Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Electrostatic Boundary Conditions in Dielectrics01:27

Electrostatic Boundary Conditions in Dielectrics

1.3K
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...
1.3K
Electrostatic Boundary Conditions01:16

Electrostatic Boundary Conditions

567
Consider an external electric field propagating through a homogeneous medium. When the electric field crosses the surface boundary of the medium, it undergoes a discontinuity. The electric field can be resolved into normal and tangential components. The amount by which the field changes at any boundary is given by the difference between the field components above and below the surface boundary.
The surface integral of an electric field is given by Gauss's law in integral form and is related to...
567
Equipotential Surfaces and Conductors01:16

Equipotential Surfaces and Conductors

3.6K
For a conductor in which all charges are at rest, the conductor's surface is equipotential. The electric field is always perpendicular to equipotential surfaces. Therefore, in a conductor with static charges, the electric field just outside the conductor is always perpendicular to the conductor's surface. Any tangential component of the electric field will cause charges to move inside the conductor, which will violate the electrostatic nature of the system. In an electrostatic...
3.6K
Potential Due to a Polarized Object01:29

Potential Due to a Polarized Object

460
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,...
460
Equipotential Surfaces and Field Lines01:29

Equipotential Surfaces and Field Lines

3.9K
Electric potential can be pictorially represented as a three-dimensional surface. On such a surface, the electric potential is constant everywhere. The equipotential surface is always perpendicular to the electric field lines, and while it is three-dimensional, it can be treated as an equipotential line in a two-dimensional case. These equipotential lines are also always perpendicular to electric field lines. The term equipotential is often used as a noun, referring to an equipotential line or...
3.9K
Electric Field of a Non Uniformly Charged Sphere01:22

Electric Field of a Non Uniformly Charged Sphere

1.6K
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...
1.6K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Spectral signature of high-order photon processes enhanced by Cooper-pair pairing.

Nature communications·2025
Same author

Two-Peak Heat Capacity Accounts for Rln(2) Entropy and Ground State Access in the Dipole-Octupole Pyrochlore Ce_{2}Hf_{2}O_{7}.

Physical review letters·2025
Same author

Field-Tunable Berezinskii-Kosterlitz-Thouless Correlations in a Heisenberg Magnet.

Physical review letters·2023
Same author

Dirac Magnons, Nodal Lines, and Nodal Plane in Elemental Gadolinium.

Physical review letters·2022
Same author

Emergent Moments and Random Singlet Physics in a Majorana Spin Liquid.

Physical review letters·2021
Same author

Tools for optimising pharmacotherapy in psychiatry (therapeutic drug monitoring, molecular brain imaging and pharmacogenetic tests): focus on antidepressants.

The world journal of biological psychiatry : the official journal of the World Federation of Societies of Biological Psychiatry·2021
Same journal

Interplay of Anisotropy, Dzyaloshinskii Moriya Interaction and Symmetry breaking Fields in a 2D XY Ferromagnet.

Journal of physics. Condensed matter : an Institute of Physics journal·2026
Same journal

Single-molecule electron transport near a charge-trapping orbital-level alignment.

Journal of physics. Condensed matter : an Institute of Physics journal·2026
Same journal

Δ<sub>T</sub>Noise as a Robust Diagnostic for Chiral, Helical and Trivial Edge Modes.

Journal of physics. Condensed matter : an Institute of Physics journal·2026
Same journal

A Quantum Framework for Negative Magnetoresistance in Multi-Weyl Semimetals.

Journal of physics. Condensed matter : an Institute of Physics journal·2026
Same journal

Magnetic anisotropy and electronic structure in surface-supported single rare-earth atom magnets: a topical review.

Journal of physics. Condensed matter : an Institute of Physics journal·2026
Same journal

Modeling thermal transport in AlN/GaN superlattices and heterostructures with machine-learned force fields.

Journal of physics. Condensed matter : an Institute of Physics journal·2026
See all related articles

Related Experiment Video

Updated: Aug 28, 2025

Finite Element Modelling of a Cellular Electric Microenvironment
08:23

Finite Element Modelling of a Cellular Electric Microenvironment

Published on: May 18, 2021

3.5K

Topological electrostatics.

B Douçot1, R Moessner2, D L Kovrizhin3

  • 1LPTHE, CNRS and Sorbonne Université, 75252 Paris Cedex 05, France.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|September 22, 2022
PubMed
Summary
This summary is machine-generated.

We developed a theory for optimal topological textures in nonlinear sigma-models, crucial for understanding skyrmion lattices in quantum Hall systems. This theory identifies conditions for texture stability and reveals new zero modes in graphene physics.

Keywords:
Grassmanniangraphenequantum Hall ferromagnetskyrmion

More Related Videos

Development of a 3D Graphene Electrode Dielectrophoretic Device
11:15

Development of a 3D Graphene Electrode Dielectrophoretic Device

Published on: June 22, 2014

12.1K
AC Electrokinetic Phenomena Generated by Microelectrode Structures
20:38

AC Electrokinetic Phenomena Generated by Microelectrode Structures

Published on: July 28, 2008

11.6K

Related Experiment Videos

Last Updated: Aug 28, 2025

Finite Element Modelling of a Cellular Electric Microenvironment
08:23

Finite Element Modelling of a Cellular Electric Microenvironment

Published on: May 18, 2021

3.5K
Development of a 3D Graphene Electrode Dielectrophoretic Device
11:15

Development of a 3D Graphene Electrode Dielectrophoretic Device

Published on: June 22, 2014

12.1K
AC Electrokinetic Phenomena Generated by Microelectrode Structures
20:38

AC Electrokinetic Phenomena Generated by Microelectrode Structures

Published on: July 28, 2008

11.6K

Area of Science:

  • Condensed Matter Physics
  • Quantum Field Theory
  • Materials Science

Background:

  • Topological textures, such as skyrmion lattices, are essential in understanding exotic quantum phenomena.
  • Nonlinear sigma-models provide a theoretical framework for describing these textures in systems like graphene and quantum Hall systems.
  • Existing models often lack a comprehensive understanding of texture optimality and stability under various conditions.

Purpose of the Study:

  • To present a theory of optimal topological textures in nonlinear sigma-models defined on Grassmannian manifolds.
  • To analyze the conditions for minimizing topological charge density fluctuations in these models.
  • To investigate the implications for N-component fermions in quantizing magnetic fields relevant to quantum Hall systems.

Main Methods:

  • Developed a theoretical framework for optimal topological textures in Grassmannian nonlinear sigma-models (Gr(M,N)).
  • Derived analytical optimality conditions by minimizing topological charge density fluctuations on spherical and toroidal geometries.
  • Employed counting arguments to determine critical values of topological charge (dc) for texture existence and uniqueness.

Main Results:

  • Established an analytical condition for optimal textures, minimizing charge density fluctuations in Grassmannian sigma models.
  • Identified a critical topological charge (dc) above which optimal textures do not exist.
  • Found unique solutions on a torus below dc, contrasting with a continuum of solutions and new non-Goldstone zero modes on a sphere.

Conclusions:

  • The theory provides a framework for understanding optimal topological textures in various quantum systems.
  • The existence and nature of optimal textures depend critically on the topological charge and system geometry.
  • Specific analytical results for Gr(2,4) are relevant to recent experimental findings in graphene.