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相关概念视频

Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

941
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...
941
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

1.0K
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...
1.0K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)

1.1K
Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the...
1.1K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

990
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,...
990
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

1.4K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
1.4K

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相关实验视频

Updated: Jul 12, 2025

Fabrication and Operation of a Nano-Optical Conveyor Belt
11:10

Fabrication and Operation of a Nano-Optical Conveyor Belt

Published on: August 26, 2015

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基于伪旋转轨道合的矢量束操纵,使用电磁诱导透明度.

Lu Zhao

    Optics express
    |October 20, 2023
    PubMed
    概括

    这项研究引入了在电磁诱导透明度 (EIT) 系统中向量束演变的新模型. 它展示了伪旋转轨道合如何控制光极化,用于先进的信息处理.

    科学领域:

    • 量子光学是一种量子光学.
    • 原子,分子和光学物理学

    背景情况:

    • 电磁诱导透明度 (EIT) 为控制光传播提供了量子连贯效应.
    • 高序点卡雷球 (HOPS) 框架为矢量束极化状态提供了几何描述.

    研究的目的:

    • 在三脚 EIT 系统中研究矢量束对轴演变的总体范式.
    • 为分析光的自旋轨道合和不可分离性引入量子光学类比.

    主要方法:

    • 使用EIT模型和HOPS框架.
    • 开发一个一般化的保利式方程与旋转不变.
    • 引入伪旋转轨道合 (PSOC) 并分析其真实和想象中的潜力.

    主要成果:

    • 在光中证明了PSOC和旋转轨道不可分离性的共存.
    • 展示了PSOC潜力的关键作用,以控制整个HOPS的矢量束状态.
    • 通过不同的PSOC系数对传输极化方向和圆度的图示修改.

    结论:

    • 提出了一个全光学方案,以灵活地在连贯的介质中调整空间变量极化.
    • 突出了可调节的空间极化多重复合在信息处理中的潜在实用性,包括量子应用.

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