Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Graphene monolayer in an ATR optical stack with a semi-infinite dielectric prism, a finite dielectric spacer layer, and a semi-infinite dielectric substrate; excitation is by TM-polarized evanescent waves under total internal reflection.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Graphene monolayer in an ATR optical stack with a semi-infinite dielectric prism, a finite dielectric spacer layer, and a semi-infinite dielectric substrate; excitation is by TM-polarized evanescent waves under total internal reflection.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Graphene monolayer in an ATR optical stack with a semi-infinite dielectric prism, a finite dielectric spacer layer, and a semi-infinite dielectric substrate; excitation is by TM-polarized evanescent waves under total internal reflection.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Graphene monolayer in an ATR optical stack with a semi-infinite dielectric prism, a finite dielectric spacer layer, and a semi-infinite dielectric substrate; excitation is by TM-polarized evanescent waves under total internal reflection.
Analytical electromagnetic-field solution for a layered ATR geometry combined with a Boltzmann-transport-based derivation of the graphene nonlinear current and second-harmonic response.
Settings
modelMaxwell equations + Boltzmann transport equation
approachperturbative expansion in electric field
geometryATR
validationnull
polarizationTM
graphene modelDirac cone approximation
harmonic orders1, 2
substrate responselinear dielectric
temperature assumptionzero temperature
Conditions
context:theoretical SHG enhancement in graphene via SPP excitation
Analytical electromagnetic-field solution for a layered ATR geometry combined with a Boltzmann-transport-based derivation of the graphene nonlinear current and second-harmonic response.
Settings
modelMaxwell equations + Boltzmann transport equation
approachperturbative expansion in electric field
geometryATR
validationnull
polarizationTM
graphene modelDirac cone approximation
harmonic orders1, 2
substrate responselinear dielectric
temperature assumptionzero temperature
Conditions
context:theoretical SHG enhancement in graphene via SPP excitation
Analytical electromagnetic-field solution for a layered ATR geometry combined with a Boltzmann-transport-based derivation of the graphene nonlinear current and second-harmonic response.
Settings
modelMaxwell equations + Boltzmann transport equation
approachperturbative expansion in electric field
geometryATR
validationnull
polarizationTM
graphene modelDirac cone approximation
harmonic orders1, 2
substrate responselinear dielectric
temperature assumptionzero temperature
Conditions
context:theoretical SHG enhancement in graphene via SPP excitation
Analytical electromagnetic-field solution for a layered ATR geometry combined with a Boltzmann-transport-based derivation of the graphene nonlinear current and second-harmonic response.
Settings
modelMaxwell equations + Boltzmann transport equation
approachperturbative expansion in electric field
geometryATR
validationnull
polarizationTM
graphene modelDirac cone approximation
harmonic orders1, 2
substrate responselinear dielectric
temperature assumptionzero temperature
Conditions
context:theoretical SHG enhancement in graphene via SPP excitation