Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Monolayer graphene modeled in the fractional quantum Hall regime at filling ν = 2/3 with intervalley-anisotropic interaction treated by a Yukawa-like finite-range pair potential.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
monolayer grapheneMLG
Variables
dimensionality= monolayer
studied material
Simulations
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.
Monolayer graphene modeled in the fractional quantum Hall regime at filling ν = 2/3 with intervalley-anisotropic interaction treated by a Yukawa-like finite-range pair potential.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
monolayer grapheneMLG
Variables
dimensionality= monolayer
studied material
Simulations
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.
Monolayer graphene modeled in the fractional quantum Hall regime at filling ν = 2/3 with intervalley-anisotropic interaction treated by a Yukawa-like finite-range pair potential.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
monolayer grapheneMLG
Variables
dimensionality= monolayer
studied material
Simulations
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.
Monolayer graphene modeled in the fractional quantum Hall regime at filling ν = 2/3 with intervalley-anisotropic interaction treated by a Yukawa-like finite-range pair potential.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
monolayer grapheneMLG
Variables
dimensionality= monolayer
studied material
Simulations
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Exact diagonalization of the graphene fractional quantum Hall Hamiltonian with nonzero-range intervalley-anisotropic Yukawa-like pair potential; comparison to the ultra-short-range limit; finite-size treatment of low-lying states and phase competition.
Settings
contextfractional quantum Hall phase diagram
ignored termsZeeman, valley-Zeeman
range controlinverse-range parameter α
filling factorν = 2/3
wavevector powerk = 2
interaction modelYukawa-like pair potential
Conditions
problem:monolayer graphene quantum Hall ferromagnetism beyond ultra-short-range approximation
Exact diagonalization of the graphene fractional quantum Hall Hamiltonian with nonzero-range intervalley-anisotropic Yukawa-like pair potential; comparison to the ultra-short-range limit; finite-size treatment of low-lying states and phase competition.
Settings
contextfractional quantum Hall phase diagram
ignored termsZeeman, valley-Zeeman
range controlinverse-range parameter α
filling factorν = 2/3
wavevector powerk = 2
interaction modelYukawa-like pair potential
Conditions
problem:monolayer graphene quantum Hall ferromagnetism beyond ultra-short-range approximation
Exact diagonalization of the graphene fractional quantum Hall Hamiltonian with nonzero-range intervalley-anisotropic Yukawa-like pair potential; comparison to the ultra-short-range limit; finite-size treatment of low-lying states and phase competition.
Settings
contextfractional quantum Hall phase diagram
ignored termsZeeman, valley-Zeeman
range controlinverse-range parameter α
filling factorν = 2/3
wavevector powerk = 2
interaction modelYukawa-like pair potential
Conditions
problem:monolayer graphene quantum Hall ferromagnetism beyond ultra-short-range approximation
Exact diagonalization of the graphene fractional quantum Hall Hamiltonian with nonzero-range intervalley-anisotropic Yukawa-like pair potential; comparison to the ultra-short-range limit; finite-size treatment of low-lying states and phase competition.
Settings
contextfractional quantum Hall phase diagram
ignored termsZeeman, valley-Zeeman
range controlinverse-range parameter α
filling factorν = 2/3
wavevector powerk = 2
interaction modelYukawa-like pair potential
Conditions
problem:monolayer graphene quantum Hall ferromagnetism beyond ultra-short-range approximation
