Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Rigid nanoscale graphene flake of variable polygonal shape (circular, square, triangular, or hexagonal) sliding on a fixed graphene substrate with a twist angle; used to study friction scaling.
No measurements recorded
SimulatedCStudied MaterialCSubstrate / Dielectric
Rigid nanoscale graphene flake of variable polygonal shape sliding on a fixed h-BN substrate with a twist angle; used to study friction scaling.
No measurements recorded
SimulatedCStudied Materialh-BNStudied Material
Materials
graphene
C
Studied Material
Also known as
graphitic flakegraphitic contact
Variables
dimensionality= 2D
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Rigid nanoscale graphene flake of variable polygonal shape (circular, square, triangular, or hexagonal) sliding on a fixed graphene substrate with a twist angle; used to study friction scaling.
No measurements recorded
SimulatedCStudied MaterialCSubstrate / Dielectric
Rigid nanoscale graphene flake of variable polygonal shape sliding on a fixed h-BN substrate with a twist angle; used to study friction scaling.
No measurements recorded
SimulatedCStudied Materialh-BNStudied Material
Materials
graphene
C
Studied Material
Also known as
graphitic flakegraphitic contact
Variables
dimensionality= 2D
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Rigid nanoscale graphene flake of variable polygonal shape (circular, square, triangular, or hexagonal) sliding on a fixed graphene substrate with a twist angle; used to study friction scaling.
No measurements recorded
SimulatedCStudied MaterialCSubstrate / Dielectric
Rigid nanoscale graphene flake of variable polygonal shape sliding on a fixed h-BN substrate with a twist angle; used to study friction scaling.
No measurements recorded
SimulatedCStudied Materialh-BNStudied Material
Materials
graphene
C
Studied Material
Also known as
graphitic flakegraphitic contact
Variables
dimensionality= 2D
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Rigid nanoscale graphene flake of variable polygonal shape (circular, square, triangular, or hexagonal) sliding on a fixed graphene substrate with a twist angle; used to study friction scaling.
No measurements recorded
SimulatedCStudied MaterialCSubstrate / Dielectric
Rigid nanoscale graphene flake of variable polygonal shape sliding on a fixed h-BN substrate with a twist angle; used to study friction scaling.
No measurements recorded
SimulatedCStudied Materialh-BNStudied Material
Materials
graphene
C
Studied Material
Also known as
graphitic flakegraphitic contact
Variables
dimensionality= 2D
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Rigid sliding calculations using the anisotropic interlayer potential (ILP) with refined parameters; periodic boundary conditions with large supercells; analytical continuum model for moiré-induced periodic potential and geometric registry analysis.
Settings
shapescircular, square, triangular, hexagonal
potentialanisotropic interlayer potential (ILP)
substratesgraphene, h-BN
rigid flaketrue
twist angle deg5
analytical modelmoiré-induced periodic potential
registry metricslocal registry index (LRI), global registry index (GRI)
edge terminationsarmchair, zigzag
sliding directionarmchair direction of the substrate
supercell paddingdistance larger than 40 Å between flake and periodic images
force field cutoff16 Å
potential parametersrefined parameters
periodic boundary conditionstrue
Conditions
context:modeled friction scaling and moiré-superstructure compensation in twisted incommensurate layered interfaces
Rigid sliding calculations using the anisotropic interlayer potential (ILP) with refined parameters; periodic boundary conditions with large supercells; analytical continuum model for moiré-induced periodic potential and geometric registry analysis.
Settings
shapescircular, square, triangular, hexagonal
potentialanisotropic interlayer potential (ILP)
substratesgraphene, h-BN
rigid flaketrue
twist angle deg5
analytical modelmoiré-induced periodic potential
registry metricslocal registry index (LRI), global registry index (GRI)
edge terminationsarmchair, zigzag
sliding directionarmchair direction of the substrate
supercell paddingdistance larger than 40 Å between flake and periodic images
force field cutoff16 Å
potential parametersrefined parameters
periodic boundary conditionstrue
Conditions
context:modeled friction scaling and moiré-superstructure compensation in twisted incommensurate layered interfaces
Rigid sliding calculations using the anisotropic interlayer potential (ILP) with refined parameters; periodic boundary conditions with large supercells; analytical continuum model for moiré-induced periodic potential and geometric registry analysis.
Settings
shapescircular, square, triangular, hexagonal
potentialanisotropic interlayer potential (ILP)
substratesgraphene, h-BN
rigid flaketrue
twist angle deg5
analytical modelmoiré-induced periodic potential
registry metricslocal registry index (LRI), global registry index (GRI)
edge terminationsarmchair, zigzag
sliding directionarmchair direction of the substrate
supercell paddingdistance larger than 40 Å between flake and periodic images
force field cutoff16 Å
potential parametersrefined parameters
periodic boundary conditionstrue
Conditions
context:modeled friction scaling and moiré-superstructure compensation in twisted incommensurate layered interfaces
Rigid sliding calculations using the anisotropic interlayer potential (ILP) with refined parameters; periodic boundary conditions with large supercells; analytical continuum model for moiré-induced periodic potential and geometric registry analysis.
Settings
shapescircular, square, triangular, hexagonal
potentialanisotropic interlayer potential (ILP)
substratesgraphene, h-BN
rigid flaketrue
twist angle deg5
analytical modelmoiré-induced periodic potential
registry metricslocal registry index (LRI), global registry index (GRI)
edge terminationsarmchair, zigzag
sliding directionarmchair direction of the substrate
supercell paddingdistance larger than 40 Å between flake and periodic images
force field cutoff16 Å
potential parametersrefined parameters
periodic boundary conditionstrue
Conditions
context:modeled friction scaling and moiré-superstructure compensation in twisted incommensurate layered interfaces