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节线半金属量子振荡过程中的费米能级涨落、有效质量减小和塞曼效应。

Fermi level fluctuations, reduced effective masses and Zeeman effect during quantum oscillations in nodal line semimetals.

作者信息

Kar Satyaki, Saha Anupam

机构信息

AKPC Mahavidyalaya, Bengai, West Bengal-712611, India.

出版信息

J Phys Condens Matter. 2021 Oct 29;34(3). doi: 10.1088/1361-648X/ac2c40.

DOI:10.1088/1361-648X/ac2c40
PMID:34598178
Abstract

We probe quantum oscillations in nodal line semimetals (NLSM) by considering an NLSM continuum model under strong magnetic field and report the characteristics of the Landau level (LL) spectra and the fluctuations in the Fermi level as the field in a direction perpendicular to the nodal plane is varied through. Based on the results on parallel magnetization, we demonstrate the growth of quantum oscillation with field strength as well as its constancy in period when plotted against 1/. We find that the density of states (DOS) which show series of peaks in succession, witness bifurcation of those peaks due to Zeeman effect. For field normal to nodal plane, such bifurcations are discernible only if the electron effective mass is considerably smaller than its free value, which usually happens in these systems. Though a reduced effective mass* causes the Zeeman splitting to become small compared to LL spacings, experimental results indicate a manifold increase in the Landefactor which again amplifies the Zeeman contribution. We also consider magnetic field in the nodal plane for which the DOS peaks do not repeat periodically with energy anymore. The spectra become more spread out and the Zeeman splittings become less prominent. We find the low energy topological regime, that appears with such in-plane field set up, to shrink further with reduced* values. However, such topological regime can be stretched out in case there are smaller Fermi velocities for electrons in the direction normal to the nodal plane.

摘要

我们通过考虑强磁场下的节点线半金属(NLSM)连续模型来探究其量子振荡,并报告当垂直于节点平面方向的磁场变化时朗道能级(LL)谱的特征以及费米能级的涨落情况。基于平行磁化的结果,我们证明了量子振荡随磁场强度的增长以及其相对于1/绘制时周期的恒定性。我们发现,连续显示出一系列峰值的态密度(DOS),由于塞曼效应见证了这些峰值的分叉。对于垂直于节点平面的磁场,只有当电子有效质量远小于其自由值时,这种分叉才明显,而这在这些系统中通常会发生。尽管有效质量的减小会使塞曼分裂相对于LL间距变小,但实验结果表明朗德因子会大幅增加,这再次放大了塞曼贡献。我们还考虑了节点平面内的磁场,对于这种情况,DOS峰值不再随能量周期性重复。谱变得更加分散,塞曼分裂也变得不那么显著。我们发现,随着有效质量*值的减小,这种平面内磁场设置下出现的低能拓扑区域会进一步缩小。然而,如果在垂直于节点平面的方向上电子的费米速度较小,这种拓扑区域可以被扩展。

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