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arXiv 1606.00407nucl-thnucl-ex
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核密度泛函超平均场论的研究进展

State-of-the-art of beyond mean field theories with nuclear density functionals

J. Luis Egido

摘要:

本文综述了基于生成坐标方法的超平均场论(BMFT)和在有效力核物理中的对称性恢复。在回顾了Hartree-Fock-Bogoliubov(HFB)理论之后,讨论了任何平均场近似(MFA)的缺点。在HFB方法中自发破坏的对称性的恢复,特别是角动量,是必要的,除其他外,描述激发态和过渡。需要粒子数投影来保证质子和中子的正确数量。此外,在变分之前的投影防止了弱配对区中的配对崩溃。缺乏围绕MFA平均值的波动是这种方法的缺点。为了在BMFT中建立相关性,人们选择了相关的自由度:四极、八极和配对振动以及单粒子振动。在GCM中,代表这些自由度的操作员被用作坐标来生成集体子空间。高度相关的GCM波函数最终被写为该空间的投影基的线性组合。线性组合的系数的变化导致Hill-Wheeler方程。以四极算符为坐标,讨论了经典的β和γ振动。我们目前的配对涨落考虑的配对间隙作为发电机坐标。最后,通过推转过程明确考虑HFB波函数的时间反演对称性破缺,使得核子对的排列在BMFT计算中开辟了一个新的维度。Gogny力的大量计算说明了密度泛函BMFTs的最新发展。最后,我们对该理论的潜在极点进行了深入的讨论。

英文摘要:

We present an overview of beyond mean field theories (BMFT) based on the generator coordinate method (GCM) and the recovery of symmetries used in nuclear physics with effective forces. After a reminder of the Hartree-Fock-Bogoliubov (HFB) theory a discussion of the shortcomings of any mean field approximation (MFA) is presented. The recovery of the symmetries spontaneously broken in the HFB approach, in particular the angular momentum, is necessary, among others, to describe excited states and transitions. Particle number projection is needed to guarantee the right number of protons and neutrons. Furthermore a projection before the variation prevents the pairing collapse in the weak pairing regime. The lack of fluctuations around the average values of the MFA is a shortcoming of this approach. To build in correlations in BMFT one selects the relevant degrees of freedom: quadrupole, octupole and the pairing vibrations as well as the single particle ones. In the GCM the operators representing these degrees of freedom are used as coordinates to generate a collective subspace. The highly correlated GCM wave function is finally written as a linear combination of a projected basis of this space. The variation of the coefficients of the linear combination leads to the Hill-Wheeler equation. We discuss the classical beta and gamma vibrations by considering the quadrupole operators as coordinates. We present pairing fluctuations by considering the pairing gaps as generator coordinates. Lastly the explicit consideration of the time reversal symmetry breaking in the HFB wave function by the cranking procedure allows the alignment of nucleon pairs opening a new dimension in the BMFT calculations. Abundant calculations with the Gogny force illustrate the state-of-the-art of BMFTs with density functionals. We conclude with a thorough discussion on the potential poles of the theory.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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