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関連する概念動画

Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

2.6K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

1.4K
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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Atomic Nuclei: Larmor Precession Frequency01:11

Atomic Nuclei: Larmor Precession Frequency

3.5K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
3.5K
The Bohr Model02:18

The Bohr Model

83.0K
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...
83.0K
Magnetic Moment of an Electron01:23

Magnetic Moment of an Electron

3.2K
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
3.2K
Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

12.2K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
12.2K

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A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
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A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

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ボーゼ-アインシュタイン凝縮物におけるベル相関

Roman Schmied1, Jean-Daniel Bancal2, Baptiste Allard1

  • 1Quantum Atom Optics Laboratory, Department of Physics, University of Basel, Klingelbergstrasse 82, 4056 Basel, Switzerland.

Science (New York, N.Y.)
|April 23, 2016
PubMed
まとめ
この要約は機械生成です。

研究者は480個のボース・アインシュタイン凝縮体で 絡み合いを超えたベル相関を検出しました これは,最も強い量子相関が多体系で実験的に利用可能であることを示しています.

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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関連する実験動画

Last Updated: Mar 22, 2026

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
07:56

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

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

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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科学分野:

  • 量子物理学
  • 原子物理学
  • 凝縮物質物理学

背景:

  • 量子相関を特徴づけるのは 多体系を理解するために重要です
  • 量子相関はよく知られていますが より強い形もあります
  • ボーゼ-アインシュタイン凝縮体は 量子現象を研究するためのプラットフォームを提供します

研究 の 目的:

  • 多体系における量子相関のより強い形であるベル相関を検知し特徴づけること.
  • 可能な限り強い非古典的相関の実験的アクセシビリティを証明する.

主な方法:

  • 多くの粒子ベルの不等式からベルの相関証の導出.
  • 約480個のボース・アインシュタイン凝縮体におけるスピン相関の測定.
  • 感度を増やすため,スピン圧縮状態を使用します.

主要な成果:

  • ボーゼ-アインシュタイン凝縮物における原子スピンの間のベル相関の検出.
  • 測定は3.8標準偏差でベルの相関値を超えました.
  • 観察された相関は典型的な絡み合いよりも強いものでした.

結論:

  • ベル相関は多体系では実験的に利用できる.
  • 集団的な測定はこれらの強い非古典的な相関を明らかにすることができます.
  • これはマクロの量子システムにおける量子現象の探索に 新たな道を開きます