el-ph matrix elements in polar materials
Posted: Wed Jun 14, 2017 4:48 pm
Dear all,
In the following paper it is stated that g (el-ph matrix elements) are separated into short- and long-range contributions where then the short-range contribution is dealt with standard wannier interpolation and both contributions are added up after interpolation at arbitrary k and q points (fine grid?)
https://journals.aps.org/prl/pdf/10.110 ... 115.176401
My question is that how is then the long-range contribution is treated? Is this part calculated within QE?
Also, for polar 2D material it is then believed that the Frohlich interaction should be treated differently when we are in long wave length limit (q<1/|d| where d is the interlayer distance):
https://journals.aps.org/prb/pdf/10.110 ... .94.085415
In fact it is then understood that the diverging behavior of g matrix elements are the result of non-zero interaction between the images of the 2D system, resembling the behavior of a bulk system. Therefore this group have suggested the modification of Coulomb potential within the QE code (they have used the QE code for g matrix elements calculation).
My question is that: is this what happens in EPW too? And is there a way to prevent this feature and implement the same procedure as they have done but in EPW? or, one also has to consider the QE modification?
I have done calculation on monolayer MoS2 and I observed diverging behavior in there near \Gamma point for phonons.
Many thanks,
Zahra
In the following paper it is stated that g (el-ph matrix elements) are separated into short- and long-range contributions where then the short-range contribution is dealt with standard wannier interpolation and both contributions are added up after interpolation at arbitrary k and q points (fine grid?)
https://journals.aps.org/prl/pdf/10.110 ... 115.176401
My question is that how is then the long-range contribution is treated? Is this part calculated within QE?
Also, for polar 2D material it is then believed that the Frohlich interaction should be treated differently when we are in long wave length limit (q<1/|d| where d is the interlayer distance):
https://journals.aps.org/prb/pdf/10.110 ... .94.085415
In fact it is then understood that the diverging behavior of g matrix elements are the result of non-zero interaction between the images of the 2D system, resembling the behavior of a bulk system. Therefore this group have suggested the modification of Coulomb potential within the QE code (they have used the QE code for g matrix elements calculation).
My question is that: is this what happens in EPW too? And is there a way to prevent this feature and implement the same procedure as they have done but in EPW? or, one also has to consider the QE modification?
I have done calculation on monolayer MoS2 and I observed diverging behavior in there near \Gamma point for phonons.
Many thanks,
Zahra