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Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

1.3K
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...
1.3K
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

1.4K
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.
1.4K
Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

3.8K
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...
3.8K
The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

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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:
56.5K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.1K
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,...
1.1K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

2.2K
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...
2.2K

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Updated: Oct 26, 2025

Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains
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Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains

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El hielo de espín de Qubit

Andrew D King1, Cristiano Nisoli2, Edward D Dahl3,4

  • 1D-Wave Systems, Burnaby, British Columbia V5G 4M9, Canada. aking@dwavesys.com cristiano@lanl.gov.

Science (New York, N.Y.)
|July 30, 2021
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores diseñaron hielo de espín artificial usando qubits superconductores, observando las fluctuaciones cuánticas y térmicas. Controlaron una fase de Coulomb y demostraron Gauss

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Área de la Ciencia:

  • Física de la materia condensada
  • Ciencia de la información cuántica
  • Nanotecnología

Sus antecedentes:

  • Los sistemas de hielo de espín artificial están diseñados como imanes frustrados que exhiben fenómenos emergentes.
  • El hielo de espín artificial convencional se basa en las interacciones magnéticas clásicas.
  • Los efectos cuánticos y las fluctuaciones térmicas pueden introducir nuevos comportamientos en tales sistemas.

Objetivo del estudio:

  • Para darse cuenta y caracterizar hielo de espín artificial en una red de qubits superconductores.
  • Investigar el papel de las fluctuaciones cuánticas y térmicas en un hielo basado en qubits.
  • Para demostrar el control sobre los fenómenos emergentes, incluyendo una fase de Coulomb y monopolos magnéticos.

Principales métodos:

  • Fabricación de una red de qubits superconductores diseñada para imitar el hielo de espín.
  • Utilizando las fluctuaciones cuánticas y térmicas para desordenar el sistema.
  • Control preciso de los qubits para manipular los estados de espín y sondear las propiedades emergentes.

Principales resultados:

  • Creó con éxito un sistema de hielo de espín artificial desordenado usando qubits superconductores.
  • Se observó un estado de base consistente con la regla clásica del hielo, modificado por fluctuaciones.
  • Logró el control de un punto de degeneración frágil, induciendo una fase de Coulomb.
  • Demostró la ley de Gauss para los monopolos magnéticos emergentes al fijar giros individuales.

Conclusiones:

  • Los qubits superconductores proporcionan una plataforma sintonizable para realizar y estudiar hielo de espín artificial.
  • El sistema exhibe fenómenos emergentes controlables, incluida una fase de Coulomb y monopolios efectivos.
  • Este trabajo allana el camino para explorar los líquidos de espín cuántico y los fenómenos topológicos en sistemas de ingeniería.