I. Introduction
Fiber Raman amplifiers (FRAs) are attractive devices in high-capacity and wideband optical transmission systems/photonic networks, because they can provide wide gain bands in any wavelength region required by properly setting their pump wavelengths [1]–[4]. In particular, the FRAs can be used as post-, pre-, and inline amplifiers in wavelength-division-multiplexing (WDM) systems, and can support new gain bands beyond the gain bands offered by rare-earth-doped fiber amplifiers such as erbium-doped fiber amplifiers (EDFAs) and thulium-doped fiber amplifiers (TDFAs) [5]–[13]. Two types of FRAs with different active fibers have been reported to date, namely: 1) silica FRAs (S-FRAs) [1]; and 2) tellurite FRAs (T-FRAs) [14]. Hybrid tellurite/silica FRAs (hybrid FRAs), which basically are a serial combination of a T-FRA and an S-FRA, were also reported [15], [16]. Note that S-FRAs can yield, in a distinct way, distributed Raman amplification (DRA) in deployed transmission fibers [1], [17]. Some S-FRAs achieved seamless gain bandwidths of up to 100 nm in the configurations of discrete (or lumped), distributed, and hybrid discrete/distributed amplification [18]–[21].