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相关概念视频

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

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

1.6K
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...
1.6K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.4K
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,...
1.4K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.0K
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...
3.0K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

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

1.5K
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 involved orbitals. The...
1.5K
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
Potential Due to a Polarized Object01:29

Potential Due to a Polarized Object

726
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
726

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Updated: Jan 17, 2026

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
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双极化干扰仪使用自旋轨道光束.

Anuj Maurya, P Senthilkumaran

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    此摘要是机器生成的。

    这项研究引入了一种能够使用Fizeau和螺旋配置的双干扰仪. 这项创新简化了通过使用旋转轨道光束来区分山峰和山谷的表面造型.

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    科学领域:

    • 光学计量学是指光学计量学.
    • 干涉测量是干涉测量的方法.
    • 波浪分析的波浪分析.

    背景情况:

    • 精确的表面造型在计量学中至关重要.
    • 在传统的干涉测量中,区分地表峰和谷 (峰谷退化) 是一个挑战.
    • 现有的干扰测量技术可能需要复杂的设置或多次测量.

    研究的目的:

    • 为了推出一种新的双干扰仪.
    • 展示一种方法,以提升在表面造型中的峰谷退化.
    • 为了提高表面计量学的方便性和准确性.

    主要方法:

    • 开发一种可在Fizeau和螺旋配置之间切换的双干扰仪.
    • 使用旋转轨道光束来实现双重功能.
    • 使用偏振选择来控制干扰仪的模式.
    • 使用作为测试对象来分析表面极端的演示.

    主要成果:

    • 双干扰仪成功地提供了Fizeau和螺旋边缘图案.
    • 可获得测试波面的相位和相位梯度分布.
    • 峰谷退化被有效地解除,简化了表面造型.
    • 干扰仪的双重性质通过极化控制来证明.

    结论:

    • 开发的双干扰仪为表面分析提供了一种简化的方法.
    • 能够切换配置和解除峰谷退化的能力增强了计量能力.
    • 旋转轨道光束为先进的干扰度应用提供了一个多功能工具.