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arXiv math-ph/0101015math-phcs.NAmath.MPmath.NA
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广义Rayleigh-Schroedinger微扰理论作为所谓准精确可解模型线性化方法

Generalized Rayleigh-Schroedinger perturbation theory as a method of linearization of the so called quasi-exactly solvable models

Miloslav Znojil

AI总结:

针对D维六次谐振子这一典型准精确可解模型,提出一种与N无关的线性方法,通过1/√D幂级数展开,在前两阶实现所有QES态的精确可解性,并给出整数运算的显式矩阵公式。

摘要:

考虑D维六次谐振子作为典型的准精确可解(QES)模型。通常,其QES N重束缚态必须使用耦合的Magyari非线性代数方程计算。我们提出并描述了一种替代的线性方法,该方法与N无关,并使用1/√D的幂级数展开。主要优点:在前两阶(简并完全消除,未微扰谱等距)同时实现精确可解性(对所有QES态)。附加优点:所有微扰修正由整数运算中的显式矩阵公式给出(没有舍入误差)。

英文摘要:

Sextic oscillator in D dimensions is considered as a typical quasi-exactly solvable (QES) model. Usually, its QES N-plets of bound states have to be computed using the coupled Magyari's nonlinear algebraic equations. We propose and describe an alternative linear method which is N-independent and works with power series in 1/\sqrt(D). Main merit: simultaneous exact solvability (for all the QES states) in the first two leading orders (the degeneracy is completely removed, the unperturbed spectrum is equidistant). An additional merit: All the perturbation corrections are given by explicit matrix formulae in integer arithmetics (there are no rounding errors).

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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