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Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
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...
Pinching-off of Coated Vesicles01:32

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Junction Potentials in Galvanic Cells01:21

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The Nernst equation, derived under the assumption of thermodynamic equilibrium, calculates the electromotive force (emf) as the sum of potential differences at phase boundaries in a reversible cell without a liquid junction. However, in irreversible cells such as the Daniell cell, an additional potential difference named the liquid-junction potential (EJ) arises across the interface of two electrolyte solutions due to different ion diffusion rates. This EJ represents the potential difference...
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Preparation of a Corannulene-functionalized Hexahelicene by Copper(I)-catalyzed Alkyne-azide Cycloaddition of Nonplanar Polyaromatic Units
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Current-driven dynamics in molecular junctions: endohedral fullerenes.

Ryan Jorn1, Jin Zhao, Hrvoje Petek

  • 1Department of Chemistry, Northwestern University, 2145 Sheridan Road, Evanston, Illinois 60208-3113, United States.

ACS Nano
|September 3, 2011
PubMed
Summary

We present a new approach for single molecule devices using electronic control of atom motion inside fullerene cages. This enables novel nanoelectromechanical systems and single molecule electronics applications.

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Area of Science:

  • Molecular Electronics
  • Nanotechnology
  • Quantum Mechanics

Background:

  • Single molecule devices offer potential for miniaturization.
  • Controlling internal atomic motion is key for novel functionalities.

Purpose of the Study:

  • Introduce a new paradigm for single molecule devices.
  • Explore electronic actuation of internal atom motion within fullerene cages.

Main Methods:

  • Combined electronic structure calculations and dynamical simulations.
  • Investigated current-triggered dynamics in endohedrally doped fullerene molecular junctions.

Main Results:

  • Observed Li atom oscillation within a C(60) cage in an Au-Li@C(60)-Au junction.
  • Demonstrated fullerene cage bouncing between gold electrodes due to atom motion.
  • Identified coupled 2D dynamics initiated by inelastic electron tunneling.

Conclusions:

  • This work establishes a new paradigm for single molecule devices.
  • Findings have implications for advancing single molecule electronics and nanoelectromechanical systems.