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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

54.8K
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.
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The de Broglie Wavelength02:32

The de Broglie Wavelength

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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...
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Fermi Level Dynamics01:12

Fermi Level Dynamics

465
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...
465
Equilibrium Conditions for a Particle01:23

Equilibrium Conditions for a Particle

1.9K
When an object is in equilibrium, it is either at rest or moving with a constant velocity. There are two types of equilibrium: static and dynamic. Static equilibrium occurs when an object is at rest, while dynamic equilibrium occurs when an object is moving with a constant velocity. In both cases, there must be a balance of forces acting on the object.
To understand the concept of equilibrium, let us first consider the forces acting on an object. When different forces act on an object, they can...
1.9K
The Bohr Model02:18

The Bohr Model

77.7K
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...
77.7K
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

910
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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Gradient Echo Quantum Memory in Warm Atomic Vapor
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誘導されたライドバーグ原子配列における量子多体ダイナミクスの制御

D Bluvstein1, A Omran1,2, H Levine1

  • 1Department of Physics, Harvard University, Cambridge, MA 02138, USA.

Science (New York, N.Y.)
|February 26, 2021
PubMed
まとめ
この要約は機械生成です。

研究者は 周期的な駆動を使って 相互作用する量子ビットの 量子多体傷跡を安定させました この方法は複雑な量子力学を制御し,量子情報科学の応用の可能性を示しています.

さらに関連する動画

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

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Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Generation and Coherent Control of Pulsed Quantum Frequency Combs

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関連する実験動画

Last Updated: Nov 16, 2025

Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

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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

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Generation and Coherent Control of Pulsed Quantum Frequency Combs
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科学分野:

  • 量子物理学
  • 多体システム
  • 量子力学について

背景:

  • 多体系における非均衡量子力学を制御することは,熱化により困難である.
  • 量子システムの相互作用はしばしばヒルベルト空間で混沌とした拡散につながります.

研究 の 目的:

  • 強烈に相互作用する量子ビットシステムにおける急速な消火後の非均衡のダイナミクスを調査する.
  • 量子多体傷を安定させる方法を探る

主な方法:

  • プログラム可能な量子シミュレータを リッドバーグの原子配列で使った
  • 3から200の量子ビットの多体システムに 周期的なドライビングを適用した.
  • 1次元と2次元でシステムを研究した.

主要な成果:

  • 量子多体傷跡と結びついた 協調的な復活の安定化が証明された
  • 固いサブハーモニー反応を観察した 分離した時間結晶の順番に似ています
  • ヒルベルト空間ダイナミクス,幾何学,相図,およびシステムサイズ依存性をマッピングした.

結論:

  • 周期的な運転は 多体システムにおける複雑なダイナミクスを制御する 新しい方法を提供します
  • この量子ダイナミクスの制御は 量子情報科学に潜在的応用があります