The optical gain e.g. from a fiber amplifier has some dependence on the wavelength, which can be disturbing. For example, in optical fiber communications with wavelength division multiplexing, the wavelength dependence of the gain can unbalance the powers in the transmitted channels. Therefore, it is common to apply methods for gain equalization, also called gain flattening. There are various technological options:
- For a given kind of active fiber, the shape of the gain spectrum can be optimized by adjusting the average inversion level of the laser-active ions. This can be done e.g. by varying the pump power or the length of the active fiber.
- The material composition of the fiber core can be optimized. For example, silica fibers can be optimized with various codopants, and fluoride fibers can offer a fairly flat gain spectrum.
- Amplifier fibers of different glass compositions can be combined in an amplifier chain to obtain a wideband hybrid amplifier. Such a device may also contain a Raman amplifier.
- Another approach is a split-band amplifier, where a wavelength-dependent splitter distributes the signal content over two or more different fiber amplifiers, and another wavelength-dependent fiber coupler serves to recombine the spectral components.
- Optical filters (gain flattening filters) can be used, which have higher losses in wavelength regions where the gain is higher. Such filters are often based on fiber Bragg gratings (long-period gratings, slanted gratings or chirped gratings), although various other types of filters have been demonstrated.
The optimization of a multi-stage amplifier with flattening filters is a complex task, since it is not obvious, e.g., which combination of amplifiers and filters gives the best results in terms of noise figure and power efficiency. A typical solution for a two-stage amplifier based on doped silica fibers would include an optical filter between the two stages.
The gain spectrum of a Raman amplifier can be flattened by using multiple pump beams  with well-balanced pump power levels.
|||K. Inoue et al., “Tunable gain-equalization using a Mach–Zehnder optical filter in multistage amplifiers”, IEEE Photon. Technol. Lett. 3, 718 (1991)|
|||S. F. Su et al., “Gain equalization in multiwavelength lightwave systems using acousto-optic tunable filters”, IEEE Photon. Technol. Lett. 4, 269 (1992)|
|||R. Kashyap et al., “Wavelength flattened saturated erbium amplifier using multiple side-tap Bragg gratings”, Electron. Lett. 29 (11), 1025 (1993)|
|||B. Clesca et al., “1.5 μm fluoride-based fiber amplifiers for wideband multichannel transport networks”, Opt. Fiber Technol. 1, 135 (1995)|
|||A. M. Vengsarkar et al., “Long-period fiber-grating-based gain equalizers”, Opt. Lett. 21 (5), 336 (1996)|
|||N. Park et al., “High-power Er–Yb-doped fiber amplifier with multichannel gain flatness within 0.2 dB over 14 nm”, IEEE Photon. Technol. Lett. 8, 1148 (1996)|
|||Y. Emori et al., “100 nm bandwidth flat-gain Raman amplifiers pumped and gain-equalized by 12-wavelength-channel WDM laser diode unit”, Electron. Lett. 35, 1355 (1999)|
|||M. Harurnoto et al., “Gain-flattening filter using long-period fiber gratings”, J. Lightwave Technol. 20 (6), 1027 (2002)|
|||Ik-Bu Sohn et al., “Gain flattened and improved EDFA using microbending long-period fibre gratings”, Electron. Lett. 38 (22), 1324 (2002)|
If you like this article, share it with your friends and colleagues, e.g. via social media: