“…However, the gain coefficient in the L-band window is smaller than that in the C-band, higher pump power and longer length of the doped fiber are normally used with L-band EDFA [5]. In literature, various gain enhancement techniques have been proposed to enhance the gain of L-band EDFA such as using narrow-band end-reflectors to feed a small fraction of the amplified spontaneous emission (ASE), up to a few tenths of a milliwatt, back into the EDF [6], utilizing unwanted backward ASE as a secondary pump source for the un-pumped section of erbium-doped fiber (EDF) [7], placing an optical circulator between two EDF segments in a two-stage reflective-type amplifier structure [8], utilizing a bidirectional pumping structure via inserting a 980 nm pump laser diode in the input part [9], incorporating a fiber Bragg grating (FBG) to reflect part of the C-band backward ASE into the EDF [10]− [13] or tunable band-pass filter in a double-pass configuration [14], adding a short length of forward pumped EDF in front of a double-pass amplifier [15], using loop configuration and a C-band seed signal [16]. Among the other gain enhancement techniques proposed is the use of a two stage structure with a bypass isolator [17] or in-line FBG with forward-backward pumping scheme [18], a three-stage structure of EDF pumped by 980 nm and 1480 nm laser diodes, which can achieve 35 dB gain with 5 dB noise figure [19] and the use of residual pump power in a three-stage configuration [20]− [21].…”