Replacing the Soft FEC Limit Paradigm in the Design of Optical Communication Systems
Alex Alvarado, Erik Agrell, Domanic Lavery, Robert Maher, Polina Bayvel
TL;DR
The paper tackles the widespread SD-FEC limit design paradigm in optical communications and demonstrates that channel-independent FEC limits fail for soft-decision bit-wise decoding, especially at low code rates and with high-order modulations. It advocates the generalized mutual information (GMI) as a universal predictor of post-FEC BER, deriving achievable-rate bounds for memoryful and memoryless channels and showing that GMI, computed from bit-wise L-values, aligns with actual decoder performance across AWGN and nonlinear optical channels. Through extensive simulations (AWGN and NLSE) and experiments (64QAM WDM), the authors show that GMI consistently predicts post-FEC BER for both LDPC and turbo codes, while pre-FEC BER and ordinary MI can mislead across varying modulations and code rates. They propose replacing the traditional SD-FEC limit with a GMI-based limit, highlighting practical implications for spectral-efficiency estimates and system design in coherent optical networks, with caveats for iterative or nonbinary decoding scenarios.
Abstract
The FEC limit paradigm is the prevalent practice for designing optical communication systems to attain a certain bit-error rate (BER) without forward error correction (FEC). This practice assumes that there is an FEC code that will reduce the BER after decoding to the desired level. In this paper, we challenge this practice and show that the concept of a channel-independent FEC limit is invalid for soft-decision bit-wise decoding. It is shown that for low code rates and high order modulation formats, the use of the soft FEC limit paradigm can underestimate the spectral efficiencies by up to 20%. A better predictor for the BER after decoding is the generalized mutual information, which is shown to give consistent post-FEC BER predictions across different channel conditions and modulation formats. Extensive optical full-field simulations and experiments are carried out in both the linear and nonlinear transmission regimes to confirm the theoretical analysis.
