Title | ||
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Calculation of Mutual Information for Partially Coherent Gaussian Channels With Applications to Fiber Optics |
Abstract | ||
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The mutual information between a complex-valued channel input and its complex-valued output is decomposed into four parts based on polar coordinates: an amplitude term, a phase term, and two mixed terms. Numerical results for the additive white Gaussian noise (AWGN) channel with various inputs show that, at high signal-to-noise ratio (SNR), the amplitude and phase terms dominate the mixed terms. For the AWGN channel with a Gaussian input, analytical expressions are derived for high SNR. The decomposition method is applied to partially coherent channels and a property of such channels called “spectral loss” is developed. Spectral loss occurs in nonlinear fiber-optic channels and it may be one effect that needs to be taken into account to explain the behavior of the capacity of nonlinear fiber-optic channels. |
Year | DOI | Venue |
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2011 | 10.1109/TIT.2011.2162187 | IEEE Transactions on Information Theory |
Keywords | Field | DocType |
index terms,amplitude term,mutual information,spectral loss,coherent channel,phase term,gaussian input,complex-valued channel input,awgn channel,mixed term,partially coherent gaussian channels,fiber optics,additive white gaussian noise,nonlinear fiber-optic channel,decomposition,channel capacity,decomposition method,polar coordinate,fiber optic,phase noise,signal to noise ratio,information theory | Statistical physics,Discrete mathematics,Nonlinear system,Telecommunications,Communication channel,Phase noise,Gaussian,Mutual information,Channel capacity,Additive white Gaussian noise,Amplitude,Mathematics | Journal |
Volume | Issue | ISSN |
57 | 9 | IEEE Trans. Information Theory 57 (2011) 5720-5736 |
Citations | PageRank | References |
5 | 0.53 | 12 |
Authors | ||
5 |
Name | Order | Citations | PageRank |
---|---|---|---|
B. Goebel | 1 | 5 | 0.53 |
R. Essiambre | 2 | 53 | 12.23 |
G. Kramer | 3 | 1053 | 77.88 |
P. J. Winzer | 4 | 20 | 7.80 |
Norbert Hanik | 5 | 55 | 14.82 |