An optical fiber amplifier based on a fluoroindate fiber doped with praseodymium (Pr3+:InF3) has been designed. The chosen fiber has a double-cladding and a 2-D shape. The electromagnetic behavior of the fiber has been simulated via a Finite Element Method (FEM) software, and the design of the fiber amplifier has been performed via a computer code, solving the rate-equations and power propagation equations. The gain G and the Amplified Spontaneous Emission (ASE) noise have been investigated as a function of different input parameters as the input signal power Ps0, the fiber length Lfiber, and the signal wavelength λs. The simulated fiber amplifier exhibits a bandwidth BG close to BG = 100 nm around the central signal wavelength λs = 4 µm, and a gain G close to G = 30.7 dB, when an input signal power Ps = 10 µW and a pump power Pp = 75 mW are considered. This pump value seems particularly low and further investigation will be performed to better understand this unexpected promising value.
Design of a Mid-IR Optical Fiber Amplifier based on a Pr3+:InF3 Glass / Loconsole, A. M.; Francione, V. V.; Annunziato, A.; Anelli, F.; Khan, Md. I.; Taccheo, S.; Prudenzano, F.. - 13003:(2024). (Intervento presentato al convegno Fiber Lasers and Glass Photonics: Materials through Applications IV 2024 tenutosi a fra nel 2024) [10.1117/12.3017504].
Design of a Mid-IR Optical Fiber Amplifier based on a Pr3+:InF3 Glass
Loconsole A. M.;Francione V. V.;Annunziato A.;Anelli F.;Prudenzano F.
2024-01-01
Abstract
An optical fiber amplifier based on a fluoroindate fiber doped with praseodymium (Pr3+:InF3) has been designed. The chosen fiber has a double-cladding and a 2-D shape. The electromagnetic behavior of the fiber has been simulated via a Finite Element Method (FEM) software, and the design of the fiber amplifier has been performed via a computer code, solving the rate-equations and power propagation equations. The gain G and the Amplified Spontaneous Emission (ASE) noise have been investigated as a function of different input parameters as the input signal power Ps0, the fiber length Lfiber, and the signal wavelength λs. The simulated fiber amplifier exhibits a bandwidth BG close to BG = 100 nm around the central signal wavelength λs = 4 µm, and a gain G close to G = 30.7 dB, when an input signal power Ps = 10 µW and a pump power Pp = 75 mW are considered. This pump value seems particularly low and further investigation will be performed to better understand this unexpected promising value.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
