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引用次数: 0
摘要
非线性薛定谔方程在许多物理领域被用来描述波动过程[1-4],如量子力学、非线性光学、孤子理论、生物物理学。有许多不同的方法和数值算法来逼近非线性薛定谔方程[5]的解,从简单的在足够多的操作上给出满意的结果到复杂的。目前广泛应用的数学物理边值问题解[6-12]是原子函数理论(theory of atomic functions, AF)。该解表示为移位缩放AF族的和。泛函微分方程是无穷可微函数和泛函微分方程的解。它们处于样条函数、三角多项式和代数多项式之间的中间位置。它们比样条曲线平滑,但不如多项式平滑。在这项工作中,我们构造了构成薛定谔方程解的位移收缩函数。第一阶段考虑FDE的算子法[4]解。第二步,对由薛定谔方程生成的n个变量进行AF的建立。
A new construction of solution of Schrodinger equation on the basis of atomic functions
Nonlinear Schrodinger equation is used to describe wave processes in many areas of physics [1–4] such as quantum mechanics, nonlinear optics, theory of solitons, biophysics. There are many different methods and numerical algorithms to approximation solutions of nonlinear Schrodinger equations [5] from simple giving satisfactory results over a sufficiently large number of operations to complex. At present solutions of boundary value problems of mathematical physics [6–12] are widely used theory of atomic functions (AF). This solution is represent as a sum of shift-scaled AF families. AFs are infinitely differentiable functions and solutions of functional differential equations (FDE). They stay an intermediate position between the splines and trigonometric and algebraic polynomials. They are smoother than splines but less smooth than the polynomial. In this work we construct AFs shift-contraction of which constitutes the solution of Schrodinger equations. On the first stage the operator method [4] solution of FDE is considered. On the second step AF building of N-variables generated by the Schrodinger equation is carried out.