Jove
Visualize
Contáctanos

Videos de Conceptos Relacionados

Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

980
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...
980
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

1.1K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of...
1.1K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

1.1K
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...
1.1K
Induced Electric Dipoles01:28

Induced Electric Dipoles

4.3K
A permanent electric dipole orients itself along an external electric field. This rotation can be quantified by defining the potential energy because the external torque does work in rotating it. Then, the potential energy is minimum at the parallel configuration and maximum at the antiparallel configuration. While the former is a stable equilibrium, the latter is an unstable equilibrium.
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
4.3K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

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

Spin–Spin Coupling: One-Bond Coupling

1.0K
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,...
1.0K

También podría leer

Artículos Relacionados

Artículos vinculados a este trabajo por autores compartidos, revista y gráfico de citas.

Ordenar por
Same author

Lunar silicon cavity.

Proceedings of the National Academy of Sciences of the United States of America·2026
Same author

Frequency reproducibility of solid-state thorium-229 nuclear clocks.

Nature·2026
Same author

Fine-structure constant sensitivity of the Th-229 nuclear clock transition.

Nature communications·2025
Same author

Coherent evolution of superexchange interaction in seconds-long optical clock spectroscopy.

Science (New York, N.Y.)·2025
Same author

Observation of generalized <i>t-J</i> spin dynamics with tunable dipolar interactions.

Science (New York, N.Y.)·2025
Same author

Temperature Sensitivity of a Thorium-229 Solid-State Nuclear Clock.

Physical review letters·2025
JoVE
x logofacebook logolinkedin logoyoutube logo
ACERCA DE JoVE
Visión GeneralLiderazgoBlogCentro de Ayuda JoVE
AUTORES
Proceso de PublicaciónConsejo EditorialAlcance y PolíticasRevisión por ParesPreguntas FrecuentesEnviar
BIBLIOTECARIOS
TestimoniosSuscripcionesAccesoRecursosConsejo Asesor de BibliotecasPreguntas Frecuentes
INVESTIGACIÓN
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchivo
EDUCACIÓN
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualCentro de Recursos para ProfesoresSitio de Profesores
Términos y Condiciones de Uso
Política de Privacidad
Políticas

Video Experimental Relacionado

Updated: Aug 12, 2025

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

10.0K

Dinámica de espín itinerante ajustable con moléculas polares

Jun-Ru Li1, Kyle Matsuda2, Calder Miller2

  • 1JILA, National Institute of Standards and Technology and Department of Physics, University of Colorado, Boulder, CO, USA. junru.li@colorado.edu.

Nature
|February 1, 2023
PubMed
Resumen

Los investigadores desarrollaron un sistema de espín cuántico controlable utilizando moléculas de potasio y rubidio. Esta plataforma permite la exploración de la dinámica de espín de muchos cuerpos y la física del movimiento de espín a través de interacciones dipolares sintonizables.

Más Videos Relacionados

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

Direct Imaging of Laser-driven Ultrafast Molecular Rotation

Published on: February 4, 2017

9.8K
Dissolution Dynamic Nuclear Polarization Instrumentation for Real-time Enzymatic Reaction Rate Measurements by NMR
10:54

Dissolution Dynamic Nuclear Polarization Instrumentation for Real-time Enzymatic Reaction Rate Measurements by NMR

Published on: February 23, 2016

10.7K

Videos de Experimentos Relacionados

Last Updated: Aug 12, 2025

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

10.0K
Direct Imaging of Laser-driven Ultrafast Molecular Rotation
10:52

Direct Imaging of Laser-driven Ultrafast Molecular Rotation

Published on: February 4, 2017

9.8K
Dissolution Dynamic Nuclear Polarization Instrumentation for Real-time Enzymatic Reaction Rate Measurements by NMR
10:54

Dissolution Dynamic Nuclear Polarization Instrumentation for Real-time Enzymatic Reaction Rate Measurements by NMR

Published on: February 23, 2016

10.7K

Área de la Ciencia:

  • La física cuántica
  • Física atómica, molecular y óptica
  • Física de la materia condensada

Sus antecedentes:

  • Los espines que interactúan fuertemente son fundamentales para el magnetismo y el procesamiento de información cuántica.
  • Los giros que interactúan con el movimiento exhiben fenómenos exóticos como la superfluidez de espín.
  • Los sistemas de espín interactivos controlables son cruciales para el estudio de la dinámica de espín compleja.

Objetivo del estudio:

  • Demostrar una plataforma altamente controlable para el estudio de la dinámica de giro itinerante.
  • Para aprovechar las interacciones dipolares sintonizables en las moléculas de potasio-rubidio para el control de espín cuántico.

Principales métodos:

  • Codificación de un sistema de espín-1/2 en los niveles de rotación molecular de las moléculas de potasio-rubidio.
  • Confinar las moléculas a los planos bidimensionales para mejorar las interacciones dipolares.
  • Ajuste preciso de las interacciones de Ising y de intercambio de espín utilizando campos eléctricos y estados moleculares.

Principales resultados:

  • Dinámica de giro itinerante sintonizable impulsada por las interacciones dipolares.
  • Cambios observados en las frecuencias de transición de rotación y la dinámica acoplada de giro-movimiento.
  • Se ha logrado la plena sintonizabilidad del hamiltoniano de espín, lo que permite la inversión de la dinámica de espín coherente.

Conclusiones:

  • Estableció una nueva plataforma de giro interactivo con interacciones dipolares fuertes y sintonizables.
  • Esta plataforma facilita la exploración de la dinámica de espín de muchos cuerpos y la física del movimiento de espín.
  • Permite la investigación avanzada en el magnetismo cuántico y el procesamiento de información cuántica.