Related Experiment Video
Updated: May 12, 2025

11:42
Fabrication of Gate-tunable Graphene Devices for Scanning Tunneling Microscopy Studies with Coulomb Impurities
Published on: July 24, 2015
15.4K
Disentangling Morphology and Conductance in Amorphous Graphene.
Nicolas Gastellu1, Ata Madanchi2, Lena Simine1,2
1Department of Chemistry, McGill University, Montréal, Québec H3A 0C7, Canada.
The Journal of Physical Chemistry Letters
|April 29, 2025
Summary
Amorphous monolayer carbon (AMC) films show electronic conductance highly dependent on their structure. Deep learning simulations reveal how morphology and crystallinity influence conductivity, offering potential for gate voltage control.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Computational Chemistry
Background:
- Amorphous monolayer carbon (AMC) films exhibit morphology-dependent electronic conductance.
- Understanding this relationship is crucial for designing novel carbon-based electronic materials.
- Traditional methods face challenges with the aperiodic nature of AMC.
Purpose of the Study:
- To analyze the electronic conductance of morphologically distinct AMCs.
- To investigate the interplay between morphology, crystallinity, and conductance.
- To explore methods for controlling AMC conductivity.
Main Methods:
- Utilized deep learning-enhanced simulations combined with percolation theory.
- Analyzed three distinct mesoscale AMC morphologies.
- Avoided periodic boundary conditions and simplified assumptions about conducting sites.
Main Results:
- Successfully reproduced the known dependence of charge conductance on AMC morphology.
- Identified limitations of partial morphology descriptors in predicting conductance.
- Demonstrated that conductance networks shift from crystallites at band edges to defects near the Fermi energy.
Conclusions:
- AMC electronic properties are intricately linked to their complex, aperiodic morphology.
- Deep learning simulations provide a robust framework for studying these systems.
- The observed shift in localization offers a pathway for gate voltage-based control of AMC conductivity.
Related Concept Videos
Band Theory
14.8K
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,...
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
14.8K
Network Covalent Solids
13.2K
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.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
13.2K
Semiconductors
484
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...
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...
484
Boundary Conditions for Current Density
745
Current density becomes discontinuous across an interface of materials with different electrical conductivities. The normal component of the current density is continuous across the boundary.
745

