Multi wavelength gain flattened erbium-doped fiber amplifier Manufacturers

To be the stage of realizing dreams of our employees! To build a happier, far more united and far more specialist team! To reach a mutual profit of our customers, suppliers, the society and ourselves for Multi wavelength gain flattened erbium-doped fiber amplifier, We will keep working hard and as we try our best to supply the best quality products, most competitive price and excellent service to every customer. Your satisfaction, our glory!!!
Multi wavelength gain flattened erbium-doped fiber amplifier, At Existing, our solutions have been exported to more than sixty countries and different regions, such as Southeast Asia, America, Africa, Eastern Europe, Russia, Canada etc. We sincerely hope to establish wide contact with all potential customers both in China and the rest part of the world.

Hot Products

  • L-band ASE Broadband Light Source Module For Optical Sensor

    L-band ASE Broadband Light Source Module For Optical Sensor

    As a professional L-band ASE Broadband Light Source Module For Optical Sensor manufactures, You can rest assured to buy L-band ASE Broadband Light Source Module For Optical Sensor from our factory and we will offer you the best after-sale service and timely delivery.
  • 1683nm 10mW DFB Butterfly Laser Diode For Ethane C2H6 Gas Sensing

    1683nm 10mW DFB Butterfly Laser Diode For Ethane C2H6 Gas Sensing

    1683nm 10mW DFB Butterfly Laser Diode For Ethane C2H6 Gas Sensing have been designed specifically to satisfy the requirements of the sensor application. The devices feature high output power and wide operating temperature range. Their 14-pin butterfly packages are either pincompatible with standard SONET OC-48 devices.
  • Erbium-ytterbium Co-doped Single-mode Fiber

    Erbium-ytterbium Co-doped Single-mode Fiber

    BoxOptronics Erbium-ytterbium co-doped single-mode fibers are mainly used in high-power telecom/CATV fiber amplifiers, laser ranging, lidar, and eye-safe lasers. The optical fiber has low splicing loss and high light-to-light conversion efficiency. Higher absorption coefficient guarantees output power and lower cost. The optical fiber can adjust the absorption coefficient and gain spectrum with good consistency.
  • 1550nm 100mW DFB PM Fiber Butterfly Laser Diode

    1550nm 100mW DFB PM Fiber Butterfly Laser Diode

    The 1550nm 100mW DFB PM fiber Butterfly Laser Diode is based on multiquantum well (MQW) distributed-feedback (DFB) and a highly reliable ridge waveguide structure. This device is housed in a high performance, 14-pin butterfly package and coupled to 1m of FC/APC-connectorized polarization-maintaining fiber.
  • 1290nm DFB Coaxial Laser Diode TEC Up to 7mW

    1290nm DFB Coaxial Laser Diode TEC Up to 7mW

    1290nm DFB Coaxial Laser Diode TEC Up to 7mW is the DFB laser diode coupled to an optical fiber and packaged into a hermetic case. The output power is available from 1MW, 1270nm~1610nm CWDM wavelength available.
  • 1X2 Polarization Beam Combiner Splitter

    1X2 Polarization Beam Combiner Splitter

    1X2 Polarization Beam Combiner Splitter is designed to either combine or split linearlypolarized light. When used as a combiner, the linearly polarized input lights are combined into a single output with two orthogonal linear polarizations. When used as a splitter, an input light with two orthogonal linear polarizations is split into two outputs each with a single linear polarization. These polarization beam combiners are frequently utilized to combine the light from two pump lasers into a single fiber to increase the power input to an erbium-doped fiber amplifier or Raman amplifier.

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