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arXiv 1107.3281math.APmath-phmath.MP
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非线性薛定谔方程的非线性阻尼延拓--数值研究

Nonlinear-damping continuation of the nonlinear Schrödinger equation - a numerical study

G. Fibich, M. Klein

摘要:

研究了临界和超临界NLS的奇异解的非线性阻尼延拓。我们的模拟结果表明,对于一般的初始条件,导致崩溃的无阻尼NLS,弱阻尼NLS的解决方案$$ iψ_t(t,\X)+Δψ+|ψ|^{p-1}ψ+iδ|ψ|^{q-1}ψ=0,\qquad0<δ\ll 1, $$是高度不对称的奇异时间,和崩溃后的散焦速度的奇异核心趋于无穷大的阻尼系数$δ$趋于零。在临界NLS的最小幂次爆破解的特殊情况下,延拓是具有较高(但有限)散焦速度的最小幂次解,其幅度随非线性阻尼指数$q$单调增加。

英文摘要:

We study the nonlinear-damping continuation of singular solutions of the critical and supercritical NLS. Our simulations suggest that for generic initial conditions that lead to collapse in the undamped NLS, the solution of the weakly-damped NLS $$ iψ_t(t,\X)+Δψ+|ψ|^{p-1}ψ+iδ|ψ|^{q-1}ψ=0,\qquad0<δ\ll 1, $$ is highly asymmetric with respect to the singularity time, and the post-collapse defocusing velocity of the singular core goes to infinity as the damping coefficient $δ$ goes to zero. In the special case of the minimal-power blowup solutions of the critical NLS, the continuation is a minimal-power solution with a higher (but finite) defocusing velocity, whose magnitude increases monotonically with the nonlinear damping exponent $q$.

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