Landau levels for a Weyl pair in a monolayer medium and thermal quantities

IF 1.2 4区 物理与天体物理 Q3 PHYSICS, MULTIDISCIPLINARY
Abdullah Guvendi, Abdelmalek Boumali
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Abstract

In this paper, we consider a Weyl pair under the effect of an external uniform magnetic field in a monolayer medium without considering any charge-charge interaction between the particles. Choosing the interaction of the particles with the magnetic field in the symmetric gauge we seek for an analytical solution of the corresponding form of a one-time fully-covariant two-body Dirac equation derived from quantum electrodynamics via the action principle. As it is usual with two-body problems, we separate the relative motion and center of mass motion coordinates. Assuming the center of mass is at rest, we derive a matrix equation in terms of the relative motion coordinates without considering any group theoretical method. This equation gives a wave equation in exactly soluble form and accordingly we obtain the spinor components and complete energy eigen-states (in closed form) for such a spinless composite structure. Our results not only give exact Landau levels for such a Weyl pair in a monolayer medium but also show the considered system behaves as a two-dimensional harmonic oscillator. Furthermore, our findings give exactly the excited states of a Weyl particle under the effect of uniform external magnetic field in a monolayer graphene sheet and there is no imprint to distinguish these modes from each other. This means that the performed experiments based on Landau levels for a monolayer graphene sheet may actually involve many-body effects. Our results provide a suitable basis to analyze the associated thermal quantities and accordingly we discuss the thermal properties by determining free energy, total energy, entropy and specific heat for the composite system in question.
单层介质中Weyl对的朗道能级和热量
在本文中,我们考虑了外均匀磁场作用下单层介质中的Weyl对,而不考虑粒子之间的电荷相互作用。选取对称规范中粒子与磁场的相互作用,利用作用原理,从量子电动力学推导出一次性全协变二体狄拉克方程,寻求其相应形式的解析解。与通常的两体问题一样,我们将相对运动坐标和质心运动坐标分开。假设质心处于静止状态,在不考虑任何群论方法的情况下,导出了相对运动坐标下的矩阵方程。该方程给出了一个完全可溶形式的波动方程,从而得到了这种无自旋复合结构的旋量分量和完全能量本征态(闭态)。我们的结果不仅给出了这种Weyl对在单层介质中的精确朗道能级,而且还显示了所考虑的系统表现为二维谐振子。此外,我们的研究结果准确地给出了Weyl粒子在单层石墨烯片上均匀外磁场作用下的激发态,并且没有印记来区分这些模式。这意味着基于朗道能级对单层石墨烯片进行的实验实际上可能涉及多体效应。我们的结果为分析相关的热量提供了一个合适的基础,因此我们通过确定所讨论的复合系统的自由能、总能、熵和比热来讨论热性质。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Revista Mexicana De Fisica
Revista Mexicana De Fisica 物理-物理:综合
CiteScore
2.20
自引率
11.80%
发文量
87
审稿时长
4-8 weeks
期刊介绍: Durante los últimos años, los responsables de la Revista Mexicana de Física, la Revista Mexicana de Física E y la Revista Mexicana de Física S, hemos realizado esfuerzos para fortalecer la presencia de estas publicaciones en nuestra página Web ( http://rmf.smf.mx).
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