Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Graphene armchair nanoribbon / 2D graphene layer under tilted laser illumination, modeled with a Floquet-Bloch Hamiltonian to study LDOS, Floquet edge states, Floquet interface states, and bulk topological states.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
studied material
Simulations
Other Computational
Semiclassical time-dependent electromagnetic field coupled to a Floquet-Bloch Hamiltonian; calculation of time-averaged local density of states and transmission amplitudes for tilted laser illumination.
Settings
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.
Graphene armchair nanoribbon / 2D graphene layer under tilted laser illumination, modeled with a Floquet-Bloch Hamiltonian to study LDOS, Floquet edge states, Floquet interface states, and bulk topological states.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
studied material
Simulations
Other Computational
Semiclassical time-dependent electromagnetic field coupled to a Floquet-Bloch Hamiltonian; calculation of time-averaged local density of states and transmission amplitudes for tilted laser illumination.
Settings
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.
Graphene armchair nanoribbon / 2D graphene layer under tilted laser illumination, modeled with a Floquet-Bloch Hamiltonian to study LDOS, Floquet edge states, Floquet interface states, and bulk topological states.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
studied material
Simulations
Other Computational
Semiclassical time-dependent electromagnetic field coupled to a Floquet-Bloch Hamiltonian; calculation of time-averaged local density of states and transmission amplitudes for tilted laser illumination.
Settings
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.
Graphene armchair nanoribbon / 2D graphene layer under tilted laser illumination, modeled with a Floquet-Bloch Hamiltonian to study LDOS, Floquet edge states, Floquet interface states, and bulk topological states.
No measurements recorded
SimulatedCStudied Material
Materials
graphene
C
Studied Material
studied material
Simulations
Other Computational
Semiclassical time-dependent electromagnetic field coupled to a Floquet-Bloch Hamiltonian; calculation of time-averaged local density of states and transmission amplitudes for tilted laser illumination.
Settings
Why these are connected
Related documents with shared materials, methods, properties, or citations.
laser parameters{"frequency":null,"polarization":"linear or circular","incidenceplane":"yz","irradiationplane":"xy","tiltanglesymbol":"θ","wavelengthrelation":"L = λ / sin θ for a single tilted laser; quasi-1D supercell relation also discussed as L = λ / (√3 a sin θ) for armchair nanoribbons"}
quantities computedtime-averaged local density of states, transmission amplitudes
laser configurationssingle perpendicular circularly polarized laser, two lasers with opposite circular polarizations, two lasers tilted along the same axis, two lasers tilted along orthogonal axes
laser parameters{"frequency":null,"polarization":"linear or circular","incidenceplane":"yz","irradiationplane":"xy","tiltanglesymbol":"θ","wavelengthrelation":"L = λ / sin θ for a single tilted laser; quasi-1D supercell relation also discussed as L = λ / (√3 a sin θ) for armchair nanoribbons"}
quantities computedtime-averaged local density of states, transmission amplitudes
laser configurationssingle perpendicular circularly polarized laser, two lasers with opposite circular polarizations, two lasers tilted along the same axis, two lasers tilted along orthogonal axes
laser parameters{"frequency":null,"polarization":"linear or circular","incidenceplane":"yz","irradiationplane":"xy","tiltanglesymbol":"θ","wavelengthrelation":"L = λ / sin θ for a single tilted laser; quasi-1D supercell relation also discussed as L = λ / (√3 a sin θ) for armchair nanoribbons"}
quantities computedtime-averaged local density of states, transmission amplitudes
laser configurationssingle perpendicular circularly polarized laser, two lasers with opposite circular polarizations, two lasers tilted along the same axis, two lasers tilted along orthogonal axes
laser parameters{"frequency":null,"polarization":"linear or circular","incidenceplane":"yz","irradiationplane":"xy","tiltanglesymbol":"θ","wavelengthrelation":"L = λ / sin θ for a single tilted laser; quasi-1D supercell relation also discussed as L = λ / (√3 a sin θ) for armchair nanoribbons"}
quantities computedtime-averaged local density of states, transmission amplitudes
laser configurationssingle perpendicular circularly polarized laser, two lasers with opposite circular polarizations, two lasers tilted along the same axis, two lasers tilted along orthogonal axes
