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Structure of positive energy states in a deformed mean-field potential

机译:变形平均场势中正能量状态的结构

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We investigate the properties of single-particle resonances in a non-spherical potential by solving the coupled-channels equations for the radial wave functions. We first generalize the box discretization method for positive energy states to a deformed system. As in the spherical case, we find that the discretized energy is stabilized against the box size when a resonance condition is met. Using the wave functions thus obtained, we then discuss the energy and the radial dependences of scattering wave functions in the vicinity of an isolated resonance. In the eigenchannel basis, where the S-matrix is diagonal, we propose a generalized expression for the factorization formula for the multi-channel wave function. We find that the factorized wave function agrees well with the exact solution inside the centrifugal barrier when the energy distance from the resonance is less than the resonance width. (C) 2004 Elsevier B.V. All rights reserved.
机译:我们通过求解径向波函数的耦合通道方程来研究非球形势中单粒子共振的性质。我们首先将正能量状态的盒离散方法推广到变形系统。与球形情况一样,我们发现当满足共振条件时,离散能量相对于盒子尺寸稳定。使用由此获得的波函数,我们然后讨论在孤立共振附近的能量和散射波函数的径向相关性。在S矩阵为对角线的本征通道基础上,我们为多通道波动函数的分解公式提出了一个广义表达式。我们发现,当距共振的能量距离小于共振宽度时,分解波函数与离心屏障内部的精确解非常吻合。 (C)2004 Elsevier B.V.保留所有权利。

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