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  • 808nm 60 Watt Fiber Coupled Diode Laser

    808nm 60 Watt Fiber Coupled Diode Laser

    The 808nm 60 Watt Fiber Coupled Diode Laser, 60W power, an 808nm wavelength, and a 106um fiber core diameter. They are also based on high reliability multi-chip technology. They are intended for use as diode pumped solid state laser pumps. The single emitter sources are driven in a series configuration and are launched into an output fiber with a 106 micron small core diameter by employing high power micro-optics. All of these multi-single emitter fiber coupled devices are cycled through a robust burn-in and inspection process to ensure long lifetime and durability. We offered with a one year warranty and typically ship from stock.
  • 1550nm 500mW Single Wavelength CW DFB Fiber Laser Module

    1550nm 500mW Single Wavelength CW DFB Fiber Laser Module

    This 1550nm 500mW Single Wavelength CW DFB Fiber Laser Module adopts DFB laser chip and high-power gain optical path module to realize the high-power output of single-mode fiber. The professionally designed laser driving and temperature control circuit ensures the safe and stable operation of the laser.
  • Multi Wavelength Gain Flattened EDFA Amplifier

    Multi Wavelength Gain Flattened EDFA Amplifier

    Multi Wavelength Gain Flattened EDFA Amplifier is a series of fiber amplifiers used in optical fiber communication system. It can amplify multiple wavelength signals in C-band at the same time, and keep the same gain among all wavelengths, with gain flatness ≤ 1.5dBm Which with wide spectrum, multi wavelength, flat gain, high gain and low noise.
  • 1270nm 5mW TO-CAN DFB Laser Diode

    1270nm 5mW TO-CAN DFB Laser Diode

    This 1270nm 5mW TO-CAN DFB Laser Diode is a product operable over a broad temperature range with a low temperature-wavelength coefficient. It is well suited for applications such as communications research, interferometry, and optical reflectometry for distance measurement in fiber or free space. Each device undergoes testing and burn-in. This laser comes packaged in a 5.6 mm TO Can. It contains an integrated aspheric focusing lens in the cap, allowing the focus spot and numerical aperture (NA) to be matched to SMF-28e+ fiber.
  • High Performance 1450nm DFB Butterfly Laser Diode

    High Performance 1450nm DFB Butterfly Laser Diode

    The High performance 1450nm DFB Butterfly Laser Diode built in Built-in monitor photodiode, thermo-electric cooler TEC and thermistor, Single mode or Polarization maintaining fiber pigtail,Wavelength/temperature coefficient 0.01nm/℃.
  • Low cost C-band ASE Broadband Light Source

    Low cost C-band ASE Broadband Light Source

    This Low cost C-band ASE Broadband Light Source has C-band wavelength, with 5~7dB spectral flatness and SM fiber and for fiber sensing applications.
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  • Reviews

  • The type of fiber laser

  • ASE light source

    ASE light source is specially designed for laboratory experiment and production. The main part of the light source is gain medium erbium-doped fiber and high-performance pump laser. The unique ATC and APC circuits ensure the stability of the output power by controlling the output of the pump laser. By adjusting APC, the output power can be adjusted within a certain range. Simple and intelligent operation and remote control.

  • Fiber laser applications

  • The basic characteristics and application fields of optical fiber temperature measurement

  • Polarization of Laser Radiation

    In most cases the emitted light from the laser is polarized. Usually linearly polarized, that is, the electric field oscillates in a specific direction perpendicular to the direction of propagation of the laser beam. Some lasers (eg, fiber lasers) do not produce linearly polarized light, but other stable polarization states, which can be converted to linearly polarized light using a suitable combination of waveplates. In the case of broadband radiation, and the polarization state is wavelength dependent, the above method cannot be used.

  • Short wavelength narrow linewidth fiber laser

    For spectral synthesis technology, increasing the number of synthesized laser sub-beams is one of the important ways to increase the synthesis power. Expanding the spectral range of fiber lasers will help increase the number of spectral synthesis laser sub-beams and increase the spectral synthesis power [44-45]. At present, the commonly used spectrum synthesis range is 1050～1072 nm. Further expanding the wavelength range of narrow linewidth fiber lasers to 1030 nm is of great significance to the spectrum synthesis technology. Therefore, many research institutions have focused on short wavelength (wavelength less than 1040 nm) narrow line Wide fiber lasers were studied. This paper mainly studies the 1030 nm fiber laser, and extends the wavelength range of the spectrally synthesized laser sub-beam to 1030 nm.

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