Dear Prof. Baroni:
Thank you very much for your reply.
However, what I wanted to say is, although QE doesn't support frozen-ph as a
"function", it can still be calculated through certain steps. Just as elastic
constant calculation, we can calculate in any DFT code, but only several code
provide
As I know, frozen phonon method is not implemented in QE. You can use frozen-ph
method either by the free software "phon",
http://www.homepages.ucl.ac.uk/~ucfbdxa/, or make it manually like this
tutorial:
http://www.abinit.org/documentation/helpfiles/for-v6.8/tutorial/lesson_rf1.html,
even tho
i am doing the linear response calculation
so how can i do frozen phonon calculation
On Wed, Aug 24, 2011 at 10:54 PM, Mike Mehl wrote:
> To keep from boring everyone, I'm taking this off-line. If anyone else
> wants to participate in the discussion please let me know and I'll add
> you to the
ok but i have seen many papers that this B2 unstability due to some
anaharmonic contributions
or it may be due to band closing phenomenon
can u explain this more correctly because i am doing calculation on
transition metal carbides
On Wed, Aug 24, 2011 at 9:01 PM, Mike Mehl wrote:
> ZnS, WC, and N
On Aug 24, 2011, at 8:21 PM, GAO Zhe wrote:
> As I know, frozen phonon method is not implemented in QE.
???
*ANY* code able to perform total-energy and atomic-force calculations can be
used to do frozen phonons ...
SB
---
Stefano Baroni - SISSA & DEMOCRITOS National Simulation Center - Tri
no i have calculated correctly because the convergence is good with higher k
points
second is that i have tested zns,wc,NiAs phase none of them have less
enthalpy at 130 gpa
other thing is that it is stable at above 250 gpa
On Wed, Aug 24, 2011 at 7:38 PM, Mike Mehl wrote:
> If the B1 structure
To keep from boring everyone, I'm taking this off-line. If anyone else
wants to participate in the discussion please let me know and I'll add
you to the conversation.
On 08/24/2011 01:07 PM, bhabya sahoo wrote:
> ok but i have seen many papers that this B2 unstability due to some
> anaharmonic
ZnS, WC, and NiAs are the likeliest candidates, but not the only ones.
The unstable B1 phonons lead to structures which relax to something
lower in energy than B1. Since all of your candidate structures have a
higher enthalpy than B1 at 130 GPa, it can't be one of those structures.
Hence, it
If the B1 structure is unstable with respect to the B2 structure above
130 GPa, but the B2 structure is dynamically unstable at and above 130
GPa, there are two possible conclusions:
1) The phonons for the B2 structure were not calculated accurately, or
2) There is a competing structure that is
sir
i am calculating the phase transition of some carbides
the transition from B1 to B2 transition occures at 130 gpa by enthalpy
compparison
but i am able to find phonon instability at 130 gpa for B1 structure
but at the same time i am not able to find the dyanamic stability of B2
phase
but it occ
On Aug 23, 2011, at 8:40 PM, bhabya sahoo wrote:
> sir
???
> i am calculating the phase transition of some carbides
> the transition from B1 to B2 transition occures at 130 gpa by enthalpy
> compparison
OK
> but i am able to find phonon instability at 130 gpa for B1 structure
you mean, a p
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