Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Quasiperiodic chiral Bistritzer-MacDonald model of twisted bilayer graphene with two incommensurate moiré potentials, focused on the inverse-golden-ratio case.
No measurements recorded
SimulatedCStudied Material
Silver-ratio variant quasiperiodic chiral Bistritzer-MacDonald model used as an additional numerical case study.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
twisted bilayer grapheneTBLGquasiperiodic twisted bilayer grapheneqBM model
Variables
model
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.
Quasiperiodic chiral Bistritzer-MacDonald model of twisted bilayer graphene with two incommensurate moiré potentials, focused on the inverse-golden-ratio case.
No measurements recorded
SimulatedCStudied Material
Silver-ratio variant quasiperiodic chiral Bistritzer-MacDonald model used as an additional numerical case study.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
twisted bilayer grapheneTBLGquasiperiodic twisted bilayer grapheneqBM model
Variables
model
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.
Quasiperiodic chiral Bistritzer-MacDonald model of twisted bilayer graphene with two incommensurate moiré potentials, focused on the inverse-golden-ratio case.
No measurements recorded
SimulatedCStudied Material
Silver-ratio variant quasiperiodic chiral Bistritzer-MacDonald model used as an additional numerical case study.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
twisted bilayer grapheneTBLGquasiperiodic twisted bilayer grapheneqBM model
Variables
model
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.
Quasiperiodic chiral Bistritzer-MacDonald model of twisted bilayer graphene with two incommensurate moiré potentials, focused on the inverse-golden-ratio case.
No measurements recorded
SimulatedCStudied Material
Silver-ratio variant quasiperiodic chiral Bistritzer-MacDonald model used as an additional numerical case study.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
twisted bilayer grapheneTBLGquasiperiodic twisted bilayer grapheneqBM model
Variables
model
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Kernel polynomial method (KPM) for density of states and wave-function calculations; Chebyshev filtering and shaking for eigenfunctions; quasiperiodic chiral Bistritzer-MacDonald model with incommensurate moiré potentials.
Settings
modelquasiperiodic chiral Bistritzer-MacDonald model
notesDensity of states, zero-energy DOS maps, and wave-function fractality analyses
unitsvF = 1, kθ = 1
approachKPM, Chebyshev filtering and shaking
parametersA1, A2, NΛ, Fn, NC
momentum space latticerational approximants to inverse golden ratio
Self-consistent BCS calculations combined with numerical evaluation of the superfluid stiffness on the quasiperiodic chiral Bistritzer-MacDonald model.
Settings
modelquasiperiodic chiral Bistritzer-MacDonald model
notesSuperconducting pairing amplitude as a function of moiré-potential strengths
unitsinteraction strength U measured relative to kinetic energy
Kernel polynomial method (KPM) for density of states and wave-function calculations; Chebyshev filtering and shaking for eigenfunctions; quasiperiodic chiral Bistritzer-MacDonald model with incommensurate moiré potentials.
Settings
modelquasiperiodic chiral Bistritzer-MacDonald model
notesDensity of states, zero-energy DOS maps, and wave-function fractality analyses
unitsvF = 1, kθ = 1
approachKPM, Chebyshev filtering and shaking
parametersA1, A2, NΛ, Fn, NC
momentum space latticerational approximants to inverse golden ratio
Self-consistent BCS calculations combined with numerical evaluation of the superfluid stiffness on the quasiperiodic chiral Bistritzer-MacDonald model.
Settings
modelquasiperiodic chiral Bistritzer-MacDonald model
notesSuperconducting pairing amplitude as a function of moiré-potential strengths
unitsinteraction strength U measured relative to kinetic energy
Kernel polynomial method (KPM) for density of states and wave-function calculations; Chebyshev filtering and shaking for eigenfunctions; quasiperiodic chiral Bistritzer-MacDonald model with incommensurate moiré potentials.
Settings
modelquasiperiodic chiral Bistritzer-MacDonald model
notesDensity of states, zero-energy DOS maps, and wave-function fractality analyses
unitsvF = 1, kθ = 1
approachKPM, Chebyshev filtering and shaking
parametersA1, A2, NΛ, Fn, NC
momentum space latticerational approximants to inverse golden ratio
Self-consistent BCS calculations combined with numerical evaluation of the superfluid stiffness on the quasiperiodic chiral Bistritzer-MacDonald model.
Settings
modelquasiperiodic chiral Bistritzer-MacDonald model
notesSuperconducting pairing amplitude as a function of moiré-potential strengths
unitsinteraction strength U measured relative to kinetic energy
Kernel polynomial method (KPM) for density of states and wave-function calculations; Chebyshev filtering and shaking for eigenfunctions; quasiperiodic chiral Bistritzer-MacDonald model with incommensurate moiré potentials.
Settings
modelquasiperiodic chiral Bistritzer-MacDonald model
notesDensity of states, zero-energy DOS maps, and wave-function fractality analyses
unitsvF = 1, kθ = 1
approachKPM, Chebyshev filtering and shaking
parametersA1, A2, NΛ, Fn, NC
momentum space latticerational approximants to inverse golden ratio
Self-consistent BCS calculations combined with numerical evaluation of the superfluid stiffness on the quasiperiodic chiral Bistritzer-MacDonald model.
Settings
modelquasiperiodic chiral Bistritzer-MacDonald model
notesSuperconducting pairing amplitude as a function of moiré-potential strengths
unitsinteraction strength U measured relative to kinetic energy