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arXiv 1902.05477nucl-thcond-mat.quant-gas
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大s波散射长度费米体系的近似自能:迈向密度泛函理论的一步

Approximate self-energy for Fermi systems with large s-wave scattering length: a step towards density functional theory

Antoine Boulet, Denis Lacroix

摘要:

在目前的工作中,我们开始从费米系统的最小哈密顿量的s-波散射是唯一的低能量常数在发挥作用。首先讨论了通常适用于较低密度的多体微扰法。然后,我们使用的再结晶技术与阶梯近似,以获得紧凑的表达式的能量和/或在壳层自能在无限自旋简并系统。与多体微扰理论相比,图解重算技术在一般情况下具有在更大密度区域内预测的优点。它也导致了非发散极限为$|a_s| \rightarrow + \infty$。尽管如此,得到的表达式是相当复杂的费米动量$k_F$的功能。我们引入全相空间平均或部分相空间方法分别应用于能量或自能,以简化它们对$(a_s k_F)$的依赖性,同时保持低密度下的正确极限和大$|a_s k_F|$的非发散性质。在不同的密度和散射长度的区域费米系统的准粒子性质进行了说明。我们的结论是,这种简化的表达式,其中的直接联系与低能量常数没有微调,可以提供一个明确的指导,以获得密度泛函理论超越微扰制度。然而,接近或接近么正的准粒子性质不能被再现,除非这个限制被明确地用作约束。最后讨论了这种准粒子近似处理如何指导强相互作用费米系统的密度泛函理论的发展。

英文摘要:

In the present work, we start from a minimal Hamiltonian for Fermi systems where the s-wave scattering is the only low energy constant at play. Many-Body Perturbative approach that is usually valid at rather low density is first discussed. We then use the resummation technique with the ladder approximation to obtain compact expressions for both the energy and/or the on-shell self-energy in infinite spin-degenerated systems. Diagrammatic resummation technique has the advantage in general to be predictive in a region of density larger compared to many-body perturbation theory. It also leads to non-diverging limit as $|a_s| \rightarrow + \infty$. Still, the obtained expressions are rather complex functional of the Fermi momentum $k_F$. We introduce the full phase-space average or the partial phase-space methods respectively applied to the energy or to the self-energy to simplify their dependences in terms of $(a_s k_F)$ while keeping the correct limit at low density and the non-diverging property at large $|a_s k_F|$. Quasi-particle properties of Fermi system in various regime of density and scattering length are then illustrated. Our conclusion is that such simplified expressions where the direct link is made with the low energy constant without fine-tuning can provide a clear guidance to obtain density functional theory beyond the perturbative regime. However, quasi-particle properties close or near unitary cannot be reproduced unless this limit is explicitly used as a constraint. We finally discuss how such approximate treatment of quasi-particle can guide the development of density functional theory for strongly interacting Fermi systems.

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