解释有限温度准粒子随机相位近似

IF 2.6 3区 物理与天体物理 Q2 PHYSICS, NUCLEAR
A. Ravlić, E. M. Ney, J. Engel, N. Paar
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引用次数: 0

摘要

在许多天体物理场景中,如核心坍缩超新星和中子星合并,以及重离子碰撞实验中,热填充核激发态之间的转变已被证明起着重要作用。有限温度准粒子随机相近似(FT-QRPA)由于其简单和可外推性,是研究热核性质的一种有效方法。FT-QRPA中的统计系综使理论比零温度理论丰富得多,但也模糊了各种物理量的含义。在这项工作中,我们阐明了FT-QRPA的几个方面,包括文献中看到的符号,并演示了如何从理论中提取物理量。为了说明有限温度跃迁的正确处理方法,我们特别强调了质子-中子FT-QRPA (FT-PNQRPA)描述的电荷交换跃迁。利用建立在核能密度泛函理论基础上的FT-PNQRPA,我们得到了相对论矩阵法和非相对论有限振幅法的解。我们证明了对热填充激发态的去激发的适当处理可以使池田和规则得到满足。此外,我们证明了这些转变对\( ^{58,78}\) Ni中恒星电子捕获(EC)速率的影响。虽然它们的加入不影响\( ^{58}\) Ni中的EC速率,但\( ^{78}\) Ni中的EC速率主要是在\(T > 0.5\) MeV温度下的去激发。在具有较大负q值的系统中,在FT-QRPA中包含去激发对于完整描述有限温度下的反应速率是必要的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Elucidating the finite temperature quasiparticle random phase approximation

In many astrophysical scenarios, such as core-collapse supernovae and neutron star mergers, as in well as heavy-ion collision experiments, transitions between thermally populated nuclear excited states have been shown to play an important role. Because of its simplicity and ability to extrapolate, the finite-temperature quasiparticle random phase approximation (FT-QRPA) is an efficient method for studying the properties of hot nuclei. The statistical ensembles in the FT-QRPA make the theory much richer than its zero-temperature counterpart, but also obscure the meaning of various physical quantities. In this work, we clarify several aspects of the FT-QRPA, including notation seen in the literature, and demonstrate how to extract physical quantities from the theory. To illustrate the correct treatment of finite-temperature transitions, we place special emphasis on the charge-exchange transitions described by the proton-neutron FT-QRPA (FT-PNQRPA). With the FT-PNQRPA built on the nuclear energy-density functional theory, we obtain solutions in a relativistic matrix approach and also in the non-relativistic finite amplitude method. We show that the proper treatment of de-excitations from thermally populated excited states causes the Ikeda sum rule to be fulfilled. In addition, we demonstrate the impact of these transitions on stellar electron capture (EC) rates in \( ^{58,78}\)Ni. While their inclusion does not affect the EC rates in \( ^{58}\)Ni, the rates in \( ^{78}\)Ni are dominated by de-excitations for temperatures \(T > 0.5\) MeV. In systems with a large negative Q-value, the inclusion of de-excitations within the FT-QRPA is necessary for a complete description of reaction rates at finite temperature.

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来源期刊
The European Physical Journal A
The European Physical Journal A 物理-物理:核物理
CiteScore
5.00
自引率
18.50%
发文量
216
审稿时长
3-8 weeks
期刊介绍: Hadron Physics Hadron Structure Hadron Spectroscopy Hadronic and Electroweak Interactions of Hadrons Nonperturbative Approaches to QCD Phenomenological Approaches to Hadron Physics Nuclear and Quark Matter Heavy-Ion Collisions Phase Diagram of the Strong Interaction Hard Probes Quark-Gluon Plasma and Hadronic Matter Relativistic Transport and Hydrodynamics Compact Stars Nuclear Physics Nuclear Structure and Reactions Few-Body Systems Radioactive Beams Electroweak Interactions Nuclear Astrophysics Article Categories Letters (Open Access) Regular Articles New Tools and Techniques Reviews.
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