Discrete and continuous nonlinear Schroedinger systems - download pdf or read online

By M. J. Ablowitz, B. Prinari, A. D. Trubatch

ISBN-10: 0521534372

ISBN-13: 9780521534376

Over the last thirty years major growth has been made within the research of nonlinear waves--including "soliton equations", a category of nonlinear wave equations that come up usually in such parts as nonlinear optics, fluid dynamics, and statistical physics. The huge curiosity during this box could be traced to figuring out "solitons" and the linked improvement of a style of resolution termed the inverse scattering rework (IST). The IST procedure applies to non-stop and discrete nonlinear Schrödinger (NLS) equations of scalar and vector sort. This paintings provides an in depth mathematical learn of the scattering concept, deals soliton strategies, and analyzes either scalar and vector soliton interactions. The authors supply complicated scholars and researchers with an intensive and self-contained presentation of the IST as utilized to nonlinear Schrödinger platforms.

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These formulas also yield δF = −i {F, r (x)} , δq(x) δF = −i {F, q(x)} . 112b) ∂t where {, } denotes the Poisson brackets. 112b) are called Hamilton’s equations of motion, and the variables ( p, q) are called conjugates. 114a) {q(x, t), q(y, t)} = {r (x, t), r (y, t)} = 0. 104b). In the case when the initial data satisfy the additional symmetry r = ∓q ∗ , we identify coordinates q(x, t), momenta q ∗ (x, t). 116) {q(x, t), q(y, t)} = q ∗ (x, t), q ∗ (y, t) = 0. 1 Overview In general, any given discretization of an integrable PDE is most likely to be nonintegrable.

6). 77). 81) as x → +∞, one obtains ¯ =0 ∂t a(k) ∂t a(k) = 0, ∂t b(k) = −2A∞ b(k), ¯ ¯ = 2A∞ b(k) ∂t b(k) or, explicitly, a(k, t) = a(k, 0), b(k, t) = e −4ik 2 t ¯ t) = a(k, ¯ 0) a(k, ¯ 0). , the zeros of a(k) and a(k)) are constant as the solution evolves. Not only the number of eigenvalues, but also their locations, are fixed. Thus, the eigenvalues are time-independent discrete states of the evolution. 1) and in integrable soliton equations in general. 83) and this also gives the evolution of the norming constants: C j (t) = C j (0)e−4ik j t , 2 ¯2 C¯ j (t) = C¯ j (0)e4i k j t .

32]; Bobenko et al. [33, 34]; Boiti et al. [35– 37]; Bruschi et al. [42, 43, 45]; Case et al. [48, 49]; Chiu and Ladik [53]; Common [56]; Doliwa and Santini [66, 67]; Gerdjikov et al. [86]; Herbst and Weideman [93]; Hirota [94–96]; Kac and van Moerbeke [98, 99]; Konotop et al. [109, 111]; Nihoff and Capel [139]; Orfanidis [141]; Ramani et al. [143]; Suris [156–160]; Taha and Ablowitz [161–164]; Tsuchida et al. [168–172]; Vakhnenenko et al. [173]; Vekslerchik [175, 176] ; Veselov and Shabat [177] 48 3 Integrable discrete nonlinear Schr¨odinger equation and references therein) for related studies involving discrete integrable systems from various perspectives.

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Discrete and continuous nonlinear Schroedinger systems by M. J. Ablowitz, B. Prinari, A. D. Trubatch


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