The principle of the conductor optical amplifier is similar to that of the rare earth doped fiber amplifier, but there are some differences. The amplification characteristics of the conductor optical amplifier mainly depend on the characteristics of the active layer and the laser cavity. Although it is also a particle number inversion amplification luminescence, the medium of luminescence is non-equilibrium carriers, i.e. electron hole pairs, rather than rare elements. The luminescence of semiconductor can be divided into photoluminescence, electroluminescence and cathodoluminescence according to different excitation modes.
The PL-SOA-A-A81-W1310-SASA is a polarization-insensitive optical amplifier with advanced epitaxial wafer growth and opto-electronic packaging tec...
The PL-SOA-A-A81-W1550-SASA is a polarization-insensitive optical amplifier with advanced epitaxial wafer growth and opto-electronic packaging tec...
The PL-SOA-1-A81-W1600-PA 1600nm Semiconductor Optical Amplifier (SOA) is single-pass, traveling-wave amplifier that perform well with both monoch...
The PL-SOA-1-A81-W1650-PA 1650nm Semiconductor Optical Amplifier (SOA) is single-pass, traveling-wave amplifier that perform well with both monoch...
The Raman-AMP-1653.7-1W-CW offers 1120-1700 nm Raman fiber amplifiers to overcome the limited emission spectral region of the rare-earth-doped fib...