関連する実験動画
Updated: May 1, 2026

11:21
Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
Published on: March 30, 2017
7.1K
ガス相のエルビウム原子の超寒冷衝突による量子カオス
Albert Frisch1, Michael Mark1, Kiyotaka Aikawa1
1Institut für Experimentalphysik, Universität Innsbruck, 6020 Innsbruck, Austria.
Nature
|March 28, 2014
まとめ
1マイクロケルビン以下に冷却された超冷たい原子ガスは,混沌としたダイナミクスを明らかにします. エルビウム原子の実験ではランダムなファノ-フェシュバッハ共振スペクトルが示され,原子相互作用における混沌とした振る舞いを確認した.
科学分野:
- 原子物理学 原子物理学とは
- 超冷たい量子ガスが存在する.
- 量子的なカオスです.
背景:
- 超冷たい原子および分子サンプルは,粒子相互作用を研究するために高エネルギー解像度を提供します.
- ランタナイド原子や分子のような複雑な種は,超冷たい物理学の研究に参入しています.
- 分子衝突の横断面におけるランダムな変動は,その背後にある混沌としたダイナミクスを示唆している.
研究 の 目的:
- 超冷たい原子系におけるランダムスペクトルを実験的に実証する.
- 複雑な原子における散乱共鳴の統計的性質を調査する.
- 超冷たい物質の混沌とした行動の影響を調査する.
主な方法:
- 原子や分子サンプルを1マイクロケルビン以下まで冷却する.
- 磁場を正確に制御して共振散乱を誘発する.
- 超冷たいエルビウムガスのファノ=フェシュバッハ共鳴の統計分布を分析した.
主要な成果:
- 超冷たい原子ガスのランダムスペクトルの存在を証明した.
- エルビウム原子におけるファノ=フェシュバッハ共鳴の高密度 (約. ボゾンでは1ガウスあたり3です).
- 共振統計がランダムマトリックス理論の予測と一致していることを確認しました.
結論:
- 超冷たいエルビウム原子は,本来の相互作用で混沌とした行動を示す.
- 観測されたランダムスペクトルは,原子の潜在エネルギー表面のアニソトロピーから生じる.
- この発見は,超冷たい原子・分子相互作用と潜在的な混沌状態を理解するための新しい理論的アプローチを必要とします.
関連する概念動画
The de Broglie Wavelength
25.7K
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...
25.7K
The Quantum-Mechanical Model of an Atom
47.1K
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...
47.1K
Electron Configuration of Multielectron Atoms
57.4K
The alkali metal sodium (atomic number 11) has one more electron than the neon atom. This electron must go into the lowest-energy subshell available, the 3s orbital, giving a 1s22s22p63s1 configuration. The electrons occupying the outermost shell orbital(s) (highest value of n) are called valence electrons, and those occupying the inner shell orbitals are called core electrons. Since the core electron shells correspond to noble gas electron configurations, we can abbreviate electron...
57.4K
The Uncertainty Principle
25.6K
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...
25.6K
The Bohr Model
67.8K
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...
67.8K
Electron Paramagnetic Resonance (EPR) Spectroscopy: Organic Radicals
2.6K
Ideally, an unpaired electron shows a single peak in the EPR spectrum due to the transition between the two spin energy states. However, coupling interactions can occur between the spins of the unpaired electron and any neighboring spin-active nuclei. This hyperfine coupling results in hyperfine splitting, where the EPR signal is split into multiplets. The signals split into 2nI + 1 peaks, where n is the number of equivalent nuclei and I is the nuclear spin. These splitting patterns provide...
2.6K

