Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Twisted bilayer graphene model at θ = 1.15° with zero heterostrain, studied at filling ν = −2 on finite momentum-space grids.
No measurements recorded
SimulatedCStudied Material
Twisted bilayer graphene model at θ = 1.15° with uniaxial heterostrain εs = 0.6% (layer strains ±εs/2 and direction φs = 130°), studied at filling ν = −2 on finite momentum-space grids.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
twisted bilayer grapheneTBG
studied material
Simulations
Other Computational
Approximated quantum Monte Carlo (AQMC) for the interacting twisted-bilayer-graphene model in momentum space; sampling-weight absolute-value approximation; benchmarked against exact diagonalization and compared with Hartree-Fock.
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.
Twisted bilayer graphene model at θ = 1.15° with zero heterostrain, studied at filling ν = −2 on finite momentum-space grids.
No measurements recorded
SimulatedCStudied Material
Twisted bilayer graphene model at θ = 1.15° with uniaxial heterostrain εs = 0.6% (layer strains ±εs/2 and direction φs = 130°), studied at filling ν = −2 on finite momentum-space grids.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
twisted bilayer grapheneTBG
studied material
Simulations
Other Computational
Approximated quantum Monte Carlo (AQMC) for the interacting twisted-bilayer-graphene model in momentum space; sampling-weight absolute-value approximation; benchmarked against exact diagonalization and compared with Hartree-Fock.
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.
Twisted bilayer graphene model at θ = 1.15° with zero heterostrain, studied at filling ν = −2 on finite momentum-space grids.
No measurements recorded
SimulatedCStudied Material
Twisted bilayer graphene model at θ = 1.15° with uniaxial heterostrain εs = 0.6% (layer strains ±εs/2 and direction φs = 130°), studied at filling ν = −2 on finite momentum-space grids.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
twisted bilayer grapheneTBG
studied material
Simulations
Other Computational
Approximated quantum Monte Carlo (AQMC) for the interacting twisted-bilayer-graphene model in momentum space; sampling-weight absolute-value approximation; benchmarked against exact diagonalization and compared with Hartree-Fock.
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.
Twisted bilayer graphene model at θ = 1.15° with zero heterostrain, studied at filling ν = −2 on finite momentum-space grids.
No measurements recorded
SimulatedCStudied Material
Twisted bilayer graphene model at θ = 1.15° with uniaxial heterostrain εs = 0.6% (layer strains ±εs/2 and direction φs = 130°), studied at filling ν = −2 on finite momentum-space grids.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
Also known as
twisted bilayer grapheneTBG
studied material
Simulations
Other Computational
Approximated quantum Monte Carlo (AQMC) for the interacting twisted-bilayer-graphene model in momentum space; sampling-weight absolute-value approximation; benchmarked against exact diagonalization and compared with Hartree-Fock.
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Hartree-Fock mean-field calculations for twisted bilayer graphene at ν = −2, used to diagnose occupation modulation and incommensurate Kekulé spiral wavevector.
Hartree-Fock mean-field calculations for twisted bilayer graphene at ν = −2, used to diagnose occupation modulation and incommensurate Kekulé spiral wavevector.
Hartree-Fock mean-field calculations for twisted bilayer graphene at ν = −2, used to diagnose occupation modulation and incommensurate Kekulé spiral wavevector.
Hartree-Fock mean-field calculations for twisted bilayer graphene at ν = −2, used to diagnose occupation modulation and incommensurate Kekulé spiral wavevector.