Stability and Instability Results for Standing Waves of Quasi-linear Schrödinger Equations
نویسنده
چکیده
iφt +∆φ+ φl ′ (|φ|2)∆l(|φ|2) + f(|φ|2)φ = 0 in (0,∞)× R , φ(0, x) = a0(x) in R N , where l and f are given functions. Here i is the imaginary unit, N ≥ 1, φ : R → C is a complex valued function. For example, the particular case l(s) = √ 1 + s models the self-channeling of a high-power ultra short laser in matter (see [6, 13, 36]) whereas if l(s) = √ s, equation (1.1) appears in dissipative quantum mechanics ([16]). It is also used in plasma physics and fluid mechanics ([14, 28]), in the theory of Heisenberg ferromagnets and magnons ([2]) and in condensed matter theory ([32]). The dynamical features are closely related to the two functions l and f . Only few intents
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تاریخ انتشار 2009