期刊
PHYSICS LETTERS A
卷 357, 期 3, 页码 196-203出版社
ELSEVIER
DOI: 10.1016/j.physleta.2006.04.032
关键词
GNLS(m, n, p, q) equation; nonlinear dispersion; linear dispersion; envelope compactons; envelope solitary patterns; conservation laws
In this Letter, to further understand the role of nonlinear dispersion in the generalized nonlinear Schrodinger equation, we introduce and study the generalized nonlinear Schrodinger equation with nonlinear dispersion (called GNLS(m, n, p, q) equation): iu(t) + a(u vertical bar u vertical bar(n-1))(xx) +bu vertical bar u vertical bar(m-1) + ic(u vertical bar u vertical bar(p-1))(xxx) +id(u vertical bar u vertical bar(q-1))(x) = 0. Some new envelope compacton solutions and solitary pattern solutions of GNLS(m, n, p, q) equation are obtained via the gauge transformation and some direct ansatze. In particular, it is shown that GNLS (m, n, p, q) equation with linear dispersion gives rise to envelope compactons and solitary patterns, which implies that nonlinear dispersion is not necessary condition for GNLS(m, n, p, q) equation to admit envelope compactons and solitary patterns. Moreover, some unusually local conservation laws are presented for GNLS(+)(n, n, n, n) equation and GNLS(-) (n, n, n, n) equation, respectively. (c) 2006 Elsevier B.V. All rights reserved.
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