Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Pristine ex-so-tic graphene-based van-der-Waals heterostructure consisting of bilayer graphene between WS₂ and Cr₂Ge₂Te6, modeled analytically through a low-energy effective Hamiltonian around K and K' points.
No measurements recorded
SimulatedCStudied MaterialWS₂Studied MaterialCr₂Ge₂Te₆Studied Material
Materials
bilayer graphene
C
Studied Material
Also known as
BLGgraphene bilayer
Variables
layer_count= 2
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.
Pristine ex-so-tic graphene-based van-der-Waals heterostructure consisting of bilayer graphene between WS₂ and Cr₂Ge₂Te6, modeled analytically through a low-energy effective Hamiltonian around K and K' points.
No measurements recorded
SimulatedCStudied MaterialWS₂Studied MaterialCr₂Ge₂Te₆Studied Material
Materials
bilayer graphene
C
Studied Material
Also known as
BLGgraphene bilayer
Variables
layer_count= 2
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.
Pristine ex-so-tic graphene-based van-der-Waals heterostructure consisting of bilayer graphene between WS₂ and Cr₂Ge₂Te6, modeled analytically through a low-energy effective Hamiltonian around K and K' points.
No measurements recorded
SimulatedCStudied MaterialWS₂Studied MaterialCr₂Ge₂Te₆Studied Material
Materials
bilayer graphene
C
Studied Material
Also known as
BLGgraphene bilayer
Variables
layer_count= 2
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.
Pristine ex-so-tic graphene-based van-der-Waals heterostructure consisting of bilayer graphene between WS₂ and Cr₂Ge₂Te6, modeled analytically through a low-energy effective Hamiltonian around K and K' points.
No measurements recorded
SimulatedCStudied MaterialWS₂Studied MaterialCr₂Ge₂Te₆Studied Material
Materials
bilayer graphene
C
Studied Material
Also known as
BLGgraphene bilayer
Variables
layer_count= 2
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Analytical low-energy reduction of a k·p Hamiltonian derived from a prior DFT/symmetry model; eigenvalues evaluated around K and K' points and compared with the full k·p spectrum.
Settings
fieldHall transport in proximity-coupled BLG heterostructure
modeleffective k·p Hamiltonian
valleysK, K'
parameters sourceZollner et al. Phys. Rev. Lett. 125, 196402 (2020)
Conditions
context:analytical low-energy electronic spectrum
comparison:low-energy reduced Hamiltonian vs full k·p Hamiltonian
Analytical low-energy reduction of a k·p Hamiltonian derived from a prior DFT/symmetry model; eigenvalues evaluated around K and K' points and compared with the full k·p spectrum.
Settings
fieldHall transport in proximity-coupled BLG heterostructure
modeleffective k·p Hamiltonian
valleysK, K'
parameters sourceZollner et al. Phys. Rev. Lett. 125, 196402 (2020)
Conditions
context:analytical low-energy electronic spectrum
comparison:low-energy reduced Hamiltonian vs full k·p Hamiltonian
Analytical low-energy reduction of a k·p Hamiltonian derived from a prior DFT/symmetry model; eigenvalues evaluated around K and K' points and compared with the full k·p spectrum.
Settings
fieldHall transport in proximity-coupled BLG heterostructure
modeleffective k·p Hamiltonian
valleysK, K'
parameters sourceZollner et al. Phys. Rev. Lett. 125, 196402 (2020)
Conditions
context:analytical low-energy electronic spectrum
comparison:low-energy reduced Hamiltonian vs full k·p Hamiltonian
Analytical low-energy reduction of a k·p Hamiltonian derived from a prior DFT/symmetry model; eigenvalues evaluated around K and K' points and compared with the full k·p spectrum.
Settings
fieldHall transport in proximity-coupled BLG heterostructure
modeleffective k·p Hamiltonian
valleysK, K'
parameters sourceZollner et al. Phys. Rev. Lett. 125, 196402 (2020)
Conditions
context:analytical low-energy electronic spectrum
comparison:low-energy reduced Hamiltonian vs full k·p Hamiltonian
