Spin-Dipole Strengths and Neutron Skin Thickness of \({}^{{90}}\)Zr, \({}^{{132}}\)Sn, \({}^{{208}}\)Pb

IF 0.3 4区 物理与天体物理 Q4 PHYSICS, NUCLEAR Physics of Atomic Nuclei Pub Date : 2024-09-02 DOI:10.1134/S1063778824700480
I. N. Borzov, S. V. Tolokonnikov
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Abstract

The strength distributions of charge exchange spin-dipole excitations are calculated in the continuum quasiparticle random-phase approximation based on the Fayans density functional with modified isovector part. An impact of the isovector parameter \(h_{2}^{-}\) of the DF3-f functional on the strength functions of charge-exchange spin-dipole excitations (\(0^{-}\), \(1^{-}\), \(2^{-}\)) are studied for \({}^{208}\)Pb, \({}^{132}\)Sn and \({}^{90}\)Zr. The sum rules are calculated using both ground state radii and direct integration of the total SD strength distributions. A comparison with the experimental SD sum rule in \({}^{90}\)Zr gives one a possibility to check previously estimated \(h_{2}^{-}\) values which described well the recent combined estimate for \(\Delta R_{np}\) in \({}^{208}\)Pb and corresponding equation of state parameters – symmetry energy \(J_{0}=J(\rho_{0})\) and a slope parameter \(L_{0}=L(\rho_{0})\).

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{${}^{90}}$锆、{${}^{132}}$锡和{${}^{208}}$铅的自旋偶极子强度和中子皮厚
摘要 在连续体准粒子随机相近似中,计算了电荷交换自旋-偶极子激发的强度分布,计算基于修正了等矢量部分的Fayans密度函数。研究了DF3-f函数的等矢量参数(h_{2}^{-}/\)对电荷交换自旋偶极子激发强度函数(\(0^{-}/\)、\(1^{-}/\)、\(2^{-}/\))的影响,适用于({}^{208}/)Pb、({}^{132}/)Sn和({}^{90}/)Zr。总和规则的计算同时使用了基态半径和总自毁强度分布的直接积分。与 \({}^{90}\)Zr 中的实验自旋和规则的比较使我们有可能检查先前估计的 \(h_{2}^{-) 值。和相应的状态方程参数--对称能(J_{0}=J(\rho_{0}))和斜率参数(L_{0}=L(\rho_{0}))。
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来源期刊
Physics of Atomic Nuclei
Physics of Atomic Nuclei 物理-物理:核物理
CiteScore
0.60
自引率
25.00%
发文量
56
审稿时长
3-6 weeks
期刊介绍: Physics of Atomic Nuclei is a journal that covers experimental and theoretical studies of nuclear physics: nuclear structure, spectra, and properties; radiation, fission, and nuclear reactions induced by photons, leptons, hadrons, and nuclei; fundamental interactions and symmetries; hadrons (with light, strange, charm, and bottom quarks); particle collisions at high and superhigh energies; gauge and unified quantum field theories, quark models, supersymmetry and supergravity, astrophysics and cosmology.
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