相关实验视频
Updated: Jun 21, 2025

11:21
Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
Published on: March 30, 2017
7.4K
一个二维波斯气体的地面状态能量
Søren Fournais1, Theotime Girardot2, Lukas Junge1
1Department of Mathematical Sciences, University of Copenhagen, Universitetsparken 5, Dk-2100 Copenhagen, OE Denmark.
概括
我们得出了2D稀释斯气体基本状态能量密度的公式. 这一结果与3D中的李-黄-公式相似,适用于各种电位.
科学领域:
- 量子力学就是量子力学.
- 统计力学就是统计力学.
- 凝聚物质物理学 凝聚物质物理学
背景情况:
- 稀释波斯气体是量子物理学的基本系统.
- 了解它们的基本状态属性对于多体物理学至关重要.
- 现有的公式,如3D中的李黄,提供了关键的见解.
研究的目的:
- 要推导出2D稀释斯气体的基本状态能量密度的公式.
- 为了建立一个2D模拟的李-黄-公式.
- 为了验证该公式对广泛的潜能进行验证.
主要方法:
- 使用量子场理论技术进行数学推导.
- 对斯气体特性热力学极限的分析.
- 专注于低密度和有限散射长度的系统.
主要成果:
- 证明了2D中基本状态能量密度的精确公式.
- 衍生式是,其中和是散射长度.
- 该公式适用于具有有限散射长度的电位,包括硬核电位.
结论:
- 该研究成功地建立了2D稀释斯气体的基态能量密度公式.
- 这项工作为众所周知的3D李-黄-公式提供了2D对应.
- 证明的通用性确保了对各种物理潜力的适用性.
相关概念视频
The Bohr Model
52.3K
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...
52.3K
Atomic Nuclei: Nuclear Spin State Population Distribution
971
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.
971
Internal Energy
4.7K
The internal energy of a thermodynamic system is the sum of the kinetic and potential energies of all the molecules or entities in the system. The kinetic energy of an individual molecule includes contributions due to its rotation and vibration, as well as its translational energy. The potential energy is associated only with the interactions between one molecule and the other molecules of the system. Neither the system's location nor its motion is of any consequence as far as the internal...
4.7K
Third Law of Thermodynamics
18.8K
A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
18.8K
Molecular Kinetic Energy
5.1K
The word "gas" comes from the Flemish word meaning "chaos," first used to describe vapors by the chemist J. B. van Helmont. Consider a container filled with gas, with a continuous and random motion of molecules. During collisions, the velocity component parallel to the wall is unchanged, and the component perpendicular to the wall reverses direction but does not change in magnitude. If the molecule’s velocity changes in the x-direction, then its momentum is changed.
5.1K
Van der Waals Equation
4.0K
The ideal gas law is an approximation that works well at high temperatures and low pressures. The van der Waals equation of state (named after the Dutch physicist Johannes van der Waals, 1837−1923) improves it by considering two factors.
First, the attractive forces between molecules, which are stronger at higher densities and reduce the pressure, are considered by adding to the pressure a term equal to the square of the molar density multiplied by a positive coefficient a. Second, the volume...
First, the attractive forces between molecules, which are stronger at higher densities and reduce the pressure, are considered by adding to the pressure a term equal to the square of the molar density multiplied by a positive coefficient a. Second, the volume...
4.0K

