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Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

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

Atomic Nuclei: Nuclear Spin State Overview

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

Atomic Nuclei: Nuclear Spin State Population Distribution

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.
¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule01:10

Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule

In the AX proton spin system, proton A can sense the two spin states of a coupled proton X, resulting in a doublet NMR signal with two peaks of equal (1:1) intensity. When proton A is coupled to two equivalent protons (AX2 spin system), the spin states of each X can be aligned with or against the external field, creating three possible scenarios. This results in a 1:2:1  triplet signal, where the central peak corresponds to the chemical shift of A and is twice as large or intense as the others.
Thomson's e/m Experiment01:19

Thomson's e/m Experiment

In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The magnetic...

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Video Experimental Relacionado

Updated: Jul 8, 2026

Three-dimensional Particle Tracking Velocimetry for Turbulence Applications: Case of a Jet Flow
13:02

Three-dimensional Particle Tracking Velocimetry for Turbulence Applications: Case of a Jet Flow

Published on: February 27, 2016

Vórtice cuántico doble en el superfluido 3He-A.

Blaauwgeers1, Eltsov, Krusius

  • 1Low Temperature Laboratory, Helsinki University of Technology, Finland.

Nature
|April 13, 2000
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores proporcionan evidencia directa de líneas de vórtice doblemente cuantizadas en el superfluido Helio-3. Estos defectos topológicos, cruciales en los sistemas cuánticos, exhiben una estructura continua única y se forman periódicamente, desafiando la comprensión previa de los vórtices cuantificados.

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Área de la Ciencia:

  • Física de la materia condensada Física de la materia condensada
  • Los fluidos cuánticos son fluidos cuánticos.
  • Defectos topológicos Defectos topológicos

Sus antecedentes:

  • Los defectos lineales, como las cuerdas cósmicas y las líneas de flujo cuantizado, son frecuentes en varios sistemas físicos.
  • Las líneas de vórtice cuantizadas, típicamente cuantizadas individualmente (n = 1), son comunes en superfluidos y condensados de Bose-Einstein.
  • Las predicciones teóricas sugirieron la posibilidad de líneas de vórtice doblemente cuantificadas (n = 2) con estructura continua en el superfluido Helio-3-A.

Objetivo del estudio:

  • Verificar experimentalmente la existencia y la naturaleza de las líneas de vórtice predichas doblemente cuantizadas en el superfluido Helio-3-A.
  • Caracterizar la estructura y el mecanismo de formación de estos nuevos defectos topológicos.

Principales métodos:

  • Utilizando mediciones de resonancia magnética nuclear (RMN) de alta resolución.
  • Observando la formación y el comportamiento de las líneas de vórtice en el superfluido Helio-3-A.

Principales resultados:

  • Pruebas experimentales directas confirman que la línea de vórtice más común en el superfluido Helio-3-A es de hecho doblemente cuantizada (n=2).
  • Las líneas de vórtice observadas exhiben una estructura continua, con la orientación del parámetro de orden cambiando suavemente.
  • La formación de líneas de vórtice ocurre en un proceso regular y periódico, análogo a los deslizamientos de fase del efecto Josephson.

Conclusiones:

  • El estudio proporciona la primera evidencia directa de líneas de vórtice doblemente cuantizadas en el superfluido Helio-3-A.
  • Estos hallazgos validan las predicciones teóricas y ofrecen nuevos conocimientos sobre el comportamiento de los defectos topológicos en fluidos cuánticos.
  • El mecanismo de formación periódica sugiere nuevas dinámicas para estas complejas estructuras cuánticas.