Related Experiment Video

Updated: Mar 17, 2026

Fabrication of Schottky Diodes on Zn-polar BeMgZnO/ZnO Heterostructure Grown by Plasma-assisted Molecular Beam Epitaxy
14:16

Fabrication of Schottky Diodes on Zn-polar BeMgZnO/ZnO Heterostructure Grown by Plasma-assisted Molecular Beam Epitaxy

Published on: October 23, 2018

8.2K

Effect of the ZnS Shell Layer on the Electrical Properties of Organic Bistable Devices Fabricated Utilizing

Nam Hyun Lee, Dong Yeol Yun, Dong Hyuk Choi

    Journal of Nanoscience and Nanotechnology
    |July 19, 2016
    PubMed

    More Related Videos

    Synthesis of Hierarchical ZnO/CdSSe Heterostructure Nanotrees06:50

    Synthesis of Hierarchical ZnO/CdSSe Heterostructure Nanotrees

    Published on: November 29, 2016

    10.5K
    Harvesting Solar Energy by Means of Charge-Separating Nanocrystals and Their Solids13:29

    Harvesting Solar Energy by Means of Charge-Separating Nanocrystals and Their Solids

    Published on: August 23, 2012

    14.8K

    Related Concept Videos

    Schottky Barrier Diode01:27

    Schottky Barrier Diode

    Schottky barrier diodes are specialized semiconductor devices characterized by their unique construction. This construction involves combining a metal layer with a moderately doped n-type semiconductor material. This combination leads to the formation of a Schottky barrier, a pivotal element that defines the diode's operational characteristics. The core functionality of Schottky barrier diodes is their capacity to allow current to flow in only one direction due to their distinctive...
    1.2K
    Semiconductors01:22

    Semiconductors

    There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
    Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
    1.8K
    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...
    1.3K
    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...
    106
    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...
    1.6K