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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Electronic properties of a π-conjugated Cairo pentagonal lattice: Direct band gap, ultrahigh carrier mobility, and slanted Dirac cones
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Electronic properties of a π-conjugated Cairo pentagonal lattice: Direct band gap, ultrahigh carrier mobility, and slanted Dirac cones

机译:π共轭开罗五边形晶格的电子性质:直接带隙,超高载流子迁移率和倾斜的狄拉克锥

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摘要

Two-dimensional (2D) lattices composed exclusively of pentagons represent an exceptional structure of materials correlated to the famous pentagonal tiling problem in mathematics, but their π conjugation and the related electronic properties have never been reported. Here, we propose a tight-binding (TB) model for a 2D Cairo pentagonal lattice and demonstrate that p-d π conjugation in the unique framework leads to intriguing properties, such as an intrinsic direct band gap, ultrahigh carrier mobility, and even slant Dirac cones. On the basis of first-principles calculations, we predict a candidate material. 2D penta-NiP_2 monolayer, derivated from bulk NiP_2 crystal, to realize the predictions of the TB model. It has ultrahigh carrier mobility (~10~5-10~6 cm~2 V~(-1) s~(-1)) comparable to that of graphene and an intrinsic direct band gap of 0.818 eV, properties which have long been desired for high-speed electronic devices. The stability and possible synthetic routes of penta-NiP_2 monolayer are also discussed.
机译:仅由五边形组成的二维(2D)晶格表示与数学中著名的五边形平铺问题有关的材料的特殊结构,但从未报道过它们的π共轭和相关的电子性质。在这里,我们提出了二维开罗五边形晶格的紧密结合(TB)模型,并证明了独特框架中的pdπ共轭会产生有趣的特性,例如固有的直接带隙,超高载流子迁移率,甚至是倾斜的狄拉克锥。在第一性原理计算的基础上,我们预测了候选材料。由块状NiP_2晶体衍生而来的二维五元NiP_2单层,可实现对TB模型的预测。它具有与石墨烯相当的超高载流子迁移率(〜10〜5-10〜6 cm〜2 V〜(-1)s〜(-1))和本征直接带隙为0.818 eV,长期以来一直是这种性能高速电子设备所需要的。还讨论了五NiP_2单层的稳定性和可能的​​合成途径。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2018年第8期|085437.1-085437.10|共10页
  • 作者单位

    School of Physics and Stale Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, Shandong, China;

    School of Physics and Stale Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, Shandong, China;

    School of the Gifted Young, University of Science and Technology of China, Hefei 230026, Anhui, China;

    School of Physics and Stale Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, Shandong, China;

    School of Physics and Stale Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, Shandong, China;

    School of Physics and Stale Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, Shandong, China;

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