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有限温度准一维电子气中的自旋关联与自旋密度波相

Spin correlations and spin-density wave phase in a finite-temperature quasi-one-dimensional electron gas.

作者信息

Kaur Kulveer, Sharma Akariti, Garg Vinayak, Moudgil R K

机构信息

Department of Physics, Punjabi University, Patiala 147 002, India.

Department of Physics, Kurukshetra University, Kurukshetra 136 119, India.

出版信息

J Phys Condens Matter. 2021 May 24;33(26). doi: 10.1088/1361-648X/abf977.

Abstract

In this paper, we theoretically investigate the effect of temperature on spin correlations in an unpolarized quasi-one-dimensional electron gas (Q1DEG). The correlations are treated dynamically within quantum version of the self-consistent mean-field approach of SingwiNumerical results for the ↑↑ and ↑↓ components of static structure factor and pair-correlation function, and the wave vector dependent static spin and charge susceptibilities are presented over a wide range of temperatureand electron coupling. We find that the recently reported (2020335403) non-monotonic-dependence of the contact pair-correlation function(= 0;) is driven primarily by an interplay between ↑↓ correlations and thermal effects. At a given temperature, the dynamics of both ↑↑ and ↑↓ correlations is found to become significant with increasing coupling, manifesting unambiguously as pronounced peak at 3.5(periodic oscillations) in the corresponding components of the structure factor (pair-correlation function). Analysis of static spin and charge susceptibilities reveals that an imbalance between ↑↑ and ↑↓ correlations may induce a transition to a spin-density wave (SDW) phase of wave vector ∼3.5above a critical coupling for a sufficiently high, while to a long-wavelength SDW phase at a low. Higher the temperature, higher is the predicted critical coupling for the SDW phase. Interestingly, transition to the SDW phase is found to precede the recently predicted Wigner crystal instability in the finite-Q1DEG. Further, if one starts with partially spin-polarized electrons, the SDW instability is found to shift to somewhat higherand. In addition, we have presented results for the free exchange-correlation energy, free correlation energy, and excess kinetic energy for the unpolarized and fully spin-polarized phases of the finite-Q1DEG. Wherever interesting, we have compared our results with the predictions of the static version of the mean-field approach.

摘要

在本文中,我们从理论上研究了温度对非极化准一维电子气(Q1DEG)中自旋关联的影响。采用Singwi自洽平均场方法的量子版本动态处理这些关联。给出了在很宽的温度和电子耦合范围内,静态结构因子和对关联函数的↑↑和↑↓分量以及与波矢相关的静态自旋和电荷磁化率的数值结果。我们发现,最近报道的(2020335403)接触对关联函数(= 0;)的非单调依赖性主要由↑↓关联与热效应之间的相互作用驱动。在给定温度下,发现随着耦合增加,↑↑和↑↓关联的动力学都变得显著,在结构因子(对关联函数)的相应分量中明确表现为在3.5处有明显峰值(周期性振荡)。对静态自旋和电荷磁化率的分析表明,↑↑和↑↓关联之间的不平衡可能会在足够高的温度下,在临界耦合之上诱导向波矢约为3.5的自旋密度波(SDW)相转变,而在低温下则向长波长SDW相转变。温度越高,预测的SDW相临界耦合越高。有趣的是,发现向SDW相的转变先于有限Q1DEG中最近预测的维格纳晶体不稳定性。此外,如果从部分自旋极化的电子开始,发现SDW不稳定性会转移到稍高的和。另外,我们给出了有限Q1DEG的非极化和完全自旋极化相的自由交换关联能、自由关联能和过剩动能的结果。在有意义的地方,我们将我们的结果与平均场方法静态版本的预测进行了比较。

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