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Wavelength Converted Fiber Laser

Single frequency wavelength converted fiber lasers from 193 nm to 795 nm. Narrow linewidth, low phase noise output for quantum sensing, spectroscopy, magnetometry, and atomic physics.

  • 193 nm Single-Frequency Frequency-Converted Laser

    193 nm is one of the most demanding wavelengths in photonics. Generating coherent output here requires multi-stage frequency conversion, DUV-grade optics, and a fiber seed stable enough to preserve narrow linewidth through every conversion step.

    Seed Laser Pro’s 193 nm Single-Frequency Laser delivers 1 to 3 mW of CW output at 193.3 nm. Linewidth stays below 80 kHz. Side-mode suppression ratio reaches 20 to 24 dB. The free-space output beam is clean, with M² below 1.4 and 1.0 mm diameter at the output port.

    Built for semiconductor lithography research, precision microfabrication, DUV spectroscopy, and medical applications. Custom wavelength configurations are available on request.

    PRODUCT FEATURES 

    • Deep UV Single-Frequency Output at 193.3 nm : Continuous-wave single longitudinal mode output in the deep ultraviolet. Coherent, stable, and fully solid-state. No gas mixtures. No high-voltage discharge. No fluorine handling.
    • Sub-80 kHz Linewidth from Fiber Seed Architecture : Spectral purity inherited directly from the narrow-linewidth fiber seed. To optimize seeding for an ArF amplifier, linewidth must be controlled below 4 GHz. At sub-80 kHz, this laser sits three orders of magnitude inside that threshold.
    • Active Power Stabilization : Output power stability within 1% RMS over two hours. Thermal and conversion efficiency drift in the DUV stage are actively compensated throughout continuous operation.

    TYPICAL APPLICATIONS 

    • Semiconductor Lithography Research and Metrology : 193 nm is the wavelength of ArF excimer lithography, used across the industry for DUV patterning. This CW single-frequency source is not a production lithography laser. It serves as a coherent reference for optics metrology, interferometric wavefront testing, and defect inspection setups where excimer coherence is too limited.
    • Precision Microfabrication : 193 nm photons carry 6.4 eV each. That energy level enables direct ablation of polymers, carbon compounds, and biological tissue. Thermal damage to surrounding material is minimal because energy coupling happens at the photochemical level rather than through heat.
    • Medical Applications : 193 nm is the clinical wavelength for corneal reshaping in refractive surgery. Coherent CW output with stable power and narrow linewidth supports both surgical laser systems and the calibration and research setups around them.
    • Deep UV Spectroscopy : Sub-80 kHz linewidth at 193 nm resolves fine spectral features in UV absorption spectra of molecules, ions, and semiconductor materials that broadband or incoherent DUV sources cannot distinguish.

    Custom wavelength or output power required? The central wavelength is customizable. Custom power configurations and OEM integration support are available. Contact Seed Laser Pro’s engineering team at the design stage.

  • 266 nm Single-Frequency Frequency-Converted Laser

    266 nm sits in the UV-C band, four times the wavelength of the 1064 nm fundamental. Reaching it requires fourth-harmonic generation from a near-infrared fiber seed. Doing it with narrow linewidth requires that every conversion stage preserves the spectral quality of the starting source.

    Seed Laser Pro’s 266 nm Single-Frequency Laser delivers 5 to 15 mW of CW output at 266 nm. Linewidth is 5 to 25 kHz. Power stability holds at 1% RMS over three hours. Wavelength tuning range covers 50 to 150 pm. Free-space output with M² below 1.3 and 1.0 mm typical beam diameter.

    Built for semiconductor material processing, UV fluorescence analysis, photochemistry, and precision UV spectroscopy. Custom wavelength configurations are available.

    PRODUCT FEATURES

    • Fourth-Harmonic Generation at 266 nm : CW output at 266 nm produced through two sequential second-harmonic generation steps from a 1064 nm single-frequency fiber seed. The conversion chain is designed to preserve narrow linewidth at each stage. The 266 nm output inherits the spectral purity of the fiber source.
    • Sub-25 kHz Linewidth : Linewidth between 5 and 25 kHz at 266 nm. Coherence length at this linewidth exceeds several kilometers. Sufficient for high-resolution UV spectroscopy, interferometric measurements, and precision material processing where coherence quality affects the result.
    • Active Power Stabilization : Output power stable at 1% RMS over three hours of continuous operation. Adjustable from 10 to 100% of the set output level throughout operation.
    • Clean Free-Space Output : M² below 1.3, 0.8 to 1.2 mm beam diameter, beam waist within 1 m of the output port. Fits standard optical tables at 290 × 500 × 130 mm.

    TYPICAL APPLICATIONS 

    • Semiconductor Processing and Inspection : 266 nm photons carry 4.66 eV per photon. That energy level exceeds the bandgap of many semiconductor and dielectric materials, enabling direct photochemical processing without the thermal damage that longer UV wavelengths cause. Narrow linewidth CW output supports both direct processing and interferometric inspection of processed surfaces.
    • Material Analysis and UV Fluorescence : Many organic molecules, aromatic compounds, and biological markers have absorption and fluorescence excitation bands in the 260 to 270 nm range. A single-frequency, narrow-linewidth 266 nm source provides selective excitation of specific spectral features that broadband UV lamps cannot resolve.
    • Photochemistry Research : Photochemical reactions initiated at 266 nm are used in polymer synthesis, photocatalysis, and photodegradation studies. Narrow linewidth allows wavelength-selective excitation of specific reactant absorption bands for controlled reaction chemistry.
    • UV Spectroscopy and Metrology : Sub-25 kHz linewidth at 266 nm supports high-resolution absorption spectroscopy of UV-active species and interferometric metrology of UV optical components. Both applications require coherence far beyond what pulsed or broadband UV sources provide.

    Need a custom configuration? Central wavelength is customizable. OEM integration, custom power levels, and engineering support available at the design stage.

  • 509 nm Single-Frequency Frequency-Converted Laser

    Seed Laser Pro’s 509 nm single-frequency laser delivers 0.05 to 3 W of CW output at 509.4 nm with 2 to 10 kHz linewidth. Built for cesium Rydberg atom research, cold atom physics, and solar cell processing. Free-space and fiber output available. Custom wavelength configurations on request.

    PRODUCT FEATURES

    • Sub-10 kHz linewidth, single longitudinal mode CW output at 509.4 nm
    • Output power 0.05 to 3 W, adjustable from 10 to 100%, RMS stability below 0.7%
    • Wavelength tuning range 100 to 300 pm, polarization extinction ratio 20 to 25 dB
    • Free-space or fiber output, M² below 1.1, 0.7 to 1.1 mm beam diameter

    TYPICAL APPLICATIONS

    • Cesium Rydberg atom physics and two-step Cs excitation at 509 nm combined with 852 nm
    • Cold atom physics, state-selective detection, and photoionization experiments
    • Solar cell characterization and photovoltaic laser processing at peak silicon quantum efficiency
    • Medical and dermatological applications in the green wavelength band
  • 532nm Low Noise Single-Frequency Laser

    Green lasers are common. A 532nm low noise laser with single longitudinal mode operation, sub-10 kHz linewidth, and M² below 1.1 is not.

    Techwin’s 532 nm frequency-converted laser produces 0.05 to 4 W of continuous-wave green output through second harmonic generation from a single-frequency fiber seed. Linewidth sits between 2 and 10 kHz. Output power stability holds at 0.3% RMS over six hours. Wavelength tuning range reaches 200 pm typically. Both free-space and fiber output options are available. This is a precision green laser source built for applications where intensity noise, beam quality, and spectral purity determine the quality of the result.

    PRODUCT FEATURES

    • High-Efficiency Nonlinear Frequency Conversion:  Second harmonic generation from a single-frequency fiber seed produces 532 nm output with high conversion efficiency. The green output inherits the single longitudinal mode operation and low phase noise of the fiber seed, giving this laser its low noise character at 532 nm.
    • M² Below 1.1 Beam Quality:  Near-perfect Gaussian beam profile with output beam diameter of 0.7 to 1.2 mm and beam waist position within 1 m of the output port. Directly usable in tight-focus applications without additional spatial filtering.
    • Intelligent Power Stabilization: Active output power stabilization holds RMS power stability at 0.3% over six hours of continuous operation. Power adjustable from 10 to 100% of the set output level.

    TYPICAL APPLICATIONS

    • Precision Processing:  Low noise, stable output power, and near-diffraction-limited beam quality make this laser suitable for precision microfabrication, laser scribing, and material processing applications where beam quality and power consistency directly affect process quality.
    • Biomedical Applications:  532 nm green light is strongly absorbed by oxyhemoglobin and melanin, making it the standard wavelength for retinal photocoagulation, dermatological treatments, and fluorescence excitation in biological imaging. The low noise and stable output of this system minimize unwanted tissue effects from power fluctuations.
    • Scientific Instruments and Quantum Optics:  Single-frequency, narrow-linewidth 532 nm output is used in holography, interferometry, Raman spectroscopy, optical tweezers, and as a pump source for optical parametric oscillators targeting visible and near-infrared wavelengths. Low intensity noise is the primary requirement across all of these.
  • 780 nm Frequency-Converted Laser for Rubidium Cooling

    780.24 nm is the rubidium D2 line. Every laser cooling experiment, magneto-optical trap, atom interferometer, and rubidium atomic clock built around rubidium atoms needs a laser locked to this transition. Techwin’s 780 nm frequency-converted laser is purpose-built for that requirement.

    The output is generated through second harmonic generation from a 1560 nm single-frequency fiber seed laser. The 780 nm output inherits the narrow linewidth, single longitudinal mode operation, and low phase noise of the fiber seed directly. High-efficiency nonlinear frequency conversion technology and power stabilization produce stable, low-noise output at 780 nm in a compact module format ready for integration into cold atom physics platforms and quantum sensing instruments.

    PRODUCT FEATURES

    • High-Efficiency SHG Frequency Conversion: Second harmonic generation from a 1560 nm single-frequency fiber seed produces 780 nm output with conversion efficiency optimized through nonlinear crystal design and optical path optimization. The 780 nm output carries the spectral purity of the fiber seed.
    • Excellent Beam Quality: Near-diffraction-limited beam quality from the fiber-based source, optimized through beam quality correction in the output stage. Suitable for direct free-space coupling into vacuum chambers and optical setups without additional spatial filtering.
    • Power Stabilization: Active power stabilization keeps output power consistent across operating conditions. Stable output power is a direct requirement for controlled optical pumping efficiency in rubidium cooling and trapping experiments.

    TYPICAL APPLICATIONS

    • Rubidium Laser Cooling and Magneto-Optical Trapping: The 780 nm D2 transition of rubidium-85 and rubidium-87 is the standard wavelength for laser cooling, magneto-optical trapping, and Bose-Einstein condensate experiments. This laser provides the frequency-stable, narrow-linewidth output required to maintain resonance with the D2 line throughout the cooling and trapping sequence.
    • Atom Interferometry and Quantum Sensing: Rubidium atom interferometers used in gravimetry, inertial navigation, and fundamental physics require a 780 nm source with tight frequency control and stable output. This frequency-converted laser provides the spectral characteristics atom interferometric systems demand.
    • Scientific Instruments and Atomic Physics Research: Rubidium atomic clocks, Rydberg atom experiments, quantum computing platforms using rubidium qubits, and precision spectroscopy all operate at or near the 780 nm D2 line. This laser serves as the primary light source for any rubidium-based experiment requiring single-frequency, stable 780 nm illumination.
  • 795 nm Single-Frequency Frequency-Converted Laser

    Seed Laser Pro’s 795 nm single-frequency laser is built around the rubidium D1 transition. It delivers 0.05 to 4 W of CW output at 795 nm with 2 to 5 kHz linewidth and power stability below 0.8% RMS. Designed for SERF magnetometers, rubidium atomic physics, and precision measurement systems. Free-space and fiber output available. Custom wavelength on request.

    Product Features

    • Sub-5 kHz linewidth, single longitudinal mode CW output at 795 nm
    • Output power 0.05 to 4 W, adjustable 10 to 100%, RMS stability below 0.8%
    • Wavelength tuning range 100 to 300 pm, polarization extinction ratio 20 to 26 dB
    • Free-space or fiber output, M² below 1.1, 0.7 to 1.1 mm beam diameter

    Typical Applications

    • SERF magnetometers requiring frequency-stable optical pumping at the rubidium D1 line
    • Rubidium atomic physics, optical pumping, and spin-exchange relaxation-free experiments
    • Precision magnetic field measurement for medical imaging, navigation, and geophysics
    • Quantum optics, polarization squeezing, and rubidium D1 spectroscopy research
Fiber lasers natively operate in the near-infrared. Nonlinear frequency conversion extends that spectral performance into the visible and UV. Techwin’s wavelength converted fiber laser range produces single frequency output at 193 nm, 266 nm, 509 nm, 532 nm, 780 nm, ...

Frequently Asked Questions

What is a wavelength converted fiber laser?

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It is a single frequency fiber seed laser whose output passes through a nonlinear crystal to produce a shorter output wavelength via SHG, SFG, or harmonic generation. The converted output inherits the linewidth, phase noise, and single longitudinal mode characteristics of the fiber seed directly.

Why use a fiber-based approach for visible and UV wavelengths?

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Fiber seeds provide superior long-term frequency stability, compact form factors, and low maintenance relative to dye lasers or many solid-state alternatives. The nonlinear conversion stage is passive and requires no alignment or adjustment under normal operating conditions. For instruments requiring consistent performance over months or years, this architecture offers a significant practical advantage.

What is the difference between the 780 nm and 795 nm outputs?

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The 780 nm output targets the rubidium D2 transition, used in laser cooling, magneto-optical traps, and atom interferometry. The 795 nm output targets the rubidium D1 transition, which is the standard wavelength for optically pumped rubidium magnetometers and quantum storage protocols. Both are produced by frequency doubling a fiber seed in the 1560 nm to 1590 nm range.

Are these lasers available for OEM integration?

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Yes. Techwin's wavelength converted fiber laser modules are available in OEM-optimized configurations with compact footprints, specified operating temperature ranges, and connector types matched to instrument integration requirements. Contact Techwin at the design stage to discuss configuration options.

Can Techwin supply alternatives to Koheras single frequency lasers?

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Techwin builds on DFB fiber architecture with PM construction throughout and verifies linewidth, phase noise, and polarization extinction ratio on every unit. Techwin is not affiliated with NKT Photonics. For buyers evaluating alternatives to premium single frequency platforms, Techwin's engineering team can review your specification and confirm whether a standard or custom configuration meets your requirements.

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