The invention relates to a supercontinuum source comprising a pump light source arranged to emit pump light and a nonlinear fiber having a core arranged to receive the pump light. The supercontinuum comprises infrared wavelengths generated in the nonlinear fiber from the pump light. The nonlinear fiber has a dispersion profile comprisinga zero dispersion wavelength,a positive peak value at a peak wavelength longer than the zero dispersion wavelength,a minimum value of dispersion at a minimum wavelength longer than the peak wavelength. The pump light is arranged to comprise substantial energy at one or more preferred pump wavelengths which are 10 nm longer than the zero dispersion wavelength or more, The invention also relates to a supercontinuum pump source comprising a nonlinear fiber having a core comprising a fluoride glass and having a core diameter smaller than 7 ?m, where the fiber has a numerical aperture of more than 0.26.

A soliton generation apparatus comprising: an optical resonator; a pumping laser for providing light at a pumping wavelength into the optical resonator; a generator for generating multiple solitons in the optical resonator; a detuning device for changing the wavelength detuning between the pumping laser wavelength and an optical resonance wavelength of the optical resonator to remove at least one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises at least one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator.

A supercontinuum source including a pump light source arranged to emit pump light and a nonlinear fiber having a core arranged to receive the pump light. The supercontinuum includes infrared wavelengths generated in the nonlinear fiber from the pump light. The nonlinear fiber has a dispersion profile including a zero dispersion wavelength, a positive peak value at a peak wavelength longer than the zero dispersion wavelength, a minimum value of dispersion at a minimum wavelength longer than the peak wavelength. The pump light is arranged to include substantial energy at one or more preferred pump wavelengths which are 10 nm longer than the zero dispersion wavelength or more. Also, a supercontinuum pump source including a nonlinear fiber having a core including a fluoride glass and having a core diameter smaller than 7 ?m, where the fiber has a numerical aperture of more than 0.26.

The present invention relates to an integrated circuit, in particular a photonic integrated circuit, for generating an electrical and/or optical frequency comb signal, the integrated circuit comprising: a pulse generation unit comprising an input port for receiving an optical high frequency signal. The present invention provides a Kerr-ring for the generation of an optical frequency comb signal. The use of the Kerr-ring for the optical frequency comb generation makes the integration possible. The present invention further relates to an optical system and a test and measurement device.

Ultrashort pulsed laser systems are described. In one example, a pulsed laser system includes a source laser configured to emit a pulsed source laser beam, a splitter configured to split the source laser beam into first and second input laser beams, a first amplifier module configured to amplify the first input laser beam using chirped pulse amplification (CPA) and to produce, at a first output port, a first output laser beam in a first spectral range based on soliton self-frequency shift (SSFS) in the first amplifier module, a second amplifier module configured to amplify the second input laser beam using CPA and to produce an intermediate beam based on SSFS in the second amplifier module, and a mid-infrared fiber configured to receive the intermediate beam and to produce, at a second output port, a second output laser beam in a second spectral range based SSFS in the mid-infrared fiber.

A soliton generation apparatus comprising: an optical resonator; a pumping laser for providing light at a pumping wavelength into the optical resonator; a generator for generating multiple solitons in the optical resonator; a detuning device for changing the wavelength detuning between the pumping laser wavelength and an optical resonance wavelength of the optical resonator to remove at least one soliton of the generated multiple solitons to provide (i) a plurality of solitons that comprises at least one less soliton than that of the generated multiple solitons or (ii) a single soliton in the optical resonator.

An integrable, non-reciprocal optical component, with guidance, between two magneto-plasmonic interfaces each formed between a dielectric and a metal. An optical port and an input signal passes through a selection region providing a selected signal whose energy is concentrated in a single plasmonic mode, LRSPP or SRSPP, by a selection aperture of a width for which these modes have optical impedances that differ significantly from each other, one of which (z1eff) is close to, or equal to, the input optical impedance (z0eff). The selected signal passes through a differentiation region, which enhances the asymmetry between the two magneto-plasmonic interfaces, to concentrate its energy on a single magneto-plasmonic interface. The differentiated signal passes through a non-reciprocal treatment region formed by two magneto-plasmonic interfaces of non-equivalent geometries. The input signal will thus undergo different treatment from a reverse signal.

A device and method for high-speed tuning soliton microcomb comprising an on-chip high-Q lithium niobate (LN) microresonator as a comb resonator whose dispersion is engineered for soliton comb generation where a strong electro-optic Pockels effect is used to dynamically tune the soliton repetition rate, with integrating electrooptic tuning and modulation elements directly integrated into the comb resonator.

Provided is a frequency shifting optical swept light source system. The system includes a light source that emits light; an amplifier that amplifies the light output from the light source; an optical converter that shifts a frequency of the amplified light and compresses a spectrum of the amplified light; and a controller that controls a current signal applied to the light source such that a repetition rate of the light output from the light source is adjusted, so that an intensity of the amplified light is adjusted, to thereby adjust a position of the compressed spectrum with respect to a predetermined frequency band.

Multiplex CARS microscopy device for analysing a sample (Ech) comprising: -a laser source (LS) suitable for emitting a primary beam (FP) having a first wavelength .sub.1, in the form of pulses (IL1) with a power called the primary power; -an optical fibre (F) supporting fewer than ten modes, said pulses propagating through the optical fibre (F) in anomalous dispersion regime so as to generate, from the primary beam, an output beam (FSC) containing a plurality of second wavelengths forming a supercontinuum (SC), and said first wavelength .sub.1, the second wavelengths being generated by non-linear conversion of the first wavelength ; -an optical system (MO) suitable for focusing the output beam onto said sample, so as to generate an anti-Stokes beam (STK) via stimulated Raman scattering induced by at least one of the second wavelengths and the first wavelength .sub.1 present in the output beam; -a photodetector (Det) suitable for detecting the anti-Stokes beam.