非赫米蒂亚边缘的声音爆发
Hong-Yu Zou1, Bing-Bing Wang1,2, Yong Ge1
1Research Center of Fluid Machinery Engineering and Technology, School of Physics and Electronic Engineering, Jiangsu University, Zhenjiang, China.
Advanced materials (Deerfield Beach, Fla.)
|February 6, 2026
概括
声学晶体中的非赫米特带拓导致边界局部化的能量损失,称为非赫米特边缘爆发. 这种现象,取决于虚构的差距关闭,可以发生在一个或两个边界.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 声学元材料是一种声学元材料.
- 非赫米特物理学 非赫米特物理学
背景情况:
- 非赫密斯带拓引入了赫密斯系统中缺少的独特现象,例如非赫密斯皮肤效应 (NHSE).
- 丢失的非赫密斯系统表现出边界局部损失概率,需要非赫密斯带拓和封闭的想象间隙.
研究的目的:
- 为了在经典波系统中证明非赫密斯边缘爆裂现象.
- 为了研究损失的非互惠声学晶体中边缘爆发的条件和特征.
主要方法:
- 一个有损失的非互惠声学晶体的理论分析.
- 对自身能量光谱的研究,以确定虚构的差距关闭点.
- 在不同的条件下,局限局部化的能量损失的表征.
主要成果:
- 非赫米斯边缘爆发在经典的声学超材料中得到了证明.
- 边缘爆发可以发生在右边界,左边界,或两者 (双极边缘爆发),这取决于想象中的差距关闭.
- 边缘破裂的具体场景是由假想的差距关闭点的数量和位置决定的.
结论:
- 边缘爆发的概念从量子扩展到古典波浪系统.
- 边缘爆破被确立为声学晶体中的内在材料属性.
- 这些发现丰富了对非赫米特带拓与材料特性相互作用的理解.
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