Graphene is a 2D material with very particular dielectric properties. For different wave ranges and different doping dielectric permittivity (depends on frequency) can be negative (i.e. graphene behaves itself like a metal) or positive (i.e dielectric) with low damping (2.3%). The dielectric permittivity can be calculated from conductivity through relation ε = 1 +i*σ/(δωε0), where δ is a thickness of the graphene layer. Conductivity σ is calculated using random phase approximation and final formula can be found in a lot of sources.
Most of Dielectric Constant requires when you use the material as insulator between channel and gate. As much as I know, Graphene can't be used for that if it has zero band gap. Silicon Dioxide, Hofnium Dioxides, Boron etc are used for that.
I would like to know why you need this value.
I am very sorry, if my answer doesnt help you much. By the way the attachments might help you.
Graphene is a 2D material with very particular dielectric properties. For different wave ranges and different doping dielectric permittivity (depends on frequency) can be negative (i.e. graphene behaves itself like a metal) or positive (i.e dielectric) with low damping (2.3%). The dielectric permittivity can be calculated from conductivity through relation ε = 1 +i*σ/(δωε0), where δ is a thickness of the graphene layer. Conductivity σ is calculated using random phase approximation and final formula can be found in a lot of sources.
I am not sure you still need this information. Anyway check this following link. In this work, they showed field dependence of dielectric constant. Hoping this might help.
I recently did some work on revealing the static and spatially-resolved dielectric constant of graphene and graphene nanoribbons. My original intention is also trying to provide the dielectric constant when simulating graphene devices.
I have question, in Terahertz frequency below far infrared, when we consider just intraband transition, is real part of Graphene permittivity negative or positive?
I see two different Kubo formula in the papers, one of them reach to negative and another to positive real part of permittivity.
It really depends on the features of your Graphene such as Fermi level and the thickness, for instance , for the Fermi level equal to zero and the thickness less than 1 micro is for sure negative.
Thanks so much, Jingtian. I am also wondering if this quantity of dielectric constant is appropriate for both of the perpendicular and parallel cases? I mean whether there would be some significant differences when considering longitudinal electric field and Transverse electric field within graphene?
I am thinking because the density of states of graphene is approaching to zero near Dirac point,which is extremely small compared to that of common semi-conductors, the fermi surface can be tuned easily through charge doping. Thus, the dielectric permittivity has a strong dependence with carrier density. So, when applying bias to graphene, what the static dielectric permittivity could change into?
I am actually now working on a method trying to resolve the dielectric screening when the electric field is applied parallel to the atomic plane for 2D materials and when the electric field is applied along the periodic direction for 1D materials. It should come up in the coming half a year. I have already gotten some good results. Regarding the effect of carrier density on the dielectric permittivity, I am not sure I understand your arguments. In my opinion, the carrier density should not affect the permittivity. The dielectric matrix depends on the whole details of the band structure and wavefunctions, instead of only the values around the Dirac points. I will update here once I have the results for in-plane screening published.
You can refer to this article for now: "First-principles theory of nonlocal screening in graphene", PHYSICAL REVIEW B 83, 081409(R) (2011). Although it did not present the position dependence, it presents the q-dependence of the transverse dielectric function. I think this can be useful for you.