absorber in two dimensions includes a first and a second piezo unit, each having a corresponding carrier, piezo driver, and carriage moveable by the piezo driver at incremental steps along a linear path with respect to the carrier between a first and a second end location, in which the linear paths of the first piezo unit and the second piezo unit are orthogonal. The nonlinear crystal/saturable absorber is fastenable on the carriage of the first piezo unit and the carrier of the first piezo unit is fastened on the carriage of the second piezo unit. The device further includes stops that define the carriage end locations, an end location detection configured to detect the carriages at their respective end locations, and a counting unit configured to count the steps covered during the moving of the carriage.

An optical clock generator includes a nonlinear cavity unit, a cross-waveguide logic gate unit and a delayer unit; and is of a six-port photonic crystal structure including two reference-light signal-input ports, a feedback-signal-input port, a system-signal and feedback-signal output port and two idle ports; the output port of the cross-waveguide logic gate unit is connected with the input port of the nonlinear cavity unit whose system-signal output port is connected with the input port of said delayer unit whose output port is connected with the input port of the cross-waveguide logic gate unit, the system-signal output port is connected with a two-branch waveguide one of which is used as the system-signal output port, and another is used as the feedback-signal output port and connected to an input port of said delayer unit, the delayer unit performs time delay on an input signal and outputs the signal to the feedback-signal-input port.

A pulsed third-harmonic laser system includes a pulsed laser, an extra-cavity nonlinear crystal, and an intracavity nonlinear crystal. The pulsed laser generates fundamental laser pulses and couples out a portion of each fundamental laser pulse out of the laser resonator to undergo second-harmonic-generation in the extra-cavity nonlinear crystal. Resulting second-harmonic laser pulses are directed back into the laser resonator and mixes with the fundamental laser pulses in the intracavity nonlinear crystal to generate third-harmonic laser pulses. The pulsed third-harmonic laser system thus maintains a non-zero output coupling efficiency regardless of the efficiency of the second-harmonic-generation stage, while the third-harmonic-generation stage benefits from the intracavity power of the fundamental laser pulses.

A microwave to optical conversion device comprising: a superconducting microwave resonator, and an optical resonator including an electro-optical material, the superconducting microwave resonator and the optical resonator being arranged one with respect to the other so as to be electro-magnetically coupled.

A dual frequency optical resonator configured for optical coupling to light having a first frequency ω1. The dual frequency optical resonator includes a plurality of alternating layer pairs stacked in a post configuration, each layer pair having a first layer formed of a first material and a second layer formed of a second material, the first material and second materials being different materials. The first layer has a first thickness and the second layer has a second thickness, the thicknesses of the first and second layer being selected to create optical resonances at the first frequency ω1 and a second frequency ω2 which is a harmonic of ω1 and the thicknesses of the first and second layer also being selected to enhance nonlinear coupling between the first frequency ω1 and a second frequency ω2.

A transparent display provides eye protection from lasers and other high intensity light sources. The transparent display allows users to view objects clearly through the display while also presenting text, graphics or video on the display surface. Simultaneously, the display assembly comprises a component that provides eye protection against high power radiation sources. The transparent display with eye protection provides both protection from high power light sources and an additional cockpit display surface for presentation of information including graphical images, symbology, video, text, and other data.

A method and apparatus to generate harmonically related laser wavelengths includes a pair of lenses at opposing faces of a non-linear optical material. The lenses are configured to promote incoming and outgoing beams to be normal to each outer lens surface over a range of acceptance angles of the incoming laser beam. This reduces reflection loss for higher efficiency operation. Additionally, the lenses allow a wider range of wavelengths for lasers for more universal application. Examples of the lenses include plano-cylindrical and plano-spherical form factors.

The invention is a nonlinear Raman optical device generating zig-zag radiation beam paths in a nonlinear medium having dichroic coatings reflecting at a pump radiation wavelength, with a first mirror between an injected beam of pump radiation and a first end of the nonlinear medium and a second mirror at a second end of the nonlinear medium, the second mirror being partially reflecting at a first Stokes wavelength of the pump radiation.

An optical amplifier arrangement has optical parametric amplifiers and white light generations and harmonic generation, in particular frequency doubling, for generating a wide visible to infrared, in any case near-infrared, spectrum of coherent ultra-short light pulses, in particular with a pump laser, and also to a . A method During operation the fundamental is in a wavelength range above 950 nm, and the second signal light and the second idler light of the second optical parametric amplifier together cover a tunability range of wavelengths between 500 nm and 5 μm, in particular between 550 nm and 3 μm, wherein between wavelengths in the tunability range throughout continuous tuning can be carried out, namely through the degeneration range of the second optical parametric amplifier (OPA2) at the fundamental of the pump laser.

A system for determining a second-order nonlinear susceptibility of a material includes a laser light source, a polarization modulator, a light collector, a polarization detector and a controller. The controller can obtain the second-order nonlinear susceptibility of the sample to be tested according to the test data. The system for determining the second-order nonlinear susceptibility of a material can directly test a material (block or film) with a thickness of hundreds of nanometers, and draw a second-order nonlinear susceptibility fitting curve of the material according to the test results of the optical system.