1996
DOI: 10.1103/physreva.54.4339
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Inverse scattering transform analysis of Stokes–anti-Stokes stimulated Raman scattering

Abstract: Zakharov-Shabat-Ablowitz-Kaup-Newel-Segur (ZS-AKNS) representation for Stokes-anti-Stokes stimulated Raman scattering (SRS) is proposed. Periodical waves, solitons and self-similarity solutions are derived. Transient and bright threshold solitons are discussed.

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Cited by 10 publications
(9 citation statements)
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“…The choice s 1 = −s 2 = −1 leads to the noncompact real form so(2, 3) and s 1 = s 2 = −1 gives another noncompact one-so (1,4). If in this last case we identify Q 01 = Q pol , Q 10 = −E s , Q 11 = E p and Q 12 = −E a then we obtain the system studied in [23] which describes Stockes-anti-Stockes wave generation. Here Q pol is the normalized effective polarization of the medium and E p , E s and E a are the normalized pump, Stockes and anti-Stockes wave amplitudes respectively.…”
Section: Real Forms Of Bmentioning
confidence: 99%
“…The choice s 1 = −s 2 = −1 leads to the noncompact real form so(2, 3) and s 1 = s 2 = −1 gives another noncompact one-so (1,4). If in this last case we identify Q 01 = Q pol , Q 10 = −E s , Q 11 = E p and Q 12 = −E a then we obtain the system studied in [23] which describes Stockes-anti-Stockes wave generation. Here Q pol is the normalized effective polarization of the medium and E p , E s and E a are the normalized pump, Stockes and anti-Stockes wave amplitudes respectively.…”
Section: Real Forms Of Bmentioning
confidence: 99%
“…then we obtain the system similar to that studied in [1,11] which describes Stokes-anti-Stokes wave generation. Here Q pol (x, t) is the normalized effective polarization of the medium and E p (x, t), E s (x, t) and E a (x, t) are the normalized pump, Stokes and anti-Stokes wave amplitudes respectively.…”
Section: Physical Applications Of 4-wave Equation With a Z 2 Reductionmentioning
confidence: 99%
“…It is described by the following Hamiltonian: In the case η = −1 if we identify q 10 = Q, q 11 = E p , q 21 = E a and q 1 = E s , where Q is the normalized effective polarization of the medium and E p , E s and E a are the normalized pump, Stokes and anti-Stokes wave amplitudes respectively, then we obtain the system of equations generalizing the one studied in [23] which describes Stokesanti-Stokes wave generation. This approach allowed us to derive a new Lax pair for (4.19).…”
Section: )mentioning
confidence: 99%
“…In the case when the reduction is of the type (2.1), i.e. p α = s α q * α then (6.21) is equivalent to 23) and can be interpreted as relations between the densities |q α | 2 of the 'particles' of type α. For the other types of reductions such interpretation is not so obvious.…”
Section: )mentioning
confidence: 99%