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Related Concept Videos

Electrostatic Boundary Conditions01:16

Electrostatic Boundary Conditions

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...
Induced Electric Fields: Applications01:27

Induced Electric Fields: Applications

An important distinction exists between the electric field induced by a changing magnetic field and the electrostatic field produced by a fixed charge distribution. Specifically, the induced electric field is nonconservative because it does not work in moving a charge over a closed path. In contrast, the electrostatic field is conservative and does no net work over a closed path. Hence, electric potential can be associated with the electrostatic field but not the induced field. The following...
Induced Electric Fields01:23

Induced Electric Fields

The fact that emfs are induced in circuits implies that work is being done on the conduction electrons in the wires. What can possibly be the source of this work? We know that it’s neither a battery nor a magnetic field, as a battery does not have to be present in a circuit where current is induced, and magnetic fields never do any work on moving charges. The source of the work is in fact an electric field that is induced in the wires. For example, if a stationary conductor is placed in a...
Electric Field Lines01:25

Electric Field Lines

The three-dimensional representation of the electric field of a positive point charge requires tracing the electric field vectors, whose lengths decrease as the square of their distance from the charge and which point away from the charge at each point. This vector field is no doubt challenging to visualize. The visualization of electric fields becomes quickly intractable as the number of charges increases.
The solution to this problem is to use electric field lines, which are not vectors but...
Electric Field01:16

Electric Field

Consider two point charges, each exerting Coulomb force on the other. It is possible to describe the Coulomb interaction via an intermediate step by defining a new physical quantity called the electric field.
In the new picture, imagine that the first charge sets up an electric field independent of all other charges in the universe. When another charge comes in its vicinity, the second charge experiences an electric force depending on the electric field at that point. The source charge does not...
Electric Field at the Surface of a Conductor01:26

Electric Field at the Surface of a Conductor

Consider a conductor in electrostatic equilibrium. The net electric field inside a conductor vanishes, and extra charges on the conductor reside on its outer surface, regardless of where they originate.
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...

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Finite Element Modelling of a Cellular Electric Microenvironment
08:23

Finite Element Modelling of a Cellular Electric Microenvironment

Published on: May 18, 2021

Dimensional crossover driven by an electric field.

Camille Aron1, Gabriel Kotliar, Cedric Weber

  • 1Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA.

Physical Review Letters
|April 3, 2012
PubMed
Summary
This summary is machine-generated.

Strong electric fields drive dimensional reduction in the dissipative Hubbard model. This effect alters spectral functions and steady currents, revealing a crossover to lower-dimensional behavior.

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Area of Science:

  • Condensed matter physics
  • Quantum mechanics
  • Statistical mechanics

Background:

  • The Hubbard model describes interacting electrons in solids.
  • Understanding driven quantum systems is crucial for novel electronic devices.
  • Dissipation and external fields introduce non-equilibrium dynamics.

Purpose of the Study:

  • Investigate the Hubbard model under a constant electric field and heat bath.
  • Analyze the phenomenon of dimensional reduction induced by strong electric fields.
  • Characterize the non-equilibrium steady-state properties.

Main Methods:

  • Derivation of steady-state equations for dynamical mean-field theory (DMFT) with dissipation.
  • Analysis of the Hubbard model in the presence of a strong electric field.
  • Calculation of spectral functions and energy distribution functions.

Main Results:

  • Observed dimensional reduction in the driven Hubbard model under strong electric fields.
  • The system effectively behaves as a lower-dimensional equilibrium Hubbard model.
  • Electric field-induced dimensional crossover impacts spectral properties and steady currents.

Conclusions:

  • Strong electric fields can induce dimensional crossovers in dissipative quantum systems.
  • This phenomenon offers new pathways to control electronic properties.
  • The derived DMFT equations provide a framework for studying driven, dissipative systems.