在元材料中的拓过渡
Harish N S Krishnamoorthy1, Zubin Jacob, Evgenii Narimanov
1Department of Physics, Queens College, City University of New York (CUNY), Flushing, NY 11367, USA.
概括
研究人员发现了超材料中的光学拓过渡. 这种过渡极大地增加了光子密度,增强了光物质相互作用和自发发射率.
科学领域:
- 光学和光子学 在光学和光子学.
- 材料科学 材料科学 材料科学
- 凝聚物质物理学 凝聚物质物理学
背景情况:
- 光-物质相互作用对许多科学和技术领域至关重要.
- 控制这些相互作用通常依赖于设计光子环境.
- 超材料由于其人工纳米结构,为操纵光提供了独特的可能性.
研究的目的:
- 为了研究异性质的元材料中的光学拓过渡.
- 为了证明这种过渡如何增强光物质相互作用.
- 探索拓过渡的潜力,以控制自发排放.
主要方法:
- 使用人工纳米结构制造,制造强有异性质的元材料.
- 对同频面的拓学的理论分析.
- 在超材料附近实验测量自发发射率.
主要成果:
- 观察到一种光学拓过渡,将异频表面从一个封闭的圆形变为一个开放的超波形.
- 这种拓过渡导致了状态的光子密度显著增加.
- 在超材料附近的发射器中测量了自发发射率的增加.
结论:
- 改变超材料中异频表面的拓,为控制光物相互作用提供了一种新的方法.
- 这种方法为增强自发发射等现象提供了新的途径.
- 这些发现为设计先进的光学设备和控制量子现象开辟了道路.
相关概念视频
Properties of Transition Metals
Transition metals are defined as those elements that have partially filled d orbitals. As shown in Figure 1, the d-block elements in groups 3–12 are transition elements. The f-block elements, also called inner transition metals (the lanthanides and actinides), also meet this criterion because the d orbital is partially occupied before the f orbitals.
Phase Transitions
Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to occupy...
Standing Waves in a Cavity
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:


