Dear Venkataramana,
apart from the tips Pietro gave it is clear to me that you get differences
between QE and VASP. You're not using the same XC functional. PW91 and PBE
are not the same and as far as I remember they differ more for stuff like
surfaces or "reaction" barriers... Just search for pa
Dear Erland (?)
In the last line of your Cu.bands.in it should be "0 0 0 1" as
there is no additional point, but I don't know if this is the
origin of your problem. If not, we need more information, e.g.,
the version you're using, maybe part of the output (especially
with respect to the point abo
gets a "weight" of 1 as there is
no additional point.
Regards
Thomas
Zitat von Manu Hegde :
looks like K-point units, please double check it.
Manu
On Sun, Apr 29, 2018 at 1:58 PM, Dr. Thomas Brumme <
thomas.bru...@uni-leipzig.de> wrote:
Dear Erland (?)
In the last line of
Dear Stefan,
you can't calculate the band structure using a self-consistent calculation.
This would mean that you search for the ground-state density (scf) whilst
your integrations in k-space are done on a very sparse grid... On the other
hand you can't calculate the band structure for hybrid fun
Dear Chris,
The potential shows the typical quadratic dependence on z since you're
calculating a charged system - there is a homogeneous background
charge since the 3D pbc system is assumed to be neutral. This has
nothing to do with the dipole correction. Depending on what you want
to do
nk that is what they recommend.
Best,
Chris
On Thu, Jun 28, 2018 at 7:04 PM, Dr. Thomas Brumme <
thomas.bru...@uni-leipzig.de> wrote:
Dear Chris,
The potential shows the typical quadratic dependence on z since you're
calculating a charged system - there is a homogeneous background ch
utput
(attached) wrong.
One way that gives me a flat vacuum potential is to use the M-P scheme but
that only works for cubic systems. After reading about the implementation
in VASP a bit I also think that is what they recommend.
Best,
Chris
On Thu, Jun 28, 2018 at 7:04 PM, Dr. Thomas Brumme <
th
Dear Alex,
if your is non-periodic in one direction (with the vacuum and the
artificial dip due to the field and dipole correction) there is no
reason to put k-points in this direction - you just increase the
computation time to get bands with no dispersion at all in this
direction. At least I th
Dear Asad,
about the order I'm not sure, but with SOC you cannot think of px or
py or dxy anymore.
For more details, see e.g. this paper:
https://journals.aps.org/prb/abstract/10.1103/PhysRevB.71.115106
working through the math you'll see that every, e.g., d-state can and
will couple to
a
Dear Lucas,
please have a look at the input description for the k-points list
and then look at your input for the bands calculation. I guess the
code assumes 0 lines for the bands as the first number in the first
line is a "0".
If you want a path along (G M K G) you should have something like:
K
Both methods should give the same result - they did at least when I
tried. But you can't calculate phonons with dipole correction so if
you want those start with assume_isolated = '2D'
But read all infos given in input_pw and the related papers - it helps
to understand how to setup the system
One can use restart_mode='restart' together with startingpot='atomic'
and startingwfc='atomic+random'... This will trick the code to use the
positions but starting with the standard starting potential and wave
functions. But be careful: the code also reads in other variables such
as electri
Dear Mohammad,
first of all: if you have problems/questions regarding BoltzTraP it might be a
good idea to ask the authors or in their google users group. See also the
web page of the new BoltzTraP2 program:
https://www.imc.tuwien.ac.at/index.php?id=21094
For the specific question using BoltzTr
Dear Anuja Chanana,
I don't think it is the pseudo which gives problems in one case and none
in the other. Looking at the structure I guess that you want to
simulate an isolated
layer in the hexagonal system, don't you? Otherwise it would make no
sense to have a vacuum of 6 Angstrom. But then,
Please, always reply to "All", i.e., also to the list, so that
others can
find the answer if they have the same problem.
Zitat von Anuja Chanana :
Dear Dr. Thomas Brumme,
Thanks for the information.
I tested the pseudopotential for bulk BN hexagonal system as well. But its
difficul
Dear Paolo,
thanks for the suggestion which I also found in the mail archive but I'm also
wondering why it was working with older versions of the code but not with
newer. Also, I don't understand what should be the problem with the input.
Sure, it is a large system, but on the other hand I alread
.
Thomas
Zitat von "Dr. Thomas Brumme" :
Dear Paolo,
thanks for the suggestion which I also found in the mail archive but I'm also
wondering why it was working with older versions of the code but not with
newer. Also, I don't understand what should be the problem with the input.
Dear Ankit,
this discussion might help:
https://www.mail-archive.com/users@lists.quantum-espresso.org/msg33771.html
Regards
Thomas
Zitat von Ankit Jain :
Dear users,
I have been trying to collect and merge .dvscf files from a grid
example of ph.x and combine these files into a single fi
Dear Julien,
Maybe it's because your cell vectors 1 and 2 are pointing
slightly in the z direction? I don't know but I think this
could be a problem. If it is just a rotation of the whole
cell you could try rotating it back... Otherwise search the
code for the message and look when it is trigger
Dear Bin,
I can't check your input thoroughly as I'm on vacation, but there are
2 things I noticed:
1. The doping seems quite high - maybe you're close to the van Hove
singularity which could explain problems. Can you try with less doping
and then - if this converges - increase the doping
we do this by setting calculation =
‘relax-vc’ or by calculating the curve of energy vs. lattice constant?
Best,
Bin
From: Dr. Thomas Brumme
Sent: Monday, September 16, 2019 7:42:59 PM
To: Quantum ESPRESSO users Forum ;
bshao...@outlook.com
Subject: Re
Dear Hussain,
Remember that the Fermi surface of a 3D bulk material is a 2D surface
in 3D space (kx, ky, kz). Thus, the Fermi surface of a 2D system is
an 1D line/curve on a 2D plane (kx, ky). The bxsf file format only
works nicely for 3D systems. You can however trick a little bit.
Instead of sp
Well, it should work and do exactly what it says but it won't respect
the hexagonal symmetry which might be problematic if you want to
enforce it. What do you mean with "not appropriate"?
You could also relax the in-plane constant by hand and in this way
keep the hexagonal symmetry - just mak
Dear Jibiao,
1. You didn't tell us what you want to do and just claimed that QE is
wrong for a molecule.
2. You wrote "[...] results from QE 5.1 are completely wrong [...]
results from QE 6.1 is also unsatisfying; the 2pz states should not be
populated at a deep level below -28 eV? "
3. I to
Dear Gautam,
here is a link:
http://lmgtfy.com/?q=crystal+structure+TMDs
or if you don't have access to Google you can also use:
http://lmgtfy.com/?s=b&q=Crystal+structure+TMDs
Regards
Thomas
Zitat von Gautam Gaddemane :
> Hello All,
> I am new to Quantum Espresso and in general to DFT and
Dear B. S. Bushan,
the pDOS is created via projection of the eigenfunctions on the atomic
orbitals given
in the pseudopotential as those states are included in the
calculation. You're using
pseudos with semicore states. Thus, for, e.g., Mo there are the 4s 4p
4d 5s 5p states.
If you look at
Dear Bibhas,
reducing the mixing_beta helps with the convergence - I reduced it to
0.3 and the optimization is running for at least 5 steps... However,
at a certain point this could happen again (convergence problems) due
to charge "jumping" back and forth between atoms - try reducing
mixi
Dear Sohail,
bilayer PdS2 becomes metallic and thus you need to change from
occupations='fixed' to 'smearing'...
See also:
http://onlinelibrary.wiley.com/doi/10.1002/anie.201309280/full
Regards
Thomas Brumme
Zitat von Sohail Ahmad :
I wish to apply electric field in Z direction to bilayer
TIONS angstrom
Pd 0.
0. 0.
S 1.76627922
1.01975766 1.28191684
S 1.76627922
-1.01975766 -1.28191684
Pd 0.
0. 6.6000
S 1.76627922
1.01975766 7.88191684
S 1.76627922
-1.01975766 5.31808316
K_POINTS AU
Dear Pascal,
If the non-SOC calculation converged, try to replace the pseudos one
by one with the relativistic ones - I know for example that the
relativistic tungsten potential of the PS library had (has?) some
problems. You could have the same problem. If it is a specific pseudo
we can
es and different
pseudopotentials (in line to what Thomas proposed).
Marko
From: users <mailto:users-boun...@lists.quantum-espresso.org>> on behalf of Dr.
Thomas Brumme <mailto:thomas.bru...@uni-leipzig.de>>
Sent: Thursday, December 19, 2019 7:03:2
Dear Chris,
within the Tersoff-Hamann approximation the STM image is proportional
to the integral of the local density of states integrated from the
Fermi energy till the bias voltage:
https://journals.aps.org/prb/abstract/10.1103/PhysRevB.31.805
As far as I remember, the method implemented in
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