相关实验视频
Updated: Sep 13, 2025

11:21
Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
Published on: March 30, 2017
7.6K
用冷原子观察费米加速
G Barontini1, V Naniyil1, J P Stinton1
1University of Birmingham, School Of Physics and Astronomy, Edgbaston, Birmingham B15 2TT, United Kingdom.
Physical review letters
|July 31, 2025
概括
科学家们使用超冷原子制造了一个可控制的费米加速器. 这种实验室模型模仿宇宙射线加速,产生高速的原子喷气,并使天体物理学和量子技术的新研究成为可能.
科学领域:
- 天体物理学 天体物理学
- 量子技术 量子技术是一种量子技术.
- 原子物理 原子物理
背景情况:
- 宇宙射线通过费米加速加速,一个过程涉及粒子散射在天体物理等离子体中的磁波动.
- 费米加速是一种具有经典和量子公式的通用过程,支着像费米-乌拉姆模型这样的动态系统.
- 在实验室环境中直接实验验证费米加速一直是具有挑战性的.
研究的目的:
- 为了实现一个完全可控制的实验室费米加速器.
- 通过使用超冷原子和工程潜在障碍来研究费米加速.
- 实验测试关于加速系统中的能量光谱的理论论证.
主要方法:
- 开发一个微尺度 (100微米) 费米加速器.
- 超冷原子与工程,可移动的潜在障碍物的碰撞.
- 引入消散来测试贝尔对能量光谱的论证.
主要成果:
- 成功创建一个可控制的费米加速器.
- 产生速度超过0.5m/s的超冷原子喷气.
- 对于加速系统中的能量光谱的贝尔论证的实验验证.
结论:
- 这项研究为使用冷原子来研究高能天体物理现象开辟了道路.
- 与现有的量子技术相比,展示的费米加速器提供了更简单的实现.
- 性能与量子技术和碰撞器中最先进的加速方法相竞争.
相关概念视频
Atomic Nuclei: Larmor Precession Frequency
1.7K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
1.7K
Atomic Spectroscopy: Effects of Temperature
460
Atomization, converting samples into gas-phase atoms and ions, is essential for atomic spectroscopy. The flame temperature required for atomization affects the efficiency of the atomic spectroscopic methods by increasing the atomization efficiency and the relative population of the excited and ground states.
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
460
Fermi Level Dynamics
346
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
346
Atomic Force Microscopy
3.6K
Atomic force microscopy (AFM) is a type of scanning probe microscopy that can analyze topographic details of various specimens like ceramics, glass, polymers, and biological samples. AFM offers over 1000 times more resolution than the optical imaging system. Images generated from AFM are three-dimensional surface profiles, offering an advantage over the flat, two-dimensional images from other imaging techniques.
The AFM Probe
The probe is regarded as the heart of any AFM setup and comprises the...
The AFM Probe
The probe is regarded as the heart of any AFM setup and comprises the...
3.6K
Fermi Level
817
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,...
817
Atomic Emission Spectroscopy: Instrumentation
601
The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers. Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
601

