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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...
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The Uncertainty Principle04:08

The Uncertainty Principle

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Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He...
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The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

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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...
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Atomic Nuclei: Nuclear Relaxation Processes01:23

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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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Electron Behavior01:09

Electron Behavior

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Electrons are negatively charged subatomic particles attracted to and orbit around the positively-charged nucleus of an atom. They reside in spaces associated with energy levels called shells and are further organized into subshells 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 nucleus have less energy,...
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Fermi Level Dynamics01:12

Fermi Level Dynamics

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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.
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関連する実験動画

Updated: May 1, 2026

Setting Limits on Supersymmetry Using Simplified Models
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ポリクロマティック時間摂動下におけるハーパーモデルの量子拡散

Hiroaki S Yamada1, Kensuke S Ikeda2

  • 1Yamada Physics Research Laboratory, Aoyama 5-7-14-205, Niigata 950-2002, Japan.

Physical review. E
|February 20, 2026
PubMed
まとめ
この要約は機械生成です。

ハーパーモデルに複数の周波数を追加すると、局在状態が量子拡散状態へと変換される。3つ以上の非可測周波数の場合、拡散への遷移は摂動強度が増加するにつれて発生する。

キーワード:
量子拡散ハーパーモデル時間依存摂動非可測周波数位相図

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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

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科学分野:

  • 量子力学
  • 物性物理学

背景:

  • ハーパーモデルは磁場中の量子ダイナミクスを記述する。
  • その状態は、ポテンシャル強度(V)の影響を受けて、局在、拡散、またはボールリスティックになり得る。

研究 の 目的:

  • 時間依存調和摂動がハーパーモデルのダイナミクスに及ぼす影響を調査する。
  • 異なる量子状態が拡散状態へと遷移する条件を決定する。

主な方法:

  • M個の非可測周波数を持つ時間依存調和摂動をハーパーモデルに適用する。
  • 結果として生じる量子ダイナミクスと状態遷移を分析する。
  • (ε,V)パラメータ空間における位相図をマッピングする。

主要な成果:

  • M≥3の場合、摂動強度(ε)が増加するにつれて、すべてのハーパーモデルの状態が量子拡散状態へと遷移する。
  • 遷移スキームと拡散挙動は、εとVに依存する。
  • これらの遷移を示す位相図を提示する。

結論:

  • 十分な非可測周波数を持つ時間依存摂動は、局在のない量子拡散を駆動することができる。
  • ハーパーモデルのダイナミクスは、外部の時間依存摂動に非常に敏感である。