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The PowerSpectrum™ HPR fiber Bragg-grating (FBG) cavity reflectors are specifically designed for high-power fiber lasers. The HPR reflectors are suitable for multi-kW lasers and are tailored to fit any fiber oscillator design.

The Med-2 Series HPR fiber Bragg-grating (FBG) cavity reflectors are specifically designed for high-power Continuous-Wave (CW) and Quasi-Continuous-Wave (QCW) Thulium (Tm) medical fiber lasers emitting at 1940 nm.

The PowerSpectrum™ RSS Raman Scattering Suppressor reduces the effect of Stimulated Raman Scattering (SRS) and increases laser power and stability.

The WSF series of wavelength suppression filters are band-stop filters that allow to block the transmission of a wavelength or a range of wavelengths over a specified bandwidth.

The WVL series of wavelength locking Fiber Bragg Gratings allow to precisely control and stabilize the wavelength of diode lasers.

TeraXion’s WaveShift series of FBG reflectors are specially designed for use in Raman Fiber Lasers or Amplifiers.  TeraXion’s WaveShift series offer excellent performances in terms of wavelength accuracy, and matching, insertion losses, and power handling

PowerSpectrum™ TPSR-Xtended is a tunable pulse stretcher optimized for high-energy ultrafast lasers.

The PowerSpectrum™ TPSR is a tunable pulse stretcher optimized for industrial and medical ultrafast lasers.

The PowerSpectrum™ CM-V is the most compact and robust, ultrafast pulse stretcher+compressor pair on the market, featuring a PowerSpectrum™ TPSR-V individually designed and tuned to a specific VBG compressor.

The all-fiber PowerSpectrum™ HPSR is a precise and compact fixed-dispersion pulse stretcher that enables optimal pulse recompression within ultrafast laser systems.

TeraXion’s all-fiber PowerSpectrum™ DMR chirped fiber Bragg gratings (CFBG) accurately set the chromatic dispersion in picosecond and femtosecond mode-locked fiber lasers, ensuring that all the wavelengths maintain a proper phase relation.

The ClearSpectrum™ TDCMX-SM chromatic dispersion compensator is slope-matched to G.652 fiber and provides adjustable, simultaneous compensation for all channels across the entire C-band, all within a single device. This 100 Gb/s-ready product supports intensity-modulation direct-detection over distances up to 80 km.

The ClearSpectrum™ DCML is a completely passive chromatic dispersion compensator that utilizes channelized fiber-Bragg gratings (FBGs) technology to provide extraordinarily low-latency while preventing interchannel and intrachannel nonlinear impairments. The chromatic dispersion compensator also features low insertion loss and high input-power handling.

The ClearSpectrum™ CDE is an ultra-compact and passive device that emulates levels of chromatic dispersion equivalent to thousands of kilometers of transport fiber, all within a space-saving module that fits within a half 1U 19-inch rack-mount module and requires no external power supply.

The ClearSpectrum™ TDCMB is a tunable chromatic dispersion management module that provides dispersion compensation and emulation within a single instrument. The module features fiber-Bragg grating (FBG) technology, which enables a broad dispersion range and operational bandwidth while also minimizing size.

The PureSpectrum™ NLL distributed feedback (DFB) laser integrates a high-power mono-mode semiconductor laser (up to 70 mW), built-in frequency discrimination, precision feedback monitoring, and high-speed frequency tuning all into a single, compact module that produces a narrow-linewidth output beam that is extremely stable and has very low noise.

The no-fuss laser module combines a DFB semiconductor laser, a low-noise current-source, and a temperature controller, all within a single, compact package. The LM operates in single-mode, producing as much as 100 mW of optical power with a linewidth less than 1 MHz and is frequency-tunable over a 50 GHz range with 10 MHz resolution.

The fiber Bragg grating (FBG) based ultra-narrowband tunable optical filter, available in both reflection and transmission-reflection models, enables high-isolation, narrowband filtering between 2 GHz and 50 GHz and ultra-narrowband filtering between 50 MHz and 500 MHz. Both models feature a high-precision, thermally-tunable platform capable of positioning peaks with 2 pm precision over a range of +/- 30 GHz from the center wavelength.

Fiber-Bragg-Gratings (FBGs) high-precision optical filters combine unmatched performance and cost effectiveness. They can be tailored for bandwidths as low as 2 GHz and centered between 700 nm to 2100 nm with < 50 pm accuracy. They are offered in different packaging options, including the best-in-class athermal package that features a < 0.5 pm/°C thermal drift. Multi-peak etalon filters with variable peak reflectivity can also be designed to fulfill specific requirements.

The LXM is a compact and rugged semiconductor DFB laser module ideal for phase and frequency noise-sensitive applications related to quantum photonics, telecom link monitoring and radio-frequency conversion. The ultra-narrow LXM-U model features a linewidth below 0.2 kHz, while the LXM-S model is optimised for frequency modulation and reaches > 2 GHz amplitude at a repetition rate of 100 kHz. This turn-key laser module offer high stability and reliable performances.

The LXM is a compact and rugged semiconductor DFB laser module ideal for frequency noise-sensitive applications such as distributed acoustic sensing (DAS), Doppler lidar and FMCW lidar. The ultra-narrow LXM-U model features a linewidth below 0.2 kHz, while the LXM-S model is optimised for frequency modulation and reaches > 2 GHz amplitude at a repetition rate of 100 kHz. This turn-key laser module offer high stability and reliable performances over a wide operating temperature range.

The narrow linewidth and high linearity distributed feedback (DFB) laser diode combines high coherence length and linear frequency modulation response characteristics. Based on an innovative epitaxial-structure design, this monolithic laser diode exhibits unique current modulation properties. It has been designed to ensure a minimal footprint, maximal performance and scalability to high volume applications.

The no-fuss laser module combines a DFB semiconductor laser, a low-noise current-source, and a temperature controller, all within a single, compact package. The LM operates in single-mode, producing as much as 100 mW of optical power with a linewidth less than 1 MHz and is frequency-tunable over a 50 GHz range with 10 MHz resolution.

The LXM is a compact and rugged semiconductor DFB laser module ideal for frequency noise-sensitive applications. The ultra-narrow LXM-U model features a linewidth below 0.2 kHz, while the LXM-S model is optimised for frequency modulation and reaches > 2 GHz amplitude at a repetition rate of 100 kHz. This turn-key laser module offer high stability and reliable performances over a wide operating temperature range.

The PureSpectrum™ NLL distributed feedback (DFB) laser integrates a high-power mono-mode semiconductor laser (up to 70 mW), built-in frequency discrimination, precision feedback monitoring, and high-speed frequency tuning all into a single, compact module that produces a narrow-linewidth output beam that is extremely stable and has very low noise.

The fiber Bragg grating (FBG) based ultra-narrowband tunable optical filter, available in both reflection and transmission-reflection models, enables high-isolation, narrowband filtering between 2 GHz and 50 GHz and ultra-narrowband filtering between 50 MHz and 500 MHz. Both models feature a high-precision, thermally-tunable platform capable of positioning peaks with 2 pm precision over a range of +/- 30 GHz from the center wavelength.

Fiber-Bragg-Gratings (FBGs) high-precision optical filters combine unmatched performance and cost effectiveness. They can be tailored for bandwidths as low as 2 GHz and centered between 700 nm to 2100 nm with < 50 pm accuracy. They are offered in different packaging options, including the best-in-class athermal package that features a < 0.5 pm/°C thermal drift. Multi-peak etalon filters with variable peak reflectivity can also be designed to fulfill specific requirements.