Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Graphene sheet modeled as a 2D Dirac material with impurity scattering rate Gamma and mass gap m, used to compute polarization tensor, conductivity, and Casimir interaction.
No measurements recorded
SimulatedCStudied Material
Casimir interaction configuration of graphene against an ideal conductor.
No measurements recorded
SimulatedCStudied Materialideal conductorReference Material
Materials
graphene
C
Studied Material
Variables
model= Dirac quasiparticles
mass_gap= m
chemical_potential= 0
impurity_scattering_rate= Gamma
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.
Graphene sheet modeled as a 2D Dirac material with impurity scattering rate Gamma and mass gap m, used to compute polarization tensor, conductivity, and Casimir interaction.
No measurements recorded
SimulatedCStudied Material
Casimir interaction configuration of graphene against an ideal conductor.
No measurements recorded
SimulatedCStudied Materialideal conductorReference Material
Materials
graphene
C
Studied Material
Variables
model= Dirac quasiparticles
mass_gap= m
chemical_potential= 0
impurity_scattering_rate= Gamma
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.
Graphene sheet modeled as a 2D Dirac material with impurity scattering rate Gamma and mass gap m, used to compute polarization tensor, conductivity, and Casimir interaction.
No measurements recorded
SimulatedCStudied Material
Casimir interaction configuration of graphene against an ideal conductor.
No measurements recorded
SimulatedCStudied Materialideal conductorReference Material
Materials
graphene
C
Studied Material
Variables
model= Dirac quasiparticles
mass_gap= m
chemical_potential= 0
impurity_scattering_rate= Gamma
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.
Graphene sheet modeled as a 2D Dirac material with impurity scattering rate Gamma and mass gap m, used to compute polarization tensor, conductivity, and Casimir interaction.
No measurements recorded
SimulatedCStudied Material
Casimir interaction configuration of graphene against an ideal conductor.
No measurements recorded
SimulatedCStudied Materialideal conductorReference Material
Materials
graphene
C
Studied Material
Variables
model= Dirac quasiparticles
mass_gap= m
chemical_potential= 0
impurity_scattering_rate= Gamma
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Analytical quantum field-theoretic calculation of the graphene polarization tensor with impurity scattering rate Gamma, Pauli-Villars regularization, conductivity derivation, and numerical evaluation of Casimir energy density via the Lifshitz formula.
Analytical quantum field-theoretic calculation of the graphene polarization tensor with impurity scattering rate Gamma, Pauli-Villars regularization, conductivity derivation, and numerical evaluation of Casimir energy density via the Lifshitz formula.
Analytical quantum field-theoretic calculation of the graphene polarization tensor with impurity scattering rate Gamma, Pauli-Villars regularization, conductivity derivation, and numerical evaluation of Casimir energy density via the Lifshitz formula.
Analytical quantum field-theoretic calculation of the graphene polarization tensor with impurity scattering rate Gamma, Pauli-Villars regularization, conductivity derivation, and numerical evaluation of Casimir energy density via the Lifshitz formula.
