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弱束缚双中子晕核的普适性质。

Universal Properties of Weakly Bound Two-Neutron Halo Nuclei.

作者信息

Hongo Masaru, Son Dam Thanh

机构信息

Department of Physics, University of Illinois, Chicago, Illinois 60607, USA.

RIKEN iTHEMS, RIKEN, Wako 351-0198, Japan.

出版信息

Phys Rev Lett. 2022 May 27;128(21):212501. doi: 10.1103/PhysRevLett.128.212501.

DOI:10.1103/PhysRevLett.128.212501
PMID:35687428
Abstract

We construct an effective field theory of a two-neutron halo nucleus in the limit where the two-neutron separation energy B and the neutron-neutron two-body virtual energy ε_{n} are smaller than any other energy scale in the problem, but the scattering between the core and a single neutron is not fine-tuned, and the Efimov effect does not operate. The theory has one dimensionless coupling which formally runs to a Landau pole in the ultraviolet. We show that many properties of the system are universal in the double fine-tuning limit. The ratio of the mean-square matter radius and charge radius is found to be ⟨r_{m}^{2}⟩/⟨r_{c}^{2}⟩=Af(ε_{n}/B), where A is the mass number of the core and f is a function of the ratio ε_{n}/B which we find explicitly. In particular, when B≫ε_{n}, ⟨r_{m}^{2}⟩/⟨r_{c}^{2}⟩=2/3A. The shape of the E1 dipole strength function also depends only on the ratio ε_{n}/B and is derived in explicit analytic form. We estimate that for the ^{22}C nucleus higher-order corrections to our theory are of the order of 20% or less if the two-neutron separation energy is less than 100 keV and the s-wave scattering length between a neutron and a ^{20}C nucleus is less than 2.8 fm.

摘要

我们构建了一个双中子晕核的有效场论,该理论适用于双中子分离能(B)和中子 - 中子两体虚能(\varepsilon_{n})小于问题中任何其他能量尺度的极限情况,但核心与单个中子之间的散射未进行微调,且埃菲莫夫效应不发生作用。该理论有一个无量纲耦合,在紫外区域形式上会趋于朗道极点。我们表明,在双重微调极限下,系统的许多性质是普遍的。发现均方物质半径与电荷半径之比为(\langle r_{m}^{2}\rangle /\langle r_{c}^{2}\rangle = Af(\varepsilon_{n}/B)),其中(A)是核心的质量数,(f)是(\varepsilon_{n}/B)比值的函数,我们已明确求出该函数。特别地,当(B\gg\varepsilon_{n})时,(\langle r_{m}^{2}\rangle /\langle r_{c}^{2}\rangle = 2/3A)。电偶极强度函数的形状也仅取决于(\varepsilon_{n}/B)的比值,并以显式解析形式导出。我们估计,对于(^{22}C)核,如果双中子分离能小于(100)keV且中子与(^{20}C)核之间的(s)波散射长度小于(2.8)fm,我们理论的高阶修正量级为(20%)或更小。

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