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関連する概念動画

The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

56.1K
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 hydrogen spectra.
56.1K
The Bohr Model02:18

The Bohr Model

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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 the...
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The de Broglie Wavelength02:32

The de Broglie Wavelength

32.6K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
32.6K
Phase Transitions: Melting and Freezing02:39

Phase Transitions: Melting and Freezing

14.4K
Heating a crystalline solid increases the average energy of its atoms, molecules, or ions, and the solid gets hotter. At some point, the added energy becomes large enough to partially overcome the forces holding the molecules or ions of the solid in their fixed positions, and the solid begins the process of transitioning to the liquid state or melting. At this point, the temperature of the solid stops rising, despite the continual input of heat, and it remains constant until all of the solid is...
14.4K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

1.8K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
1.8K
Phase Transitions: Vaporization and Condensation02:39

Phase Transitions: Vaporization and Condensation

20.3K
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 molecules...
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Updated: Jun 16, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

冷たい原子と量子制御について

Steven Chu1

  • 1Physics Department, Stanford University, Stanford, California 94305-4060, USA.

Nature
|March 15, 2002
PubMed
まとめ
この要約は機械生成です。

このコレクションは,原子の性質を制御するための重要な技術であるレーザー冷却と原子の罠を調査しています. それは,原子物理学と分子制御の進歩のための歴史的文脈を提供します.

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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Gradient Echo Quantum Memory in Warm Atomic Vapor
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Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 12, 2013

関連する実験動画

Last Updated: Jun 16, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 12, 2013

科学分野:

  • 原子物理 原子物理学
  • 量子力学は,量子力学という
  • レーザースペクトロスコピーは,

背景:

  • レーザー冷却とトラッピングは,原子物理学における重要な進歩を表しています.
  • 原子と分子の内部と外部の自由度の制御は,長年の研究目標である.

研究 の 目的:

  • レーザー冷却とトラッピングに関する歴史的視点を提供するためです.
  • 原子および分子制御におけるより広範な研究活動の中で,レーザー冷却とトラッピングを文脈化します.

主な方法:

  • レーザー冷却とトラッピング技術の歴史的レビュー.
  • 原子と分子の自由度制御のための研究方向の分析.

主要な成果:

  • レーザー冷却とトラッピングは,原子操作における重要な発展として提示されます.
  • 概要は,原子や分子に対する正確な制御のための技術の進化を強調しています.

結論:

  • レーザー冷却とトラッピングは原子物理学に大きな影響を与えました.
  • この研究は,原子や分子システムに対する洗練された制御のための継続的な探求を強調しています.