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Network Covalent Solids02:18

Network Covalent Solids

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Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
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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...
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Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
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Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
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Junction Field Effect Transistors (JFETs) exhibit specific operational characteristics based on the relationship between the drain current (id) and the drain-source voltage (Vds), along with varying gate-source voltages (Vgs).
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A Standard and Reliable Method to Fabricate Two-Dimensional Nanoelectronics
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Two-dimensional graphyne-graphene heterostructure for all-carbon transistors.

Jing Huang1, Jun Kang1

  • 1Beijing Computational Science Research Center, 100193 Beijing, People's Republic of China.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|February 2, 2022
PubMed
Summary

Semiconducting graphyne and graphene heterostructures exhibit excellent electron transport properties for next-generation field-effect transistors (FETs). These all-carbon devices offer tunable n-type or p-type contacts, paving the way for advanced electronics.

Keywords:
Ohmic contactSchottky barrier heightall-carbonelectron tunnelingfield effect transistorsgraphynetwo-dimensional heterostructure

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Nanotechnology

Background:

  • Two-dimensional (2D) graphyne is a promising semiconducting carbon allotrope for high-mobility applications.
  • All-carbon field-effect transistors (FETs) are under development for next-generation electronics.
  • Van der Waals heterostructures offer unique electronic properties through material stacking.

Purpose of the Study:

  • To investigate the electronic properties of 2D graphyne and graphene (GY/G) van der Waals heterostructures.
  • To determine the suitability of GY/G heterostructures for all-carbon FETs.
  • To explore methods for tuning the electronic contact properties of GY/G heterostructures.

Main Methods:

  • First-principles calculations were employed to simulate the electronic structure of GY/G heterostructures.
  • Analysis of band dispersion, charge transfer, and Fermi level alignment was performed.
  • The effect of external electric fields and doping on Schottky barrier height (SBH) was investigated.

Main Results:

  • The band dispersion of individual graphene and graphyne layers remained intact upon heterostructure formation.
  • Charge transfer from graphene to graphyne resulted in an n-type Ohmic contact with zero SBH.
  • Efficient electron tunneling and tunable contact properties (n-type to p-type) were demonstrated.

Conclusions:

  • GY/G heterostructures exhibit excellent electron transport properties, making them suitable for 2D FETs.
  • Tunable SBH via external electric fields or doping offers design flexibility for electronic devices.
  • These findings provide valuable insights for the development of advanced all-carbon electronic devices.