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Related Concept Videos

Energy Bands in Solids01:01

Energy Bands in Solids

Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
 Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states that no two...
Fermi Level Dynamics01:12

Fermi Level Dynamics

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
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...
Band Theory02:35

Band Theory

When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...

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Related Experiment Video

Updated: Jul 11, 2026

Fabrication of Gate-tunable Graphene Devices for Scanning Tunneling Microscopy Studies with Coulomb Impurities
11:42

Fabrication of Gate-tunable Graphene Devices for Scanning Tunneling Microscopy Studies with Coulomb Impurities

Published on: July 24, 2015

Substrate-induced bandgap opening in epitaxial graphene.

S Y Zhou1, G-H Gweon, A V Fedorov

  • 1Department of Physics, University of California, Berkeley, California 94720, USA.

Nature Materials
|September 11, 2007
PubMed
Summary

Graphene grown on silicon carbide (SiC) substrates naturally forms an energy gap, crucial for electronic applications like transistors. This bandgap engineering approach offers a simpler alternative to complex graphene modifications.

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Theoretical Calculation and Experimental Verification for Dislocation Reduction in Germanium Epitaxial Layers with Semicylindrical Voids on Silicon

Published on: July 17, 2020

Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Nanotechnology

Background:

  • Graphene is a promising material for advanced electronics due to its unique properties.
  • A major limitation for graphene in electronics is its lack of a natural energy bandgap.
  • Existing methods to create a bandgap in graphene are often complex and difficult to implement.

Purpose of the Study:

  • To investigate a method for opening an energy gap in graphene.
  • To explore the potential of substrate interaction for graphene bandgap engineering.
  • To assess the feasibility of using epitaxial growth for creating functional graphene electronics.

Main Methods:

  • Epitaxial growth of graphene on silicon carbide (SiC) substrates.
  • Characterization of the electronic properties of the grown graphene layers.
  • Analysis of the relationship between sample thickness and the observed energy gap.

Main Results:

  • Graphene epitaxially grown on SiC substrates exhibits an energy gap of approximately 0.26 eV.
  • The energy gap size decreases with increasing graphene layer thickness.
  • The bandgap diminishes to near zero for samples with more than four layers.
  • The observed gap is attributed to the breaking of sublattice symmetry caused by graphene-substrate interaction.

Conclusions:

  • Epitaxial growth of graphene on SiC is an effective method for creating a tunable energy bandgap.
  • This substrate-induced bandgap engineering offers a promising route for developing graphene-based electronic devices, such as transistors.
  • The findings suggest a simpler pathway for harnessing graphene's electronic potential without complex fabrication techniques.