连续体中的全光学允许度-非对称的准束状态
Rodrigo Berté1, Thomas Possmayer2, Andreas Tittl3
1Chair in Hybrid Nanosystems, Nanoinstitut München, Fakultät für Physik, Ludwig-Maximilians-Universität München, München, 80799, Germany. R.Berte@physik.uni-muenchen.de.
Light, science & applications
|May 7, 2025
概括
研究人员使用激光光在薄膜中诱导可调节的光子共振. 这种破坏对称的方法可以精确控制光物质相互作用,并为先进的光学应用选择波长.
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
背景情况:
- 响应通常发生在有限系统中.
- 光学属性的定期调制可以在连续介质中诱导共振.
研究的目的:
- 证明薄膜中的周期性电容度调制可以打破对称性,并在连续体 (qBICs) 中激发光子准束状态.
- 为了证明短暂的共振可以通过超短激光脉冲干扰来定制.
主要方法:
- 使用干扰的超短激光脉冲定期调节薄膜电容性.
- 通过调整束参数来定制短暂共振.
主要成果:
- 在连续体 (qBICs) 中通过对称性破坏激发光子准束状态.
- 波长和质量因子中的可调共振.
- 第三和生成的光谱选择性增强.
- 观测超快的动态和时间选择性近场增强,精确到皮秒.
结论:
- 光学诱导的电容性不对称性为无边界介质中可调节的共振提供了一条途径.
- 在按需的光物质相互作用和用于动态光操纵的无 lithography 的 metasurfaces 中的潜在应用.
更多相关视频
相关概念视频
Susceptibility, Permittivity and Dielectric Constant
1.3K
When placed in an external electric field, a dielectric material gets polarized. The charge density in the dielectric material is given by the sum of the bound and free charge densities, while the total charge density can also be written in terms of the total electric field. The bound charge density can be measured in terms of polarization, leading to the relationship between electric displacement and polarization.
1.3K
Electrostatic Boundary Conditions in Dielectrics
1.0K
When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's...
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's...
1.0K
Electromagnetic Waves in Matter
2.9K
Electromagnetic waves can travel in the vacuum as well as in matter. For example light, which is an electromagnetic wave, can travel through air, water, or glass.
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the...
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the...
2.9K
Dielectric Polarization in a Capacitor
4.5K
The presence of a dielectric medium in a capacitor not only changes the voltage and capacitance but also affects the electric field. In general, dielectrics can be of two types: polar and nonpolar. In a polar dielectric, the positive and negative charges in the molecules are separated by a distance and hence have a permanent dipole moment. In contrast, no such charge separation exists in a nonpolar dielectric, however the nonpolar molecules get polarized in the presence of an external electric...
4.5K
Potential Due to a Polarized Object
351
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
351
The de Broglie Wavelength
25.2K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
25.2K


