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Band warping, band non-parabolicity, and Dirac points in electronic and lattice structures

机译:乐队翘曲,乐队非抛物,和电子和晶格结构中的DIRAC点

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Abstract We illustrate at a fundamental level the physical and mathematical origins of band warping and band non-parabolicity in electronic and vibrational structures. We point out a robust presence of pairs of topologically induced Dirac points in a primitive-rectangular lattice using a p-type tight-binding approximation. We analyze two-dimensional primitive-rectangular and square Bravais lattices with implications that are expected to generalize to more complex structures. Band warping is shown to arise at the onset of a singular transition to a crystal lattice with a larger symmetry group, which allows the possibility of irreducible representations of higher dimensions, hence band degeneracy, at special symmetry points in reciprocal space. Band warping is incompatible with a multi-dimensional Taylor series expansion, whereas band non-parabolicities are associated with multi-dimensional Taylor series expansions to all orders. Still band non-parabolicities may merge into band warping at the onset of a larger symmetry group. Remarkably, while still maintaining a clear connection with that merging, band non-parabolicities may produce pairs of conical intersections at relatively low-symmetry points. Apparently, such conical intersections are robustly maintained by global topology requirements, rather than any local symmetry protection. For two p-type tight-binding bands, we find such pairs of conical intersections drifting along the edges of restricted Brillouin zones of primitive-rectangular Bravais lattices as lattice constants vary relatively to each other, until these conical intersections merge into degenerate
机译:<![cdata [ 抽象 我们以基本级别说明了电子和振动结构中的带翘曲和带非抛物率的物理和数学起源。我们使用A P 型紧密结合近似,指出了原始矩形晶格成对的拓扑诱导的颗粒状点对的鲁棒存在。我们分析了二维原语 - 矩形和方形Bravais格子,其中有望推广到更复杂的结构。在具有较大对称基团的晶格的单数转变的晶格开始时出现带翘曲,这允许在往复空间中的特殊对称点处的较高尺寸的不可缩短的尺寸的不可缩短的表示。乐队翘曲与多维泰勒系列扩展不兼容,而乐队非抛物率与所有订单相关的多维泰勒串联扩展。仍然乐队非抛物率可以合并到较大对称组的开始处的带翘曲。值得注意的是,同时仍然保持与该合并的明确连接,频带非抛物率可以在相对低对称点处产生成对的锥形交叉点。显然,这种锥形交叉点受到全球拓扑要求的强大维护,而不是任何局部对称保护。对于两个 p - 型紧密绑带,我们发现这种圆锥形交叉点沿着原始的矩形Bravais格子的限制布里渊区的边缘漂移,因为晶格常数相对彼此不同,直到这些锥形交叉融为堕落

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