在多极量子光学中测量尺和单元转换.
1School of Physics, Engineering and Technology, University of York, England, YO10 5DD, UK.
概括
这项研究介绍了多极量子光学的转换,将标尺和单元方法统一到Power-Zienau-Woolley配方中. 它揭示了对量子电动力学中的伦特根和阿哈罗诺夫-卡舍尔效应的见解.
科学领域:
- 量子光学就是一个量子光学.
- 量子电动力学 量子电动力学
- 原子和分子物理学 原子和分子物理学
背景情况:
- 多极量子光学研究了多体系统中的光物质相互作用.
- 传统的形式主义需要转变,以便进行全面的分析.
研究的目的:
- 描述变换统一标尺和单元方法.
- 从非相对论形式主义中推导出Power-Zienau-Woolley的公式.
- 在这个框架内识别罗恩特根和阿哈罗诺夫-卡舍尔效应.
主要方法:
- 在拉格朗的阶段应用到电磁场的尺寸转换.
- 对哈密尔顿式应用的单位转换.
- 对由此产生的量子电动力学公式进行分析.
主要成果:
- 这两种转换产生了Power-Zienau-Woolley的公式.
- 形式主义解释了内部和质量中心运动.
- 识别了伦特根和阿哈罗诺夫-卡舍尔效应.
结论:
- 多极形式主义是光学过程的强大平台.
- 这项研究澄清了伦特根和阿哈罗诺夫-卡舍尔效应的起源.
- 这些效应具有重要的理论和实验意义.
相关概念视频
Quantum Numbers
34.0K
It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
34.0K
The Quantum-Mechanical Model of an Atom
41.5K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing...
41.5K
Potential Due to a Polarized Object
346
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,...
346
Gauss's Law: Cylindrical Symmetry
7.3K
A charge distribution has cylindrical symmetry if the charge density depends only upon the distance from the axis of the cylinder and does not vary along the axis or with the direction about the axis. In other words, if a system varies if it is rotated around the axis or shifted along the axis, it does not have cylindrical symmetry. In real systems, we do not have infinite cylinders; however, if the cylindrical object is considerably longer than the radius from it that we are interested in,...
7.3K
Gauss's Law: Planar Symmetry
7.7K
A planar symmetry of charge density is obtained when charges are uniformly spread over a large flat surface. In planar symmetry, all points in a plane parallel to the plane of charge are identical with respect to the charges. Suppose the plane of the charge distribution is the xy-plane, and the electric field at a space point P with coordinates (x, y, z) is to be determined. Since the charge density is the same at all (x, y) - coordinates in the z = 0 plane, by symmetry, the electric field at P...
7.7K
Symmetry in Maxwell's Equations
3.2K
Once the fields have been calculated using Maxwell's four equations, the Lorentz force equation gives the force that the fields exert on a charged particle moving with a certain velocity. The Lorentz force equation combines the force of the electric field and of the magnetic field on the moving charge. Maxwell's equations and the Lorentz force law together encompass all the laws of electricity and magnetism. The symmetry that Maxwell introduced into his mathematical framework may not be...
3.2K


