amplifiers (EDFAs) [68]. The RFL gain block consists of a P-doped fiber as the
gain medium; the laser cavity is obtained by FBG inscribed in Ge-doped silica
fibers. The two FBGs are then spliced to the gain medium fiber. The splice losses
could be reduced or even avoided by inscribing the FBGs directly into the
heavily P-doped silica fibers. The number of cavities depends on the Stokes
shift. For a Ge-doped silica fiber, the Stokes shift is limited to 13.2 THz. For
example, five laser cavities are needed to shift the Yb-doped fiber laser pump
emitting at 1060 nm to the pump wavelength of 1480 nm for EDFAs. Using a
heavily P-doped silica fiber, the number of cavities is reduced to only two, thanks
to the Stokes shift of 39.9 THz. This shift is three ...