在哈伯德模型中,反铁磁排序的拓半金属具有旋转轨道合
Garima Goyal1, Dheeraj Kumar Singh1
1Department of Physics and Materials Science, Thapar Institute of Engineering and Technology, Patiala 147004, Punjab, India.
概括
研究人员在2D系统中探索了具有磁性秩序的迪拉克半金属. 他们确定了稳定条件并分析了边缘状态,在磁场下发现过渡到韦尔半金属状态.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 量子力学就是量子力学.
背景情况:
- 迪拉克半金属是具有独特电子性质的拓材料.
- 非对称的对称性在新的量子现象中起着至关重要的作用.
- 磁性排序可以显著改变电子带结构.
研究的目的:
- 调查二维系统中具有磁性秩序的迪拉克半金属的存在.
- 为了确定稳定这些状态的相位图.
- 分析边缘状态和磁场的影响.
主要方法:
- 哈特里-福克平均场理论.
- 哈巴德模型. 哈巴德模型.
- 阶段图分析 (第二邻旋轨道合与哈伯德相互作用).
主要成果:
- 在相位图中确定了一个区域,在该区域中,具有磁顺序的迪拉克半金属得到稳定.
- 在直角方向上的带的计算边缘状态.
- 在平面内磁场下观察到韦尔半金属 (WSM) 状态的稳定.
结论:
- 非对称的对称性使得2D系统中的磁性迪拉克半金属状态成为可能.
- 磁场可以诱导拓相位过渡到WSM状态.
- 边缘状态在迪拉克和韦尔半金属阶段表现出不同的行为.
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