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関連する概念動画

The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

59.8K
The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
59.8K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.5K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.5K
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

2.4K
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.
2.4K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

2.1K
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...
2.1K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.5K
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
1.5K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

1.7K
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.7K

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関連する実験動画

Updated: Feb 22, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

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2次元フェルミ-ハバード系におけるスピン不均衡

Peter T Brown1, Debayan Mitra1, Elmer Guardado-Sanchez1

  • 1Department of Physics, Princeton University, Princeton, NJ 08544, USA.

Science (New York, N.Y.)
|October 1, 2017
PubMed
まとめ

研究者は磁場とドーピングで フェルミ-ハバードモデルを研究しました 彼らはアニゾトロピックな反鉄磁気相関と非単調な偏振を観察し,強固に相関するシステムにおける量子磁気と超伝導性の洞察を明らかにした.

さらに関連する動画

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

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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

Published on: March 30, 2017

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関連する実験動画

Last Updated: Feb 22, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

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Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
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Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

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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

Published on: March 30, 2017

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科学分野:

  • 凝縮物質物理学
  • 量子多体システム

背景:

  • 強い相互作用と磁場が 新しい量子現象を誘発する
  • 2次元のフェルミ・ハバードモデルは 強く相関するフェルミオンを理解する鍵です

研究 の 目的:

  • 実験的に調査する フェルミ-ハバードモデル ジーマンフィールドと様々なドーピングの下で
  • 磁気相関と分極の出現を明らかにする
  • 低温相図をマッピングする.

主な方法:

  • 2次元のフェルミ-ハバードモデルによる測定結果
  • ジーマン・フィールドの適用とドーピングの制御
  • 磁気相関と局所的偏振の分析

主要な成果:

  • アニゾトロプ的反鉄磁気相関が観察され,傾斜順序の先駆体を示した.
  • 強烈に相互作用するレジームでドーピングによる非単調な局所的偏極化行動が検出されました.
  • 反鉄磁気分離器から金属相への移行を特定した.

結論:

  • フェルミ・ハバードモデルの複雑な相図に関する実験的洞察
  • 量子システムにおける相互作用,磁場,ドーピングの相互作用を理解する.
  • エキゾチックな超伝導性と磁気のさらなる探査のための基盤です.