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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
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: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.5K
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,...
1.5K
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)

1.5K
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
Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

5.0K
All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not contribute to...
5.0K

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Updated: Jan 26, 2026

Direct Imaging of Laser-driven Ultrafast Molecular Rotation
10:52

Direct Imaging of Laser-driven Ultrafast Molecular Rotation

Published on: February 4, 2017

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Lasers de espín ultrarrápidos

Markus Lindemann1, Gaofeng Xu2, Tobias Pusch3

  • 1Photonics and Terahertz Technology, Ruhr-Universität Bochum, Bochum, Germany. markus.lindemann@rub.de.

Nature
|April 5, 2019
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores desarrollaron un nuevo spin-laser que demuestra frecuencias de modulación de temperatura ambiente de más de 200 GHz. Este avance en los láseres semiconductores utiliza el giro del portador y la polarización de la luz para la comunicación óptica ultrarrápida.

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Área de la Ciencia:

  • Óptica y fotónica
  • Física de los semiconductores
  • La tecnología Spintronics

Sus antecedentes:

  • Los láseres son cruciales para las aplicaciones y el estudio de fenómenos complejos.
  • Spintronics aprovecha el giro y la carga de los electrones, lo que lleva a los láseres de espín.
  • Los láseres semiconductores convencionales se enfrentan a limitaciones de velocidad.

Objetivo del estudio:

  • Para demostrar experimentalmente el funcionamiento ultrarrápido en láseres de espín.
  • Para explorar el acoplamiento entre el giro del portador y la polarización de la luz.
  • Para superar las limitaciones de velocidad en los láseres semiconductores.

Principales métodos:

  • Utilizando láseres semiconductores comunes.
  • Aprovechando el acoplamiento entre el giro del portador y la polarización de la luz.
  • Investigando el papel del tiempo de relajación del giro del portador y la anisotropía del índice de refracción.

Principales resultados:

  • Se han logrado frecuencias de modulación de temperatura ambiente por encima de los 200 gigahertz.
  • Excedido velocidades láser semiconductor convencional por casi un orden de magnitud.
  • Se ha demostrado que los tiempos de relajación de giro cortos y una gran anisotropía del índice de refracción son beneficiosos.

Conclusiones:

  • Los láseres de espín ofrecen una vía para superar las limitaciones de velocidad en los láseres modulados directamente.
  • Esta tecnología promete una nueva generación de comunicaciones ópticas ultra rápidas y de bajo consumo energético.
  • Se obtuvieron nuevas ideas sobre el funcionamiento del láser y la espintrónica.