1989
DOI: 10.1070/qe1989v019n09abeh009130
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Optimal self-compression of multisoliton pulses in an optical fiber

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Cited by 59 publications
(90 citation statements)
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“…(1) reduces to the standard NLS equation (2). Several localized and periodic structures of standard NLS are documented in the literature [21,46,47]. Equation (2) admits N th order RW solution.…”
Section: Appendix Amentioning
confidence: 99%
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“…(1) reduces to the standard NLS equation (2). Several localized and periodic structures of standard NLS are documented in the literature [21,46,47]. Equation (2) admits N th order RW solution.…”
Section: Appendix Amentioning
confidence: 99%
“…To begin with we consider the first-order breather solution of the NLS equation (2), which is given in [46] and is a special case of the GB solution (4), where the parameters f and v are expressed in terms of a complex eigenvalue (say λ), that is f = 2 √ 1 + λ 2 and v = Im(λ), and X 1 and T 1 serve as coordinate shifts from the origin. The real part of the eigenvalue represents the angle that the one-dimensionally localized solutions form with the T axis, and the imaginary part characterizes frequency of periodic modulation.…”
Section: Characteristics Of Breathersmentioning
confidence: 99%
“…(6) cannot be found analytically, but it is possible to find them numerically. 12,14 Analytically we can find only the points of bifurcation at which these states split off from the polarized ones.…”
Section: (10)mentioning
confidence: 99%
“…The phases of the two components are locked in the following composite (nonpolarized) solitonstate solutions 12,13 …”
mentioning
confidence: 99%
“…In this model the discrete spectrum solutions, interacting with condensate, transform from solitons to the oscillating structures -breathers. The family of NLSE breathers includes the well known solutions of Pere-grine [12], Kuznetsov-Ma [10,11] and Akhmediev [13].…”
Section: Introductionmentioning
confidence: 99%