Abstract:The Kaup-Newell (KN) hierarchy contains the derivative nonlinear Schrödinger equation (DNLSE) amongst others interesting and important nonlinear integrable equations. In this paper, a general higher grading affine algebraic construction of integrable hierarchies is proposed and the KN hierarchy is established in terms of aŝ 2 Kac-Moody algebra and principal gradation. In this form, our spectral problem is linear in the spectral parameter. The positive and negative flows are derived, showing that some interesti… Show more
“…we reproduce results of [4,6,7,17] on the relationship between the DNLSH and the massive Thirring model [8,11,14,16].…”
Section: Example 5: Massive Thirring Modelsupporting
confidence: 53%
“…The most straightforward continuation of this work is to use the advantages of the functional representation and to derive other classes of explicit solutions which complement the bright-soliton solutions derived in [4] and dark solitons presented above. This can be done starting from the bilinear equations of proposition 7.1 which can be associated with the Fay identities for the thetafunctions and used to derive the quasiperiodic solutions, or with various determinant identities that lead to Wronskian, Toeplitz and other solutions.…”
Section: Discussionmentioning
confidence: 99%
“…Consequently, we use the term DNLSH for the hierarchy whose simplest equations are (1.2) (see the recent paper [4] on the negative flows of the Kaup-Newell hierarchy).…”
This paper is devoted to the negative flows of the derivative nonlinear Schrödinger hierarchy (DNLSH). The main result of this work is the functional representation of the extended DNLSH, composed of both positive (classical) and negative flows. We derive a finite set of functional equations, constructed by means of the Miwa's shifts, which contains all equations of the hierarchy. Using the obtained functional representation we convert the nonlocal equations of the negative subhierarchy into local ones of higher order, derive the generating function of the conservation laws and the N-soliton solutions for the extended DNLSH under non-vanishing boundary conditions.
“…we reproduce results of [4,6,7,17] on the relationship between the DNLSH and the massive Thirring model [8,11,14,16].…”
Section: Example 5: Massive Thirring Modelsupporting
confidence: 53%
“…The most straightforward continuation of this work is to use the advantages of the functional representation and to derive other classes of explicit solutions which complement the bright-soliton solutions derived in [4] and dark solitons presented above. This can be done starting from the bilinear equations of proposition 7.1 which can be associated with the Fay identities for the thetafunctions and used to derive the quasiperiodic solutions, or with various determinant identities that lead to Wronskian, Toeplitz and other solutions.…”
Section: Discussionmentioning
confidence: 99%
“…Consequently, we use the term DNLSH for the hierarchy whose simplest equations are (1.2) (see the recent paper [4] on the negative flows of the Kaup-Newell hierarchy).…”
This paper is devoted to the negative flows of the derivative nonlinear Schrödinger hierarchy (DNLSH). The main result of this work is the functional representation of the extended DNLSH, composed of both positive (classical) and negative flows. We derive a finite set of functional equations, constructed by means of the Miwa's shifts, which contains all equations of the hierarchy. Using the obtained functional representation we convert the nonlocal equations of the negative subhierarchy into local ones of higher order, derive the generating function of the conservation laws and the N-soliton solutions for the extended DNLSH under non-vanishing boundary conditions.
“…Eq. (1.6) also can be derived from the generalized KN hierarchy [15] under n = 3 and proper parameter. Second, when β = 1 4 and x → ix, t → it, r = −q * the system (1.5) become…”
Due to higher-order Kaup-Newell (KN) system has more complex and diverse solutions than classical second-order flow KN system, the research on it has attracted more and more attention. In this paper, we consider a higher-order KN equation with third order dispersion and quintic nonlinearity. Based on the theory of the inverse scattering, the matrix Riemann-Hilbert problem is established. Through the dressing method, the solution matrix with simple zeros without reflection is constructed. In particular, a new form of solution is given, which is more direct and simpler than previous methods. In addition, through the determinant solution matrix, the vivid diagrams and dynamic analysis of single soliton solution and two soliton solution are given in detail. Finally, by using the technique of limit, we construct the general solution matrix in the case of multiple zeros, and the examples of solutions for the cases of double zeros, triple zeros, single-double zeros and double-double zeros are especially shown.
“…The inverse scattering transform for the MT model was studied by Kuznetsov and Mikhailov [4] and many others [5,6,7,8,9]. The Darboux transformation, Bäcklund transformation of the MT model and its connection with other integrable systems have been investigated by Kaup and Newell [10], Lee [11,12], Prikarpatskii [13,14] , Franca et al [15] and Degasperis [16].…”
In the present paper, we are concerned with the tau function and its connection with the Kadomtsev-Petviashvili (KP) theory for the massive Thirring (MT) model. First, we bilinearize the massive Thirring model under both the vanishing and nonvanishing boundary conditions. Starting from a set of bilinear equations of two-component KP-Toda hierarchy, we derive the multi-bright solution to the MT model by the KP hierarchy reductions. Then, we show that the discrete KP equation can generate a set of bilinear equations of a deformed KP-Toda hierarchy through Miwa transformation. By imposing constraints on the parameters of the tau function, the general dark soliton solution to the MT model is constructed from the tau function of the discrete KP equation. Finally, the dynamics and properties of oneand two-soliton for both the bright and dark cases are analyzed in details.
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