Dear Prof. Tran and Prof. Abo,
Thank you very much for your kindly reply.
The 4*4*1 supercell (including 64 atoms) I want to calculate is really large.
When I set the h-BN monolayer 3*3*1 supercell including 36 atoms, the
calculation can be successfully completed.
At present, I am doing a
Dear Prof. Fabien??
Thank you very much for reading and helping to solve my question.
I opened the file output.log, and there was only one line in it:
stop error
I found the output.log file for a previous successful example of hybrid
functional computation, which shows the following:
Dear Wien2k developers??
I want to ask a question about the calculation error of hybrid functional by
email. I am very sorry that I wrote the wrong name of the question. It appeared
in "How to select the appropriate nband in hybrid functionals calculations"
he content of hf.error is:
** Error in Parallel HF
** testerror: Error in Parallel HF
And the content of file from hf_1.error to hf_5.error is:
error in hf
Thank you again for reading my question. Any suggestions are welcome??
Yifan Ding
Institute of Physics, Chinese Academy of Science (CAS)
Add
Dear Prof. Blaha??
Thank you very much for your kindly reply.
While browsing previous discussions, I noticed that the DOS energy range of
LDA/GGA calculation is determined by case.in1, and the DOS energy range of
hybrid functional calculation has nothing to do with case.in1, but is related
Dear Wien2k developers??
When YS-PBE0 is used to calculate the DOS of pristine h-BN, the problem I
encounter is that I don't know how to select the appropriate nband to obtain
the DOS of energy window -20 eV ~ 20 eV.
At first, I calculated the DOS of pristine h-BN using PBE96. The emin and
Dear Prof. Blaha,
I will follow your instructions. Thank you very much!
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By doing structural optimization ([4] VARY B/A RATIO with CONSTANT VOLUME and
C/A (orthorh lattice)), I found that when 11 different structures were set
(vary B/A ratio: -5%,-4%,-3%,-2%,-1%, 0, 1%, 2%, 3%, 4%, 5%), the same number
of total k-points in full BZ caused different the number of
Dear Dr Fabien Tran,
Thank you very much for your very clear explanation. Then all my confusions
have been cleared.
Ding
On Mon, 4 May 2020 at 11:24 pm, Tran, Fabien
wrote:
> The way lstart works to generate case.sigma may be a bit confusing. The
> Ecut asked by lstart does not
ould manually change included file names in lstart.def (add both
"case.inst_sigma" and "case.inst" in it)?
Many thanks and sorry for asking so many questions, which may seem to be silly.
Ding
> On 4 May 2020, at 7:26 pm, Tran, Fabien wrote:
>
> Hi,
> Ideally, the integrate
if this sampling issue will
affect the correctness of the charge density as well as the net difference
charge density in the unit cell.
Many thanks,
Ding
> On 3 May 2020, at 2:50 am, Tran, Fabien wrote:
>
> If I'm not wrong (I have never tried this combination of keywords), you
densities
(option “Over”.
Can I ask if this is correct way to do the calculation of the difference
charge density for magnetic materials? and also if there is an automatic
option to directly calculate it in Wien2k “, just like option “Diff” for
non-magnetic materials ?
Many thanks,
Ding
On Sun, 3 May
o many questions in this email.
Best regards,
Ding
> On 2 May 2020, at 10:12 pm, Tran, Fabien wrote:
>
> From your output2, we can see that you discarded the states that are below
> -0.3 Ry
> (the occupancy in the last column is zero for them) to calculate the electron
> density.
of the whole
valence electrons should be set slightly above Emax of energy band 10,
which is -0.2916?
Many thanks,
Ding
On Mon, 27 Apr 2020 at 16:25, Peter Blaha
wrote:
> For a difference density it is of course necessary that you treat the
> same states in the solids and in the atom.
&
Dear Dr Fabien Tran,
Thanks for your reply. Your explanation is very clear and helpful!
Ding
On Sat, 2 May 2020 at 18:49, Tran, Fabien wrote:
> Hi,
>
> The valence orbitals can also extend in the region (very) close to the
> nucleus.
> An example is given in Fig. 4 in o
in the bonding (please correct me if I'm wrong). But what I can see
from the graph is very deep purple-coloured region at the centre of the Ti
site, which suggests a dense accumulation of electrons at the Ti site. So could
I ask why the difference charge densities in this "round region&quo
the difference charge densities in Ti are positive. So can
someone explain why the difference charge densities in Ti core are very
positive?
Sorry for asking this question that may look stupid.
Many thanks,
Ding
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Dear Prof Peter Blaha,
Thank you very much for your detailed explanation.
Many thanks,
Ding
On Mon, 27 Apr 2020 at 4:25 pm, Peter Blaha
wrote:
> For a difference density it is of course necessary that you treat the
> same states in the solids and in the atom.
> While in an atom this
he results in case.scf1.
Look forward to the answers.
Many thanks,
Ding
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of structure factors by lapw3 or
other component subprograms of Wien2k?
Many thanks in advance,
Ding
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in Appendix.
(PS: Dear Professor Peter Blaha, sorry for creating a new topic as I think
it is essential to get a new title to highlight my question.)
Many thanks,
Ding
Appendix:
SIN O/L (A-1)Fg (HF by Wien2k)Fg
(conventional HF)
0.239697 21.680524 22.072255
0.27
re factors are completely wrong
compared to the electron structure factors converted from X-ray structure
factors by Mott formula. I don't know if it is wrong to generate electron
structure factors with lapw3 by directly copying case.vcoul to case.clmsum.
Thank you for your help!
Best reg
I am running wien version 14 on a machine of type DELL with operating system
Fedora, fortran compiler 2013 and math libraries mkl
The purpose of my calculations is to test the dftd3 bandstructure dispersive
correction in Wien2k.
According to the userguide, I download and compile the dftd3
.
On Thu, Apr 21, 2016 at 5:44 PM, ding <dingming...@qq.com> wrote:
Dear WIEN2K users,
I want to force everything but only one atom d states to be
non-spinpolarized. For example, there are two Fe atoms in a unit cell, and I
want to keep only one Fe atom to be spinpolarized, while the
Dear WIEN2K users,
I want to force everything but only one atom d states to be
non-spinpolarized. For example, there are two Fe atoms in a unit cell, and I
want to keep only one Fe atom to be spinpolarized, while the other to be
non-spinpolarized. Would anyone tell me how to carry out this
Dear saurabh,
Maybe you should copy the case.indm to case.indmc.
Mingcui
-- --
??: "saurabh singh";;
: 2015??10??24??(??) 8:35
??: "wien";
:
Dear all I am calculating the density of states of the bcc iron, the lattice
parameter is 5.416902 Bohr, the space group is NO. 229, the problem I
encoutered is that when calculating the density of states, the plotted range of
energy is alway less than the Fermi level,
I see in the case.int
of bcc iron
Sometimes you have to increase the emax in case.in1
K-VECTORS FROM UNIT:4 -7.0 ***2.5***13 red emin/emax/nband
De: wien-boun...@zeus.theochem.tuwien.ac.at
wien-boun...@zeus.theochem.tuwien.ac.at en nombre de ding dingming...@qq.com
Enviado: jueves, 24 de julio
Dear Silke,
Thanks for your reply, I want to calculate the Hund's rule coupling J of p
orbitals in Graphene.
Best,
Mingcui Ding
-- Original --
From: Peter Blaha;pbl...@theochem.tuwien.ac.at;
Date: Wed, Apr 23, 2014 00:55 AM
To: A Mailing list for WIEN2k
Dear all,
I want to calculate the effective hund's rule coupling of atom, is there a
method to the effective hund's rule coupling by wien2k? I know one can use
constraint LDA to calculate the effective U.
Thanks
Mingcui Ding
Tongji University
Dear Wannier users,
How to apply symmetry protection in Wannier 90 code? The unit cell is
LaFeAsO, the space group is 129_P4/nmm, and one unit cell contains two
equivalent Fe atoms. I use the 10 Fe 3d orbitals to get the effecitve tight
binding Hamiltionian. But I found that the
Dear all,
What does restart in the case.dayfile mean as is shown in the following:
:ENERGY convergence: 1 0.1 .00185000
:CHARGE convergence: 1 0.1 -.052
restart
stop
Best wishes!
Mingcui
Tongji university,China
-- next part --
in advance for your help,
--
Yang Ding
http://www.aps.anl.gov/Users/Scientific_Interest_Groups/HPSynC/people/%7EYDing.html
Staff Scientist
RM-B3180/Blgd-401
HPSynC at Advanced Photon Source
Argonne National Laboratory
9700 S. Cass Avenue
Argonne, IL 60439
Phone: 630-252-6288
Email: yangding
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