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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...
The Hall Effect01:30

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Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
Electric Field of Two Equal and Opposite Charges01:30

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Debye–Huckel–Onsager Conductance Equation01:28

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The Debye-Hückel-Onsager equation is a cornerstone of physical chemistry, providing a method to determine the molar conductance (Λm) and molar conductance at infinite dilution (Λ°m) for uni-univalent electrolytes.Uni-univalent electrolytes are electrolytes that dissociate in solution to produce one cation with a +1 charge and one anion with a –1 charge per formula unit.This equation addresses two crucial phenomena: the asymmetry effect and the electrophoretic effect. According to this equation,...
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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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Related Experiment Video

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Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
10:36

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Published on: January 21, 2016

Visualizing atomic-scale negative differential resistance in bilayer graphene.

Keun Su Kim1, Tae-Hwan Kim, Andrew L Walter

  • 1Advanced Light Source, E O Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.

Physical Review Letters
|February 5, 2013
PubMed
Summary

We observed negative differential resistance (NDR) in bilayer graphene using scanning tunneling microscopy. This quantum tunneling behavior, influenced by electric fields and defects, is key for future graphene devices.

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Nanotechnology

Background:

  • Bilayer graphene exhibits unique electronic properties.
  • Understanding quantum tunneling is crucial for electronic device development.

Purpose of the Study:

  • Investigate atomic-scale tunneling characteristics of bilayer graphene on silicon carbide.
  • Explain the origin of observed negative differential resistance (NDR).

Main Methods:

  • Utilized scanning tunneling microscopy (STM) for high-resolution tunneling spectroscopy.
  • Analyzed the electronic spectrum under a transverse electric field.

Main Results:

  • Discovered unexpected negative differential resistance (NDR) at the Dirac energy.
  • NDR spatially varies within the unit cell and originates from van Hove singularities.
  • Electron interference with defects significantly impacts NDR.

Conclusions:

  • Provided an atomic-level understanding of quantum tunneling in bilayer graphene.
  • Results are a significant step towards developing graphene-based tunneling devices.