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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)

1.5K
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...
1.5K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.2K
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,...
1.2K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.2K
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...
1.2K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.5K
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...
3.5K
The Bohr Model02:18

The Bohr Model

68.0K
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...
68.0K
¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

2.4K
The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
2.4K

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将单个电子合到波斯-爱因斯坦凝结体中.

Jonathan B Balewski1, Alexander T Krupp, Anita Gaj

  • 15. Physikalisches Institut, Universität Stuttgart, Pfaffenwaldring 57, 70569 Stuttgart, Germany.

Nature
|November 1, 2013
PubMed
概括

一个单一的瑞德伯格电子与斯-爱因斯坦凝聚物相互作用,激发声子,引起集体振荡. 这种电子-物质合比离子更强,揭示了新的量子现象.

科学领域:

  • 量子物理学的量子物理学
  • 凝聚物质物理学 凝聚物质物理学
  • 原子物理 原子物理

背景情况:

  • 电子 - 声子合对材料特性如超导性至关重要.
  • 巴丁 - 库珀 - 施里弗超导产生于电子 - 声子相互作用形成库珀对.

研究的目的:

  • 研究单个局部电子与斯-爱因斯坦凝结体之间的相互作用.
  • 描述由此产生的电子 - 声子合和凝聚剂动态.

主要方法:

  • 形成一个Rydberg结合状态,其中单个电子由离子核局部化.
  • 观察电子与斯-爱因斯坦凝结物的相互作用.
  • 测量电子寿命和冷凝物反应.

主要成果:

  • 里德伯格电子激发声子,在凝聚物中诱导集体振荡.
  • 由于质量比,电子-凝聚物合明显比离子杂质更强.
  • 观察到的长电子寿命和有限尺寸效应归因于对凝聚物外围的探索.
  • 瑞德伯格电子波函数 (n=202) 延伸到8微米,包括数千个原子.

结论:

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  • 单个瑞德伯格电子可以强烈地对并影响波斯-爱因斯坦凝结体.
  • 这种有利的质量比增强了电子-声波合强度.
  • 未来的研究可以探索电子轨道成像,声子介导合和量子光学应用.