霍尔丹石墨烯台球与相对论中微子台球

Dung Xuan Nguyen, Barbara Dietz
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摘要

我们研究了有限尺寸的蜂窝状晶格--石墨烯台球--的能谱波动特性,其临界点受霍尔丹模型的原位势能和近邻相互作用的影响,下文称之为霍尔丹石墨烯台球。这些石墨烯台球的形状包括具有可积分动力学的矩形台球、具有混沌动力学的矩形台球和具有三重旋转对称性的矩形台球。研究表明,石墨烯台球的光谱特性与具有相应形状的非相对论量子台球的光谱特性相吻合,无论是在能带边缘还是在零能量的迪拉克点附近的低能激发区域。在那里,色散关系是线性的,因此,频谱是用与相对论中微子台球相同的相对论狄拉克方程来描述无质量半自旋粒子的,其频谱特性与违反了时间反转不变性的非相对论量子台球的频谱特性一致。与预期行为的偏差归因于不同的边界条件和边界的反向散射,这导致了对应于两个狄拉克点的谷态的混合,而这两个狄拉克点又通过时间反转相互映射。我们采用哈当模型在两个狄拉克点中的一个点上引入间隙,使反向散射在间隙的能量区域被抑制,并证明在那里光谱中的相关性符合相应形状的中微子台球的相关性。
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Haldane graphene billiards versus relativistic neutrino billiards
We study fluctuation properties in the energy spectra of finite-size honeycomb lattices, graphene billiards, subject to the Haldane-model onsite potential and next-nearest neighbor interaction at critical points, referred to as Haldane graphene billiards in the following. The billiards had the shapes of a rectangular billiard with integrable dynamics, one with chaotic dynamics, and one whose shape has, in addition, threefold rotational symmetry. It had been shown that the spectral properties of the graphene billiards coincide with those of the nonrelativistic quantum billiard with the corresponding shape, both at the band edges and in the region of low energy excitations around the Dirac points at zero energy. There, the dispersion relation is linear and, accordingly, the spectrum is described by the same relativistic Dirac equation for massless half-spin particles as relativistic neutrino billiards, whose spectral properties agree with those of nonrelativistic quantum billiards with violated time-reversal invariance. Deviations from the expected behavior are attributed to differing boundary conditions and backscattering at the boundary, which leads to a mixing of valley states corresponding to the two Dirac points, that are mapped into each other through time reversal. We employ a Haldane model to introduce a gap at one of the two Dirac points so that backscattering is suppressed in the energy region of the gap and demonstrate that there the correlations in the spectra comply with those of the neutrino billiard of the corresponding shape.
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