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Ferromagnetism01:31

Ferromagnetism

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Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
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Paramagnetism01:30

Paramagnetism

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Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
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Diamagnetism01:26

Diamagnetism

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Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
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Magnetism01:30

Magnetism

6.2K
Magnets are commonly found in everyday objects, such as toys, hangers, elevators, doorbells, and computer devices. Experimentation on these magnets shows that all magnets have two poles: one is labeled north (N) and the other south (S). Magnetic poles repel if they are alike and attract if unlike. Moreover, both poles of a magnet attract unmagnetized pieces of iron.
An individual magnetic pole cannot be isolated. No matter how small, every piece of a magnet contains a north pole and a south...
6.2K
Potential Due to a Magnetized Object01:24

Potential Due to a Magnetized Object

261
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
261
Magnetic Moment of an Electron01:23

Magnetic Moment of an Electron

1.1K
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
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Updated: Jun 3, 2025

Author Spotlight: Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
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El altermagnetismo: una perspectiva química

Shannon S Fender1, Oscar Gonzalez1, D Kwabena Bediako1,2

  • 1Department of Chemistry, University of California, Berkeley, California 97420, United States.

Journal of the American Chemical Society
|January 9, 2025
PubMed
Resumen

Los altermagnetos son nuevos materiales magnéticos con una magnetización neta cero pero con propiedades electrónicas únicas. Su potencial para la conversión de carga a espín los hace prometedores para la espintrónica.

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Área de la Ciencia:

  • Física de la materia condensada
  • Ciencias de los materiales
  • Química Cuántica

Sus antecedentes:

  • Los altermagnetos son una nueva clase de materiales magnéticos colineares compensados por espín.
  • Exhiben una magnetización neta cero pero poseen comportamientos electrónicos similares a los ferromagnetos.
  • Estas propiedades surgen de las bandas de espín dividido bajo condiciones de simetría específicas, independientemente del acoplamiento de espín-órbita.

Objetivo del estudio:

  • Esbozar los criterios esenciales para lograr una fase altermagnética.
  • Proporcionar una derivación cualitativa de la estructura de la banda electrónica y el análisis de simetría utilizando principios químicos.
  • Explorar el potencial de los altermagnetos en los dispositivos espintrónicos y revisar los materiales candidatos.

Principales métodos:

  • Análisis de simetría basado en principios químicos.
  • Derivación cualitativa de la estructura de la banda electrónica.
  • Revisión de los materiales candidatos altermagnéticos existentes.

Principales resultados:

  • Se establecieron criterios fundamentales para el altermagnetismo.
  • Demostró un camino para entender las estructuras de la banda altermagnética.
  • Identificó altermagnetos como prometedores para aplicaciones de conversión de carga a espín.

Conclusiones:

  • Los altermagnetos ofrecen propiedades únicas derivadas de la simetría, no del acoplamiento de espín-órbita.
  • Representan un avance significativo en la espintrónica, particularmente para la conversión de carga a espín.
  • La investigación adicional por parte de los químicos es crucial para avanzar en este campo emergente.