1984
DOI: 10.1016/0375-9601(84)90827-2
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General N-soliton solution of the AKNS class on arbitrary background

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Cited by 194 publications
(122 citation statements)
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“…4.2], [36], [41]) one introduces the quantities ϕ k (x) = ψ 2,− (z k , x) + γ k ψ 2,+ (z k , x) ψ 1,− (z k , x) + γ k ψ 1,+ (z k , x) , …”
Section: Transformation Operators For J -Self-adjoint Dirac-type Operunclassified
“…4.2], [36], [41]) one introduces the quantities ϕ k (x) = ψ 2,− (z k , x) + γ k ψ 2,+ (z k , x) ψ 1,− (z k , x) + γ k ψ 1,+ (z k , x) , …”
Section: Transformation Operators For J -Self-adjoint Dirac-type Operunclassified
“…, Q 2N expressed in the similar way. Our method is closely related to the Neugebauer-Meinel approach [3]. Let D is given by (38).…”
Section: The Multi-soliton Darboux Matrixmentioning
confidence: 99%
“…There are several methods to construct the Darboux matrix (which generates soliton solutions) [1,2,3,4,6,5,7,8]). However, these methods are technically difficult when applied to the matrix versions of the spectral problems which are naturally represented in Clifford algebras [9,10,12].…”
Section: Introductionmentioning
confidence: 99%
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“…Through solving the relevant linear system with a given seed solution, with no need to refer to the special boundary conditions, a series of new analytical solutions can be generated under the Darboux transformation. By performing the iterative algorithm of the Darboux transformation successively, one can obtain the n-times iterated potential transformation formula in terms of the Wronskian determinant [22] or Vandermonde-like determinant [26]. This paper is devoted to applying the Darboux transformation method to System (3) based on the Lax pair derived from the matrix AKNS scheme.…”
Section: Introductionmentioning
confidence: 99%