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α-T模型中准粒子的动力学:赝自旋极化和横向磁场对颤动的作用。

Dynamics of a quasiparticle in the α-T model: role of pseudospin polarization and transverse magnetic field on zitterbewegung.

作者信息

Biswas Tutul, Kanti Ghosh Tarun

机构信息

Department of Physics, University of North Bengal, Raja Rammohunpur-734013, India. Department of Physics, Vivekananda Mahavidyalaya, Burdwan-713103, India.

出版信息

J Phys Condens Matter. 2018 Feb 21;30(7):075301. doi: 10.1088/1361-648X/aaa60b.

Abstract

We consider the α-T model which provides a smooth crossover between the honeycomb lattice with pseudospin 1/2 and the dice lattice with pseudospin 1 through the variation of a parameter α. We study the dynamics of a wave packet representing a quasiparticle in the α-T model with zero and finite transverse magnetic field. For zero field, it is shown that the wave packet undergoes a transient zitterbewegung (ZB). Various features of ZB depending on the initial pseudospin polarization of the wave packet have been revealed. For an intermediate value of the parameter α i.e. for [Formula: see text] the resulting ZB consists of two distinct frequencies when the wave packet was located initially in rim site. However, the wave packet exhibits single frequency ZB for [Formula: see text] and [Formula: see text]. It is also unveiled that the frequency of ZB corresponding to [Formula: see text] gets exactly half of that corresponding to the [Formula: see text] case. On the other hand, when the initial wave packet was in hub site, the ZB consists of only one frequency for all values of α. Using stationary phase approximation, we find analytical expression of velocity average which can be used to extract the associated timescale over which the transient nature of ZB persists. On the contrary, the wave packet undergoes permanent ZB in presence of a transverse magnetic field. Due to the presence of a large number of Landau energy levels, the oscillations in ZB appear to be much more complicated. The oscillation pattern depends significantly on the initial pseudospin polarization of the wave packet. Furthermore, it is revealed that the number of the frequency components involved in ZB depends on the parameter α.

摘要

我们考虑α - T模型,该模型通过参数α的变化,在具有赝自旋1/2的蜂窝晶格和具有赝自旋1的骰子晶格之间提供了一个平滑的过渡。我们研究了在α - T模型中,代表准粒子的波包在零横向磁场和有限横向磁场下的动力学。对于零场情况,结果表明波包会经历瞬态颤动(ZB)。已经揭示了取决于波包初始赝自旋极化的ZB的各种特征。对于参数α的中间值,即对于[公式:见原文],当波包最初位于边缘位置时,产生的ZB由两个不同的频率组成。然而,对于[公式:见原文]和[公式:见原文],波包表现出单频ZB。还发现对应于[公式:见原文]的ZB频率恰好是对应于[公式:见原文]情况的一半。另一方面,当初始波包位于中心位置时,对于所有α值,ZB仅由一个频率组成。使用驻相近似,我们找到了速度平均值的解析表达式,该表达式可用于提取ZB瞬态性质持续的相关时间尺度。相反,在存在横向磁场的情况下,波包会经历永久ZB。由于存在大量的朗道能级,ZB中的振荡似乎要复杂得多。振荡模式显著取决于波包的初始赝自旋极化。此外,还发现参与ZB的频率分量数量取决于参数α。

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