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Dielectric Polarization in a Capacitor01:31

Dielectric Polarization in a Capacitor

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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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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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Electrostatic Boundary Conditions in Dielectrics01:27

Electrostatic Boundary Conditions in Dielectrics

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When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's permittivity....
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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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Electric Field of a Non Uniformly Charged Sphere01:22

Electric Field of a Non Uniformly Charged Sphere

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Gauss's law states that the electric flux through any closed surface equals the net charge enclosed within the surface. This law is beneficial for determining the expressions for the electric field for a particular charge distribution if the electric flux is known.
Consider a non-uniformly charged sphere, for which the density of charge depends only on the distance from a point in space and not on the direction. Such a sphere has a spherically symmetrical charge distribution. Here, the electric...
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Electric Dipoles and Dipole Moment01:30

Electric Dipoles and Dipole Moment

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Consider two charges of equal magnitude but opposite signs. If they cannot be separated by an external electric field, the system is called a permanent dipole. For example, the water molecule is a dipole, making it a good solvent.
Theoretically, studying electric dipoles leads to understanding why the resultant electric forces around us are weak. Since electric forces are strong, remnant net charges are rare. Hence, the interaction between dipoles helps us understand electrical interactions in...
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Video Experimental Relacionado

Updated: Feb 27, 2026

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
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Isoladores eléctricos multipolares cuantificados

Wladimir A Benalcazar1, B Andrei Bernevig2, Taylor L Hughes3

  • 1Department of Physics and Institute for Condensed Matter Theory, University of Illinois at Urbana-Champaign, IL 61801, USA.

Science (New York, N.Y.)
|July 8, 2017
PubMed
Resumen
Este resumen es generado por máquina.

Revelamos cómo los momentos multipolares eléctricos más altos, como el cuádrupolo y el octopolo, pueden cuantificarse topológicamente en cristales. Este descubrimiento introduce nuevas fases topológicas con estados límite exóticos y cargas fraccionarias.

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Área de la Ciencia:

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

Sus antecedentes:

  • La fase de Berry ofrece un marco moderno para comprender la polarización eléctrica en sólidos cristalinos.
  • Los conceptos topológicos son cada vez más vitales para clasificar las fases de la materia más allá de los enfoques convencionales.

Objetivo del estudio:

  • Para extender la formulación de la fase de Berry a momentos eléctricos multipolares más altos (cuadrupolo, octopolo).
  • Identificar las condiciones y los modelos mínimos para la cuantización topológica de estos momentos multipolares.
  • Explorar las implicaciones para la clasificación de fases topológicas y la realización experimental.

Principales métodos:

  • Utilizando el formalismo de fase de Berry para analizar los momentos multipolares eléctricos.
  • Desarrollo de sistemas de modelos mínimos que exhiben cuantización topológica.
  • Introducción de un nuevo método de caracterización utilizando bucles de Wilson "anidados" para las invariantes topológicas.
  • Investigar los fenómenos fronterizos, incluidos los límites abiertos y los estados angulares.

Principales resultados:

  • Demostró que los momentos cuádrupolos y octopolos pueden ser observables cuantificados topológicamente.
  • Límites con huecos identificados que actúan como fases topológicas de menor dimensión.
  • Descubrió estados angulares topológicamente protegidos con carga fraccionaria, un fenómeno de fraccionamiento de límites.
  • Se introdujo una nueva clase de invariantes topológicos derivados de bucles de Wilson "anidados".

Conclusiones:

  • El estudio amplía la clasificación de las fases topológicas de la materia mediante la incorporación de momentos multipolares eléctricos más altos.
  • Propuso tres implementaciones experimentales de los fenómenos topológicos observados.
  • Abre nuevas vías para explorar la materia topológica y sus propiedades electromagnéticas únicas.