D=0.1 , D=2.5. Movies of individual runs for Model A (deterministic part of the dispersion coefficient is positive constant) for the absolute value of the signal as a function of the retarded time. The movie counter runs with the distance, upto z=95. The retarded time domain is limited by 1/20 of the periodic cell size. Click here D=0.1 , D=2.5 to see the full domain (in time) version of the movie run upto z=50; and here D=0.1, D=2.5 to check the respective dispersion maps profile.

D=0.1, D=2.5. Movies of individual runs for Model B (dispersion managment case) for the absolute value of the signal as a function of the retarded time. The movie counter runs with the distance, upto z=95. The retarded time domain is limited by 1/20 of the periodic cell size. Click here D=0.1 , D=2.5 to see the full domain (in time) version of the movie run upto z=50; and here D=0.1, D=2.5 to check the respective dispersion maps profile.

 Model A. The set of supplementary Figures for
avearged peak amplitude of the pulse D=0.1 , D=2.5 ;
averaged pulse width measured at the half-of-the-peak-amplitude D=0.1 , D=2.5 ;
averaged pulse width measured at the quarter-of-the-peak-amplitude D=0.1 , D=2.5 ;
Average pulse shape at z=95 D=0.1 , D=2.5 ;
PDF of the peak amplitude of the pulse at z=95 D=0.1 , D=2.5 ;
PDF of pulse width measured at the half-of-the-peak-amplitude at z=95 D=0.1, D=2.5;
PDF of pulse width measured at the quarter-of-the-peak-amplitude at z=95 D=0.1 , D=2.5 ;

Model B. The set of supplementary Figures for
avearged peak amplitude of the pulse D=0.1 , D=2.5 ;
averaged pulse width measured at the half-of-the-peak-amplitude D=0.1, D=2.5 ;
averaged pulse width measured at the quarter-of-the-peak-amplitude D=0.1 , D=2.5 ;
Average pulse shape at z=95 D=0.1 , D=2.5 ;
PDF of the peak amplitude of the pulse at z=95 D=0.1 , D=2.5 ;
PDF of pulse width measured at the half-of-the-peak-amplitude at z=95 D=0.1 , D=2.5 ;
PDF of pulse width measured at the quarter-of-the-peak-amplitude at z=95 D=0.1 , D=2.5 ;
PDF of the pulse amplitude additionally averaged over z from [30,95] for =1: D=0.1 , D=2.5 ;
PDF of the the width measured at the half-of-the-peak-amplitude additionally averaged over z from [30,95] for  l=1: D=0.1 , D=2.5 ;
PDF of the the width measured at the quarter-of-the-peak-amplitude additionally averaged over z from [30,95] for  l=1: D=0.1 , D=2.5 .