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Exclusive sub-lattices for extended and localized states in graphene ribbons: their role in Klein tunneling, disorder and magnetic field effects

机译:石墨烯带中扩展和局部状态的唯一子晶格:它们在克莱因隧穿,无序和磁场效应中的作用

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We report the existence of two sub-lattices in metallic graphene nanoribbons that present a decoupled behavior. Each sub-lattice, one for extended states (ES) and another exclusively for localized states (LS), is formed by a combination of A and B graphene sites. In the sub-lattice ES all electronic transport phenomena occur, including the Klein tunneling through an external applied potential barrier. In contrast, the sub-lattice LS does not contribute to the transport of quasi-particles and strongly localized states are induced within the potential barrier region. The sub-lattices ES and LS are detected by analyzing Klein states and totally localized states that were systematically perturbed by the contributions of hyperboloid bands generated by the potential barrier. This is performed by gradually increasing the energy of the applied potential. The existence of both sub-lattices are tested by considering disorder and magnetic field effects in the system. The results indicate that both sublattices behave as if there are decoupled, even at the presence of an external applied barrier and that they can be coupled by applying an external magnetic field.
机译:我们报告了金属石墨烯纳米带中存在两个子格,它们表现出分离的行为。每个子晶格(一个用于扩展状态(ES),另一个专门用于局部状态(LS))由A和B石墨烯位点组成。在亚晶格ES中,所有电子传输现象都会发生,包括穿过外部施加的势垒的Klein隧穿。相反,亚晶格LS不会有助于准粒子的传输,并且在势垒区域内会诱导出强烈的局部状态。通过分析由势垒产生的双曲面带的贡献而系统地扰动的克莱因态和完全局域态,可以检测出亚晶格ES和LS。这是通过逐渐增加施加电势的能量来执行的。通过考虑系统中的无序和磁场效应来测试两个子晶格的存在。结果表明,即使在存在外部施加的势垒的情况下,两个子晶格也表现出去耦的状态,并且可以通过施加外部磁场来耦合它们。

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