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Related Concept Videos

The Electrical Double Layer01:30

The Electrical Double Layer

In the region where two bulk phases meet, an intricate electric charge distribution arises due to charge transfer, ion adsorption, molecular orientation, and charge distortion. This complex distribution is commonly referred to as the electrical double layer.When a solid electrode interfaces with ions in an electrolyte solution, the speed of electron transfer dictates the rates of oxidation and reduction. The electrode acquires a charge through the escape of atoms into the solution as cations or...
P-N junction01:11

P-N junction

A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
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Boundary Conditions for Current Density

Current density becomes discontinuous across an interface of materials with different electrical conductivities. The normal component of the current density is continuous across the boundary.
Electric Field Inside a Conductor01:20

Electric Field Inside a Conductor

When a conductor is placed in an external electric field, the free charges in the conductor redistribute and very quickly reach electrostatic equilibrium. The resulting charge distribution and its electric field have many interesting properties, which can be investigated with the help of Gauss's law.
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Electrostatic Boundary Conditions in Dielectrics01:27

Electrostatic Boundary Conditions in Dielectrics

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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...

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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Insulating behavior at the neutrality point in single-layer graphene.

F Amet1, J R Williams, K Watanabe

  • 1Department of Applied Physics, Stanford University, Stanford, California 94305, USA.

Physical Review Letters
|June 11, 2013
PubMed
Summary
This summary is machine-generated.

At very low temperatures, graphene

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Area of Science:

  • Condensed matter physics
  • Materials science

Background:

  • Graphene's electronic properties at low temperatures are crucial for understanding quantum phenomena.
  • Boron nitride is a key substrate for high-quality graphene devices.

Purpose of the Study:

  • Investigate low-temperature conductance in graphene on boron nitride.
  • Characterize the insulating behavior at the Dirac point.

Main Methods:

  • Measurements of electrical conductance in graphene on boron nitride.
  • Temperature variation down to 20 mK.
  • Application of perpendicular magnetic fields.

Main Results:

  • Observed diverging resistivity with power-law behavior at low temperatures.
  • Reached several megohms per square resistivity at 20 mK.
  • Transitioned to a broken-valley-symmetry, ν=0 quantum Hall state under magnetic field.

Conclusions:

  • The insulating behavior at zero magnetic field is attributed to broken valley symmetry.
  • This contrasts with typical conductivity saturation observed in other systems.
  • Suggests novel electronic states in graphene/boron nitride heterostructures.