相关实验视频
Updated: Jun 28, 2025

11:21
Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
Published on: March 30, 2017
7.4K
在室温下从连续体中的束状态中激发极子凝结
Xianxin Wu1,2, Shuai Zhang1, Jiepeng Song3
1CAS Key Laboratory of Standardization and Measurement for Nanotechnology, National Center for Nanoscience and Technology, Beijing, 100190, P. R. China.
Nature communications
|April 18, 2024
概括
在矿光子晶体中实现了室温激子-极子凝结. 这一突破使低值连贯光源和集成光子电路成为可能.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 光子学是指光子学的使用方法.
- 材料科学 是一种材料科学.
背景情况:
- 刺激极光子 (极光子) 对于开发节能连贯光源至关重要.
- 连续体中的边界状态 (BIC) 为极子凝聚提供了高质量的因子.
- 目前的BIC极子凝结受限于冷温度,因为激子的结合能很低.
研究的目的:
- 为了证明室温BIC极子凝结.
- 为了探索波束发射和模式切换在BIC极子中.
- 为了使BIC极子凝结物的实际应用.
主要方法:
- 使用矿光子晶格.
- 在极子分散的位点附近调查极子凝聚.
- 分析用于模式切换的极子-极子散射.
主要成果:
- 在矿光子晶体中实现了室温BIC极子凝结.
- 观测到具有长距离连贯性的定向束辐射.
- 在小型化的BIC极子模式之间展示了切换效应.
结论:
- 在矿光子晶体中,室温BIC极子凝结是可行的.
- 这一进步支持集成光子和拓电路的开发.
- 这些发现为实际的,节能的光通信技术铺平了道路.
相关概念视频
Phase Transitions: Vaporization and Condensation
17.6K
The physical form of a substance changes on changing its temperature. For example, raising the temperature of a liquid causes the liquid to vaporize (convert into vapor). The process is called vaporization—a surface phenomenon. Vaporization occurs when the thermal motion of the molecules overcome the intermolecular forces, and the molecules (at the surface) escape into the gaseous state. When a liquid vaporizes in a closed container, gas molecules cannot escape. As these gas phase...
17.6K
Potential Due to a Polarized Object
398
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,...
398
Atomic Nuclei: Nuclear Spin State Population Distribution
974
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
974
Fermi Level
589
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
589
The Bohr Model
53.2K
Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as...
53.2K
Atomic Nuclei: Nuclear Relaxation Processes
649
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
649

