Graphene - Green's function technique

Click For Summary
The discussion focuses on the application of Matsubara Green's function technique to graphene, specifically addressing the complexities arising from its two sublattices, A and B. Participants express confusion over which Green's functions to use when calculating the screened Coulomb potential and evaluating the polarization bubble. The importance of locality in the context of graphene is highlighted, with suggestions to refer to specific sections of relevant reviews for clarification. A request for further explanation on a particular equation related to the Green's functions is also made, indicating a need for more detailed analysis. Overall, the conversation emphasizes the intricacies of Green's function techniques in graphene studies.
csopi
Messages
81
Reaction score
2
Graphene -- Green's function technique

Hi,

I am looking for a comprehensive review about using Matsubara Green's function technique for graphene (or at least some hints in the following problem). I have already learned some finite temperature Green's function technique, but only the basics.

What confuses me is that graphene has two sublattices (say A and B), and so (in principle) we have four non-interacting Green's functions: G_{AA}(k,\tau)=-\langle T_{\tau}a_k(\tau)a_k^{\dagger}(0)\rangle, ,

where a_k is the annihilation operator acting on the A sublattice. G_{AB}, G_{BA} and G_{BB} are defined in a similar way.

Of course, there are connections between them, but G_{AA} and G_{AB} are essentially different. Now when I am to compute e.g. the screened Coulomb potential, I do not know, which Green's function should be used to evaluate the polarization bubble.

Thank you for your help!
 
Physics news on Phys.org


I think you will find the answer you are looking for when you consider the expression for the bubble in coordinate space.
 


Dear DrDu,

thank you for your response, but I do not think, I understand how your suggestion helps me. Please explain it to me a bit more thoroughly.
 


I mean that the electromagnetic field couples locally to the electrons. Hence the bubble is some integral containing a product of two Greensfunctions G(x,x')G(x,x'). What consequences does locality have in the case of Graphene?
 


Dear tejas777,

This is a very nice review, thank you very much. Let me ask just one final question: can you explain, how comes
F_{s,s'}(p,q)

in eq. (2.12) and (2.13) ?
 


Look at section 6.2 (on page 19/23) in:

http://nanohub.org/resources/7436/download/Notes_on_low_field_transport_in_graphene.pdf

Now, the link contains a specific example. You can probably use this type of approach to derive a more general expression, one involving the ##s## and ##s'##. I may have read an actual journal article containing the rigorous analysis, but I cannot recall which one it was at the moment. If I am able to find that article I will post it here asap.
 

Similar threads

  • · Replies 7 ·
Replies
7
Views
1K
Replies
1
Views
2K
  • · Replies 12 ·
Replies
12
Views
3K
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 175 ·
6
Replies
175
Views
26K
  • · Replies 5 ·
Replies
5
Views
11K
  • · Replies 3 ·
Replies
3
Views
2K