在非互惠的威利斯单原子格子中,Brillouin区域的定义是不互惠的
1Department of Mechanical Engineering, Union College, Schenectady, New York 12308, USAalbabaah@union.edu.
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|December 1, 2023
概括
在非互惠的威利斯单原子格子 (WMLs) 中分析了布里卢恩区域 (BZ) 定义. BZ边界随着非互惠的变化而变化,在1D和2D网格中产生不对称的波传播.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 固态物理 固态物理
- 材料科学是一种材料科学.
背景情况:
- 非互惠的网格表现出独特的波浪传播特性.
- 了解Brillouin区域 (BZ) 行为对于描述格子动态至关重要.
- 威利斯单原子格子 (WMLs) 为探索非互惠提供了一个可调的平台.
研究的目的:
- 在非互惠的威利斯单原子格子 (WMLs) 中分析量化布里卢恩区域 (BZ) 定义.
- 调查非互惠对 BZ 几何和带结构的影响.
- 在一维和二维WML中探索BZ的行为.
主要方法:
- 分析量化Brillouin区域边界的分析量化.
- 对非互惠网格的分散图的分析.
- 对二维 (正方形) WMLs 的数学扩展.
主要成果:
- 在1D WML中,BZ边界由于非互惠性而变化,保持恒定宽度,但产生不对称的分散.
- 散射图显示前进和后退波的波数范围不均.
- 在正方形WML中,非互惠导致移动和不规则形状的BZ具有恒定的面积.
结论:
- 非互惠性从根本上改变了WMLs中的Brillouin区域特征.
- 观察到的BZ转移和形状变化直接影响波浪传播行为.
- 这些发现为设计具有量身定制的波动力学的新型超材料提供了洞察力.
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