Low-energy effective Dirac theory for graphene in crossed magnetic and in-plane electric fields; analytical solution in terms of parabolic cylinder functions; numerical evaluation of the resulting spectra for zigzag and armchair boundary conditions.
Settings
modelcontinuum Dirac model
regime|beta| <= 1
field geometryperpendicular magnetic field and in-plane electric field
boundary conditionszigzag, armchair
dimensionless field ratiobeta = cE/(vF H)
Conditions
context:theoretical analysis of Landau level collapse
Low-energy effective Dirac theory for graphene in crossed magnetic and in-plane electric fields; analytical solution in terms of parabolic cylinder functions; numerical evaluation of the resulting spectra for zigzag and armchair boundary conditions.
Settings
modelcontinuum Dirac model
regime|beta| <= 1
field geometryperpendicular magnetic field and in-plane electric field
boundary conditionszigzag, armchair
dimensionless field ratiobeta = cE/(vF H)
Conditions
context:theoretical analysis of Landau level collapse
Low-energy effective Dirac theory for graphene in crossed magnetic and in-plane electric fields; analytical solution in terms of parabolic cylinder functions; numerical evaluation of the resulting spectra for zigzag and armchair boundary conditions.
Settings
modelcontinuum Dirac model
regime|beta| <= 1
field geometryperpendicular magnetic field and in-plane electric field
boundary conditionszigzag, armchair
dimensionless field ratiobeta = cE/(vF H)
Conditions
context:theoretical analysis of Landau level collapse
Low-energy effective Dirac theory for graphene in crossed magnetic and in-plane electric fields; analytical solution in terms of parabolic cylinder functions; numerical evaluation of the resulting spectra for zigzag and armchair boundary conditions.
Settings
modelcontinuum Dirac model
regime|beta| <= 1
field geometryperpendicular magnetic field and in-plane electric field
boundary conditionszigzag, armchair
dimensionless field ratiobeta = cE/(vF H)
Conditions
context:theoretical analysis of Landau level collapse