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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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Induced Electric Dipoles01:28

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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...
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Dielectric Polarization in a Capacitor01:31

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The presence of a dielectric medium in a capacitor not only changes the voltage and capacitance but also affects the electric field. In general, dielectrics can be of two types: polar and nonpolar. In a polar dielectric, the positive and negative charges in the molecules are separated by a distance and hence have a permanent dipole moment. In contrast, no such charge separation exists in a nonpolar dielectric, however the nonpolar molecules get polarized in the presence of an external electric...
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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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Potential Due to a Polarized Object01:29

Potential Due to a Polarized Object

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A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
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Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

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A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
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Updated: Sep 10, 2025

Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals
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Polarización multiferroica inducida dinámicamente

Carolina Paiva1, Michael Fechner2, Dominik M Juraschek1,3

  • 1Tel Aviv University, School of Physics and Astronomy, Tel Aviv 6997801, Israel.

Physical review letters
|August 27, 2025
PubMed
Resumen

Los científicos ahora pueden crear polarización y magnetización ferroeléctrica en materiales no polares utilizando pulsos láser. Este descubrimiento permite un control ultrarrápido de las propiedades multiferroicas y magnetoeléctricas en nuevos materiales.

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Área de la Ciencia:

  • Física de la materia condensada
  • Ciencias de los materiales
  • La óptica cuántica

Sus antecedentes:

  • La polarización y la magnetización ferroeléctricas se encuentran típicamente en materiales distintos.
  • El logro de la multiferroicidad (coexistencia de ferroelectricidad y magnetismo) en materiales no polares y no magnéticos es un desafío significativo.
  • El control de estas propiedades en escalas de tiempo ultrarrápidas sigue siendo un área activa de investigación.

Objetivo del estudio:

  • Describir un nuevo mecanismo para inducir la polarización ferroeléctrica y la magnetización en materiales no polares y no magnéticos.
  • Para demostrar la inducción transitoria de estas propiedades utilizando pulsos láser ultrarrápidos.
  • Explorar el control de la polarización multiferroica a través de la quiralidad del pulso láser y los modos de fonón.

Principales métodos:

  • Modelado fenomenológico
  • Cálculos de los primeros principios
  • Excitación láser ultrarrápida de los modos de fonón en el borato de litio gamma (γ-LiBO2)

Principales resultados:

  • Se ha demostrado la inducción transitoria de la polarización ferroeléctrica, la magnetización o ambas simultáneamente en γ-LiBO2.
  • Se demostró que la polarización y la magnetización inducidas dependen de la polarización (lineal, circular, elíptica) y la quiralidad del pulso láser.
  • Se estableció que la dirección y la magnitud de la polarización multiferroica pueden ajustarse mediante la quiralidad del láser y los modos de fonón.

Conclusiones:

  • Se ha establecido una nueva vía para crear y controlar la multiferroicidad y la magnetoelectricidad en materiales no polares.
  • Los pulsos láser ultrarrápidos ofrecen un método prometedor para el control dinámico de la polarización magnética y eléctrica.
  • Este trabajo abre caminos para el desarrollo de nuevos dispositivos multiferroicos con capacidades de conmutación ultrarrápida.