2017
DOI: 10.1016/j.aml.2017.02.002
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Novel higher-order rational solitons and dynamics of the defocusing integrable nonlocal nonlinear Schrödinger equation via the determinants

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Cited by 45 publications
(26 citation statements)
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“…With the increase of the interaction strength, the central region of the cross‐shaped RW creates two sharp peaks at t3/4. The cross‐shaped RW is separated into two hyperbolic line RWs at t0, whose behavior is similar to that of the rational‐soliton in the (1+1)‐dimensional system 88,89 ; then they merge back into the constant background, the strong interaction resulting in the change of the waveform. We stress that the dynamical behavior of the higher order line RWs of nonlocal Maccari system () is different from that of the corresponding higher order line RWs in other nonlocal systems, such as the nonlocal two‐dimensional NLS equation 48,90 and nonlocal DS equation 31,70 .…”
Section: General Line Rws On Top Of the Periodic Line‐wave Backgroundmentioning
confidence: 96%
“…With the increase of the interaction strength, the central region of the cross‐shaped RW creates two sharp peaks at t3/4. The cross‐shaped RW is separated into two hyperbolic line RWs at t0, whose behavior is similar to that of the rational‐soliton in the (1+1)‐dimensional system 88,89 ; then they merge back into the constant background, the strong interaction resulting in the change of the waveform. We stress that the dynamical behavior of the higher order line RWs of nonlocal Maccari system () is different from that of the corresponding higher order line RWs in other nonlocal systems, such as the nonlocal two‐dimensional NLS equation 48,90 and nonlocal DS equation 31,70 .…”
Section: General Line Rws On Top Of the Periodic Line‐wave Backgroundmentioning
confidence: 96%
“…In this section, we will establish the determinant representation of the N -fold DT for Eq.(2). The spectral problem (6) can transform to Ψ [2] x = U [2] Ψ [2] , Ψ…”
Section: N -Fold Dt Of Reverse-space-time Dnls Equationmentioning
confidence: 99%
“…Nonlinear evolution equations play an important role and their solutions have been a hot research spot, including soliton [1,2,3,4], breather [5,6,7], rogue wave [8,9,10,11] and others [12,13,14,15]. The derivative nonlinear Schrödinger equation (DNLS) [16,17,18,19] iq t − q xx + i(q 2 q * ) x = 0, (…”
Section: Introductionmentioning
confidence: 99%
“…In this subsection, we use the generalized DT [19,[40][41][42]48,49] to derive dark-bright mixed highorder soliton solutions for equation (1.3). Let the spectral parameter λ = λ 1 + , where is a small parameter and (−2 Im(λ 1 )/Im(μ…”
Section: (C) Dark-bright Mixed High-order Soliton Solutionsmentioning
confidence: 99%
“…A natural problem is that how to use the Darboux transformation (DT) to analyse the soliton and breather structures from the viewpoint of the spectral parameter in the Lax pair in detail. Recently, the DT has been extended to derive multi-bright-bright and multi-dark-dark solitons for the nCNLS equations [39], high-order rational solitons [40][41][42] of the non-local NLS equation and its two-component case [43,44], and the dark-dark multi-solitons of the defocusing AB system [45]. To the best of our knowledge, the dark-bright mixed solitons and breathers, as well as their semi-rational extensions for the nCNLS equations (1.3) were not studied by the DT before.…”
Section: Introductionmentioning
confidence: 99%