Presentation Overview Project objectives Gain characteristics of EDFA Gain flattening - non-uniform gain over the spectrum
- implications
Project Objectives - ASE not considered – optimum length is shorter when ASE taken into account
Expand the current EDFA Simulink model to show the gain over the entire 1550nm window - important to know gain in range 1530nm – 1560nm
Consider gain flattening, and Integrate forward ASE into the EDFA model Why Simulink?
Why use Simulink when an EDFA can be simulated using simulation tools such as OASIX or PTDS? Why use Simulink when an EDFA can be simulated using simulation tools such as OASIX or PTDS? - OASIX or PTDS
- Simulink
- dynamic model
- input pump power as well as other EDFA parameters can be easily modified
EDFA Gain characteristics Significant equations governing EDFA dynamics Output pump and signal power:
and are wavelength dependant as shown in the figure - and are the absorption and emission coefficients, respectively
this relationship is how the wavelength dependency of the gain arises EDFA gain ratio between the absorption and emission at a particular wavelength is critical in determining the gain
Note on Aspects of Simulation when performing simulations on the EDFA model it is important to simulate all the wavelengths simultaneously instead of one at a time EDFAs work in the nonlinear regime, so properties like linear superposition don’t hold true when there are several channels in an EDFA there is an effect called gain stealing - the energy that each of the channels takes from the pump depends on the details of the emission and absorption spectra
before simulating the gain, the optimum length was determined
Optimum Length
Simulink Models implementation of the ordinary nonlinear differential equation used for studying EDFA gain dynamics input/output
EDFA Gain
Gain Flattening using the equations shown earlier, I derived an equation relating the pump gain (GP) to the signal gain (GS) the resultant equation is:
for a GS of 30dB, GP should follow the curve shown in the figure theoretical view of what the pump should be practically, in order to get a different power at each wavelength might be difficult - something to be further analyzed
Thank You
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