Jove
Visualize
Contáctanos

Videos de Conceptos Relacionados

The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

59.8K
The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
59.8K
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
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

2.4K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
2.4K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

2.1K
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 one, the...
2.1K
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)

1.7K
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...
1.7K

También podría leer

Artículos Relacionados

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

Ordenar por
Same author

A physics-informed alternative to Richardson-Lucy deconvolution across SNR regimes without iteration cutoffs.

Nature communications·2026
Same author

Magneto-Optical Trapping of a Metal Hydride Molecule.

Physical review letters·2026
Same author

Enhancement of Curie temperature in ferromagnetic insulator-topological insulator heterostructures.

Reports on progress in physics. Physical Society (Great Britain)·2026
Same author

Chemistry in a Cryogenic Buffer Gas Cell.

The journal of physical chemistry letters·2025
Same author

Detection of anyon braiding through pump-probe spectroscopy.

Proceedings of the National Academy of Sciences of the United States of America·2025
Same author

Fourier synthesis optical diffraction tomography for kilohertz rate volumetric imaging.

Science advances·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: Feb 22, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

8.7K

Desequilibrio de espín en un sistema Fermi-Hubbard en 2D

Peter T Brown1, Debayan Mitra1, Elmer Guardado-Sanchez1

  • 1Department of Physics, Princeton University, Princeton, NJ 08544, USA.

Science (New York, N.Y.)
|October 1, 2017
PubMed
Resumen

Los investigadores estudiaron el modelo de Fermi-Hubbard con los campos magnéticos y el dopaje. Observaron correlaciones antiferromagnéticas anisotrópicas y polarización no monótona, revelando conocimientos sobre el magnetismo cuántico y la superconductividad en sistemas fuertemente correlacionados.

Más Videos Relacionados

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

10.5K
Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

7.9K

Videos de Experimentos Relacionados

Last Updated: Feb 22, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

8.7K
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

10.5K
Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

7.9K

Área de la Ciencia:

  • Física de la materia condensada
  • Sistemas cuánticos de muchos cuerpos

Sus antecedentes:

  • Las fuertes interacciones y los campos magnéticos impulsan nuevos fenómenos cuánticos.
  • El modelo bidimensional de Fermi-Hubbard es clave para comprender los fermiones fuertemente correlacionados.

Objetivo del estudio:

  • Para investigar experimentalmente el modelo de Fermi-Hubbard bajo campos de Zeeman y variando el dopaje.
  • Para revelar la aparición de las correlaciones magnéticas y la polarización.
  • Para mapear el diagrama de fase a baja temperatura.

Principales métodos:

  • Medidas resueltas en el sitio en el modelo bidimensional de Fermi-Hubbard.
  • Aplicación de un campo de Zeeman y dopaje controlado.
  • Análisis de las correlaciones magnéticas y la polarización local.

Principales resultados:

  • Se observaron correlaciones anisotrópicas antiferromagnéticas, lo que indica un precursor del orden de inclinación.
  • Se detectó un comportamiento de polarización local no monótono con dopaje en regímenes de interacción fuerte.
  • Identificó una transición del aislante antiferromagnético a la fase metálica.

Conclusiones:

  • Perspectivas experimentales en el complejo diagrama de fase del modelo de Fermi-Hubbard.
  • Comprender la interacción de las interacciones, los campos magnéticos y el dopaje en los sistemas cuánticos.
  • Fundación para una mayor exploración de la superconductividad y el magnetismo exóticos.