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The Energies of Atomic Orbitals03:21

The Energies of Atomic Orbitals

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In an atom, the negatively charged electrons are attracted to the positively charged nucleus. In a multielectron atom, electron-electron repulsions are also observed. The attractive and repulsive forces are dependent on the distance between the particles, as well as the sign and magnitude of the charges on the individual particles. When the charges on the particles are opposite, they attract each other. If both particles have the same charge, they repel each other.
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Atomic Radii and Effective Nuclear Charge03:08

Atomic Radii and Effective Nuclear Charge

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The elements in groups of the periodic table exhibit similar chemical behavior. This similarity occurs because the members of a group have the same number and distribution of electrons in their valence shells.
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Electron Behavior00:54

Electron Behavior

98.1K
Overview
Electrons are negatively charged subatomic particles that are attracted to an orbit around the positively-charged nucleus of an atom. They reside in locations that are associated with energy levels called shells and are further organized into sub-shells and orbitals within each shell.
Electrons Orbit the Nucleus
Electrons are found in specific locations outside of the nucleus. The shell in which an electron resides indicates the general energy level of the electron: those closer to the...
98.1K
Electron Affinity03:07

Electron Affinity

35.0K
The electron affinity (EA) is the energy change for adding an electron to a gaseous atom to form an anion (negative ion).
35.0K
The Bohr Model02:18

The Bohr Model

49.4K
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...
49.4K
Nuclear Binding Energy02:13

Nuclear Binding Energy

12.0K
The difference between the calculated and experimentally measured masses is known as the mass defect of the atom. In the case of helium-4, the mass defect indicates a “loss” in mass of 4.0331 amu – 4.0026 amu = 0.0305 amu. The loss in mass accompanying the formation of an atom from protons, neutrons, and electrons is due to the conversion of that mass into energy that is evolved as the atom forms. The nuclear binding energy is the energy produced when the atoms’ nucleons...
12.0K

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相关实验视频

Updated: May 7, 2025

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−
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Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−

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低核电荷的双环电子自我能量

V A Yerokhin1, Z Harman1, C H Keitel1

  • 1<a href="https://ror.org/052d0h423">Max Planck Institute for Nuclear Physics</a>, Saupfercheckweg 1, D 69117 Heidelberg, Germany.

Physical review letters
|January 3, 2025
PubMed
概括
此摘要是机器生成的。

对于 1S Lamb 转移的新计算为电子自我能量提供了非常准确的结果. 这种改进的精度影响了莱德伯格常数,为提供了更精确的理论预测.

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Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures
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相关实验视频

Last Updated: May 7, 2025

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科学领域:

  • 原子物理 原子物理
  • 量子电动力学 量子电动力学

背景情况:

  • 羔羊转移是两个原子能级别,即2S1/2和2P1/2之间的能量差异很小,但很显著,在类似的原子中.
  • 对于测试基本物理和确定基本常数而言,对Lamb转移的准确理论计算至关重要.

研究的目的:

  • 为了执行 1S Lamb 转换的双循环电子自能的所有顺序计算.
  • 提高这些计算的数值准确性,并将其扩展到较低的核电荷.
  • 为了提供一个更精确的理论预测,为1S羊羔转移在及其对莱德伯格常数的影响.

主要方法:

  • 对核结合强度参数Zα的所有顺序进行计算.
  • 利用先进的计算技术,以提高数值准确度超过一个数量级.
  • 将所有顺序的结果推算到中性的具体情况.

主要成果:

  • 实现了1S Lamb转移的双循环电子自能计算,以前所未有的准确性.
  • 对的推算结果是以前值的两倍精确,差异为2.8标准偏差.
  • 转移了中1S-2S过渡频率的理论预测,将瑞德伯格常数减小1标准偏差.

结论:

  • 全顺序计算方法显著提高了Lamb变化预测的精度.
  • 改进的准确性提供了在强电场中更严格的量子电动力学 (QED) 测试.
  • 这项工作完善了瑞德伯格常数的理论值,影响了原子物理学和计量学.