4×4 Luttinger Hamiltonian with confinement potential; effective 2D Hamiltonian derived by integrating out kz; spin-projected band structure calculation using numerical solution of the time-independent Schrödinger equation in a triangular well confinement potential.Kwant
Real-space finite-difference discretization of the effective Hamiltonian combined with non-equilibrium Green's function transport calculations to obtain conductance and local density of states for transverse magnetic focusing devices.Kwant
4×4 Luttinger Hamiltonian with confinement potential; effective 2D Hamiltonian derived by integrating out kz; spin-projected band structure calculation using numerical solution of the time-independent Schrödinger equation in a triangular well confinement potential.Kwant
Real-space finite-difference discretization of the effective Hamiltonian combined with non-equilibrium Green's function transport calculations to obtain conductance and local density of states for transverse magnetic focusing devices.Kwant
4×4 Luttinger Hamiltonian with confinement potential; effective 2D Hamiltonian derived by integrating out kz; spin-projected band structure calculation using numerical solution of the time-independent Schrödinger equation in a triangular well confinement potential.Kwant
Real-space finite-difference discretization of the effective Hamiltonian combined with non-equilibrium Green's function transport calculations to obtain conductance and local density of states for transverse magnetic focusing devices.Kwant
4×4 Luttinger Hamiltonian with confinement potential; effective 2D Hamiltonian derived by integrating out kz; spin-projected band structure calculation using numerical solution of the time-independent Schrödinger equation in a triangular well confinement potential.Kwant
Real-space finite-difference discretization of the effective Hamiltonian combined with non-equilibrium Green's function transport calculations to obtain conductance and local density of states for transverse magnetic focusing devices.Kwant
vector potential optionsA = -Bz y x-hat, A = Bz x y-hat
Conditions
context:modeled_transport
validation:{"quantities":["transverse magnetic focusing conductance spectra"],"references":["Lee et al. 2018","Winkler 2003"],"techniques":["transport"],"source_type":"literature_experimental_data"}
vector potential optionsA = -Bz y x-hat, A = Bz x y-hat
Conditions
context:modeled_transport
validation:{"quantities":["transverse magnetic focusing conductance spectra"],"references":["Lee et al. 2018","Winkler 2003"],"techniques":["transport"],"source_type":"literature_experimental_data"}
vector potential optionsA = -Bz y x-hat, A = Bz x y-hat
Conditions
context:modeled_transport
validation:{"quantities":["transverse magnetic focusing conductance spectra"],"references":["Lee et al. 2018","Winkler 2003"],"techniques":["transport"],"source_type":"literature_experimental_data"}
vector potential optionsA = -Bz y x-hat, A = Bz x y-hat
Conditions
context:modeled_transport
validation:{"quantities":["transverse magnetic focusing conductance spectra"],"references":["Lee et al. 2018","Winkler 2003"],"techniques":["transport"],"source_type":"literature_experimental_data"}
