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Polarization-multiplexed nonlinear inverse synthesis with standard and reduced-complexity NFT processing: erratum

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Abstract

We correct a formula for the numerical nonlinear Fourier transform in [1]. The conclusions of our work are unchanged.

© 2019 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

In Section 3.1 of [1] the single-step transfer matrix U(n), Eq. (20) and its derivative Eq. (25) are not correct. The transfer matrix—obtained via eigenvalue decomposition—should be

Um,l(n)={c0jλs0m=l=1,ql1(n)s0m=1andl2,σqm1(n)*s0m2andl=1,rm1,l1[c0+jλs0ejλδ]m=2andl3orl=2andm3,rm1,l1[c0+jλs0]+ejλδ(1rm1,m1)m=l=2orm,l3,
where rml=qm(n)*ql(n)/k=1M|qk(n)|2. The derivative U(n) follows from (1). Equation (20) in [1], though not exact, is a first order approximation of (1). The use of Eq. (20) in [1] rather than (1) yields different performance at higher powers and oversampling factors, see Figs. 1(a) and 1(b) for M = 2. However, since the oversampling factor in [1] is ND=NI=4, both matrices can be used without any variation. We verified that the performance metrics showed in [1] in Figs. 3(a) and 3(b) are unaffected when the new matrix (1) is used for the signal processing.

 figure: Fig. 1

Fig. 1 NMSE—Eq. (37) of [1]—versus oversampling factor ND, with NI = 16 and Ns = 8.

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References

1. S. Civelli, S. Turitsyn, M. Secondini, and J. Prilepsky, “Polarization-multiplexed nonlinear inverse synthesis with standard and reduced-complexity NFT processing,” Opt. Express 26, 17360–17377 (2018). [CrossRef]  

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Figures (1)

Fig. 1
Fig. 1 NMSE—Eq. (37) of [1]—versus oversampling factor ND, with NI = 16 and Ns = 8.

Equations (1)

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U m , l ( n ) = { c 0 j λ s 0 m = l = 1 , q l 1 ( n ) s 0 m = 1 and l 2 , σ q m 1 ( n ) * s 0 m 2 and l = 1 , r m 1 , l 1 [ c 0 + j λ s 0 e j λ δ ] m = 2 and l 3 or l = 2 and m 3 , r m 1 , l 1 [ c 0 + j λ s 0 ] + e j λ δ ( 1 r m 1 , m 1 ) m = l = 2 or m , l 3 ,
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