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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: Three-Bond Coupling (Vicinal Coupling)01:22

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

1.4K
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...
1.4K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.4K
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...
1.4K
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

2.9K
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...
2.9K
Three-Winding Transformers01:19

Three-Winding Transformers

648
Three identical single-phase transformers can be configured to form a three-phase transformer connection, which involves high-voltage and low-voltage windings. The high-voltage windings are denoted by capital letters A-B-C, while the low-voltage windings are labeled with lowercase letters a-b-c, representing their respective phases. This notation helps distinguish between the high and low voltage sides of the transformer.
In the per-unit equivalent circuit of a grounded Y-Y three-phase...
648

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绕合阶段用于伪旋转衍生的拓光子学.

Tianyuan Liu1,2, Min Qiu3,4,5, Wei Yan6,7

  • 1College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou, Zhejiang, China.

Nature communications
|December 24, 2025
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概括

这项研究引入了一个新的理论框架,用于设计伪旋转拓相,使用光子晶体中的 evanescent 合. 它使新的旋转谷霍尔阶段和边缘状态能够在不打破时间逆向对称的情况下实现.

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科学领域:

  • 拓式光子学 拓式光子学
  • 凝聚物质物理学 凝聚物质物理学
  • 材料科学是一种材料科学.

背景情况:

  • 拓相通常依赖于旋转轨道相互作用或反铁磁.
  • 设计伪旋转衍生的拓阶段需要灵活的理论框架.

研究的目的:

  • 提出一个灵活的理论框架来设计伪旋转衍生的拓阶段.
  • 在光子晶体中探索新的拓阶段和边缘状态.
  • 为了证明这些现象的实用在绝缘体设计.

主要方法:

  • 开发基于共振器之间的 evanescent 合的理论框架.
  • 使用量子化合绕数来描述拓.
  • 设计光子晶体与量身定制的合线数.
  • 建议在绝缘体 (SOI) 装置设计.

主要成果:

  • 进化合表现出具有量子化合绕数的 $\pi_1(S^1) $ 拓.
  • 演示了旋转谷霍尔相 (SVHP),异常霍尔相和反螺旋边缘状态的设计.
  • 在非反磁磁系统中,在没有时间逆转对称性破坏的情况下实现 SVHP.
  • 设计的反螺旋边缘状态独立于下一个最接近的合.

结论:

  • 拟议的框架为设计伪旋转拓阶段提供了一种多功能和简单的方法.
  • 结果与传统的制造工艺相兼容.
  • 潜在的应用包括自旋谷保护的光传输和缓慢的光导.