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相关概念视频

Carbon-13 (¹³C) NMR: Overview01:10

Carbon-13 (¹³C) NMR: Overview

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Carbon-13 is a naturally occurring NMR-active isotope of carbon with a low natural abundance of 1.1%. In contrast, carbon-12 is the most abundant isotope of carbon with zero nuclear spin. Therefore, it is NMR inactive. The gyromagnetic ratio of carbon-13 is smaller than that of protons. As a result, carbon-13 resonance is about 6000 times weaker than proton resonance. For a given magnetic field strength, the resonance frequency of carbon-13 is about one-fourth of the resonance frequency for...
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¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

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The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.7K
Properties of Organometallic Compounds01:23

Properties of Organometallic Compounds

1.6K
Organometallic compounds are compounds that contain a carbon–metal bond. Carbon belongs to an organyl group like alkyl, aryl, allyl, or benzyl groups. The metal can be from Group I or Group II of the periodic table, a transition metal, or a semimetal.
1.6K
Ferromagnetism01:31

Ferromagnetism

2.9K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
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Paramagnetism01:30

Paramagnetism

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Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
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π Electron Effects on Chemical Shift: Overview01:27

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An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
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AM-C33:一种改变磁性的碳.

Mingqing Liao1, Yuehua Wang1, Pengcheng Ye1

  • 1School of Materials Science and Engineering, Jiangsu University of Science and Technology Zhenjiang 212100 China mingqing_liao@just.edu.cn fjwang@just.edu.cn.

Chemical science
|November 5, 2025
PubMed
概括

研究人员推出了AM-C33,这是一种基于3D碳的p电子变磁体. 这种材料为自旋电子设备提供了有前途的性能,结合了铁磁和反铁磁的优势.

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科学领域:

  • 凝聚物质物理学 凝聚物质物理学
  • 材料科学 材料科学 材料科学
  • 量子化学 是一个量子化学.

背景情况:

  • 变磁材料将铁磁自旋分裂与反铁磁稳定性相结合.
  • p电子自旋电子材料提供了长时间的自旋连贯性和寿命.
  • 之前没有实现过3Dp电子变磁体.

研究的目的:

  • 从理论上提出和描述一个新的3Dp电子变磁半导体.
  • 探索基于碳的材料对变磁的潜力.
  • 调查拟议材料的可调性和功能.

主要方法:

  • 使用了第一原则计算.
  • 分析了电子带结构和磁性特性.
  • 模拟了应变工程效应.

主要成果:

  • 一个完全基于碳的p电子变磁半导体AM-C33被提出.
  • AM-C33的带隙为0.52 eV,旋转分裂为0.31 eV,过渡温度为121.5 K.
  • 应变工程允许调整带隙和旋转分裂,并确定了具有独特功能的元稳定相.

结论:

  • 这项工作为设计3Dp电子替代磁体提供了一个有前途的途径.
  • 拟议的AM-C33推进了用于自旋电子的碳基变磁材料.
  • 该材料的调节性质和多样化的功能为设备应用开辟了新的途径.