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Waveguiding in massive two-dimensional Dirac systems

机译:大规模二维狄拉克系统中的波导

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摘要

The study of waveguide propagating modes is essential for achieving directional electronic transport in two-dimensional materials. Simultaneously, exploring potential gaps in these systems is crucial for developing devices akin to those employed in conventional electronics. Building upon the theoretical groundwork laid by Hartmann and Portnoi Phys. Rev. A 89, 012101 (2014), which focused on implementing waveguides in pristine graphene monolayers, this work delves into the impact of a waveguide on two-dimensional gapped Dirac systems. We derive exact solutions encompassing wave functions and energy-bound states for secant-hyperbolic attractive potential in gapped graphene, with a gap generated by sublattice asymmetry or Kekulé-distortion. These solutions leverage the inherent properties and boundary conditions of the Heun polynomials. Our findings demonstrate that the manipulation of the number of accessible energy-bound states, i.e., transverse propagating modes, relies on factors, such as the width and depth of the potential as well as the gap value of the two-dimensional material.
机译:波导传播模式的研究对于实现二维材料的定向电子传输至关重要。同时,探索这些系统中的潜在差距对于开发类似于传统电子产品中使用的设备至关重要。在Hartmann和Portnoi奠定的理论基础上[Phys. Rev. A 89, 012101 (2014)],这项工作专注于在原始石墨烯单层中实现波导,这项工作深入研究了波导对二维间隙狄拉克系统的影响。我们推导了包含波函数和能量束缚态的精确解,用于间隙石墨烯中割线双曲吸引势,以及由亚晶格不对称或凯库勒畸变产生的间隙。这些解决方案利用了 Heun 多项式的固有性质和边界条件。我们的研究结果表明,可接近的能量束缚态数量的操纵,即横向传播模式,依赖于诸如势的宽度和深度以及二维材料的间隙值等因素。

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