首页> 外文期刊>Nuclear Physics, A: Journal Devoted to the Experimental Study of the Fundamental Constituents of Matter and Their Actions >Cooper pairs in the Borromean nuclei He-6 and Li-11 using continuum single particle level density
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Cooper pairs in the Borromean nuclei He-6 and Li-11 using continuum single particle level density

机译:库尔对在伯托基核He-6和Li-11中使用连续核单粒度密度

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摘要

A Borromean nucleus is a bound three-body system which is pairwise unbound because none of the two body subsystem interactions are strong enough to bind them in pairs. As a consequence, the single-particle spectrum of a neutron in the core of a Borromean nucleus is purely continuum, similarly to the spectrum of a free neutron, but two valence neutrons are bound up in such a core. Most of the usual approaches do not use the true continuum to solve the three-body problem but use a discrete basis, like for example, wave functions in a finite box. In this paper the proper continuum is used to solve the pairing Hamiltonian in the continuum spectrum of energy by using the single particle level density devoid of the free gas. It is shown that the density defined in this way modulates the pairing in the continuum. The partial-wave occupation probabilities for the Borromean nuclei He-6 and Li-11 are calculated as a function of the pairing strength. While at the threshold strength the (s1/2)(2) and (P3/2)(2) configurations are equally important in He-6, the (s1/2)(2) configuration is the main one in Li-11. For very small strength the (s1/2)(2) configuration becomes the dominant in both Borromean nuclei. At the physical strength, the calculated wave function amplitudes show a good agreement with other methods and experimental data which indicates that this simple model grasps the essence of the pairing in the continuum. (C) 2017 Elsevier B.V. All rights reserved.
机译:Borromean Nucleus是一个绑定的三体系,它是成对的未结合,因为两个身体子系统相互作用中都不是足够强的,以成对绑定它们。因此,伯莫核的核心中中子的单粒子光谱纯粹连续,与自由中子的光谱类似,但是在这种芯中束缚了两个价中子。大多数通常的方法都不使用真正的连续体来解决三体问题,但使用离散的基础,例如,在有限盒中的波函数。在本文中,采用适当的连续体通过使用无缺乏自由气体的单粒子水平密度来解决连续的能量频谱中的配对哈密顿。结果表明,以这种方式定义的密度调节连续体中的配对。 Borromean Nuclei He-6和Li-11的部分波占用概率作为配对强度的函数计算。虽然在阈值强度下(S1 / 2)和(2)和(P3 / 2)(2)配置在HE-6中同样重要,但(S1 / 2)(2)配置是LI-11中的主要一个。对于非常小的强度,(S1 / 2)(2)配置成为Borromean核中的主导。在物理强度下,计算的波函数幅度与其他方法和实验数据显示出良好的一致性,这表明这种简单的模型可以掌握连续体中配对的本质。 (c)2017年Elsevier B.V.保留所有权利。

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