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RP Fiber Power – Simulation and Design Software
for Fiber Optics, Amplifiers and Fiber Lasers

Example Case: Erbium-doped Fiber Amplifier

Description of the Model

We simulate a fiber amplifier with the following properties:

Results

Figure 1 shows the power distributions in the amplifier fiber, including ASE, and also the fractional erbium excitation level. The latter is higher on the left side, because the signal power is lower there.

power distribution in erbium-doped fiber amplifier
Figure 1: Power distribution in the fiber.

Figure 2 shows the optical spectrum of amplified spontaneous emission (ASE) for both directions. Backward ASE is significantly stronger at short wavelengths. This is the usual case for quasi-three-level gain media.

ASE spectrum of erbium-doped fiber amplifier
Figure 2: Spectrum of the amplified spontaneous emission (ASE).

Next we consider the saturation characteristics: the amplifier gain is reduced for high input power levels. Curves are shown for pump powers of 100 mW to 500 mW (from each side).

saturation characteristics of erbium-doped fiber amplifier
Figure 3: Saturation characteristics.

Now we check the dependence of amplifier output signal power on the fiber length. This shows that the fiber length is in that case not a very critical parameter for the power efficiency.

fiber amplifier: dependence on fiber length
Figure 4: Variation of the fiber length.

The last graph shows the gain and the noise figure at the signal wavelength as functions of the total pump power.

gain and noise figure of EDFA
Figure 5: Gain and noise figure as functions of pump power for a signal input power of 1 mW.

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