in the small and large unit cells. In this case
some numerical noise (e.g., from the FFTs) can introduce some errors.
But actually, what do you mean by I can't compare?
My recommendation: use the same unit cell.
F. Tran
On Tue, 10 Jul 2012, David Tompsett wrote:
Dear All,
I have
and
symmetry as for the low symmetry. Why is this the case? What is the effect
of having different sized unit cells?
Thank you,
David Tompsett.
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VESTA (http://jp-minerals.org/vesta/en/) also has good utilities for
letting you redefine the unit cell vectors via a matrix transformation.
David.
On Sat, Jun 30, 2012 at 5:59 AM, Laurence Marks L-marks at
northwestern.eduwrote:
Try cryscon (http://www.shapesoftware.com), perhaps also
Blaha pblaha at
theochem.tuwien.ac.atwrote:
You have to check directly in the code. Without looking in the code I do
not know what r-index = 11 should do ? I guess this is not a documented
option, but Pavel Novak migth have put in something
Am 06.06.2012 14:11, schrieb David Tompsett
104670.12 (large number)
Adding a negative sign will change the calculation:
RINDEX = -11 = 1/r**krad for krad 10 = :XOP ? (small number)
File of reference: $WIENROOT/SRC_lapwdm/radint.f
On 6/7/2012 7:08 AM, David Tompsett wrote:
Hi Peter,
Thanks for the response. The option r-index = 11
Dear All,
I have been attempting to use lapwdm to obtain the expectation value of the
radial distribution of orbitals i.e. r.
I have attempted the simplest case that I could think of, the hydrogen atom
in a large cell. I used an RMT of 4.5 au so that a fraction 0.99 of the
charge lies inside the
Dear All,
I need a little help with the program lapwdm.
I am trying to quantify the radial extent of d-orbitals of manganese ions.
I wanted to use the expectation value r calculated by lapwdm using
RINDEX=11, LSINDEX=1.
I am not using SO-coupling and am using the latest release of Wien2k.
A
.
With kind regards,
K. Balamurugan.
David Tompsett.
--
*K. Balamurugan
Pittsburgh, USA.
+1 412 961 5055*
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Dear All,
Has anyone implemented a way to calculate the hyperfine field due to
dipolar interactions between the nuclear spin and the electron spin density
outside the muffin tin sphere? This is referred to as B_lat in Pavel
Novak's notes on hyperfine calculations in Wien2k.
Many thanks,
David
Dear All,
There have been several discussions over the past year regarding errors of
LOPW plane waves exhausted in high symmetry cells. I have recently come
across the same problems in a cubic (space group 212) cell. I could only
avoid them by taking RKmax up to 9.5. This however, seems to be
the eigenvalues should be. Has anyone seen such a problem before? Also,
which part of the source code should print these eigenvalues? I would like
to check if the problem is with IO by trying to flush the stream.
Many thanks,
David Tompsett.
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not consistent with Z
edit Elemant120.inst and rerun lstart afterwards or change Z in StructGen!
If I try to put 5g states into case.inst (for element #120) lstart stops
with a format error.
Thank you,
David Tompsett.
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Dear All,
I am considering calculations of magnetic order in transition metal anion
compounds. Is anyone aware of cases where DFT+U predicts the wrong magnetic
order compared to experiment, but where hybrids predict correctly?
Thank you,
David Tompsett.
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. to partial
occupancies?
Therefore, can I trust the calculated forces in a metallic system?
Can I use the total energy from Tetra for metals reliably?
Many thanks for any help,
David Tompsett.
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Hi Laurence,
Is there any explanation or reference as to why they are OK? The Bloch paper
suggests that they won't be.
Cheers,
David.
2011/7/28 Laurence Marks L-marks at northwestern.edu
The forces are fine.
On Jul 28, 2011 4:55 AM, David Tompsett dat36 at cam.ac.uk wrote:
Dear All,
I
30 of that
paper. Is any in particular difficult for LAPW methods?
Many thanks,
David Tompsett.
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Dear Alay,
DFT+U is more than just a SIC correction method. It corrects some
self-interaction, but also incorporates Hartree-Fock effects via a Coulomb
matrix. See PHYSICAL REVIEW B 79, 035103 (2009).
To tread both d and f electrons try:
EuTe.inorb
1 1 0nmod, natorb, ipr
Hi Shamik,
Sayed's advice is good. There are also some procedures based on Fixed spin
moment calculations. You will have to think carefully about whether your
system is metallic or locaised type. The links in the appendix to this paper
should help:
Ylvisaker and Pickett, PHYSICAL REVIEW B 79,
?
Many thanks,
David Tompsett.
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, but don't understand why I see the
warning here. Does anyone know what the cause is? I am running using MPI
parallel over 24 cores. Will the parallelisation setup affect this cluster
size problem?
Thank you,
David Tompsett.
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atoms are light, so I expected the RLO's
would have little effect.
I did sensible things like converge with respect to the emax in case.in1,
k-points, IFFT factor=4.
Many thanks for your help,
David Tompsett.
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strategy more
generally?
Many thanks,
David Tompsett.
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.storage.cluster node-h18.storage.cluster
1:node-h17.storage.cluster node-h17.storage.cluster
1:node-h17.storage.cluster node-h17.storage.cluster
granularity:1
extrafine:1
lapw2_vector_split:1
Many thanks,
David Tompsett.
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Dear All,
I am performing calculations on slabs of the material LiFePO4 using GGA+U in
the latest Wien2k release.
To perform min_lapw internal parameter optimisation I reduce the RMT's and
use R=1.06 for Phosphorus. This results in a need to reduce the default for
energy separation of core
Dear Fhokrul,
With only one k-point you should only have a discrete set of energies.
Therefore I think the DOS would be a set of delta functions. Your energy
resolution in case.int is unlikely to capture them.
Best,
David.
Md. Fhokrul Islam wrote:
Dear Wien2k users,
I am trying to
Dear Jian-Xin,
The Fermi surface can not be plotted from a parallel calculation because
XCrysden needs the eigenvalues from a single case.output1* file. From a
parallel calculation a separate case.output1* file is produced for each cpu.
So to solve the problem you need to write a small script
Dear All,
After recently updating to the latest version of Wien2k I found that the
lapwdmc executable had not been produced, but the real version had been.
I copy the compile.msg below from SRC_lapwdm/. Does anyone know how I
can fix this problem?
Thank you,
David.
--
David A. Tompsett
at the
link above. Thus it may appear that one's code is working well and then
odd errors will occur for particular cases.
After rebuilding my Wien2k with either old MKL 9.1 or the latest
10.2.2.025 the problems disappeared.
Best wishes,
David Tompsett.
--
David A. Tompsett
Quantum Matter
this problem or where I
should look to solve it?
Many thanks,
David Tompsett.
Peter Blaha wrote:
Please check case.output2
D.A. Tompsett schrieb:
Dear All,
I am trying to run a supercell calculation of transition metals in a
Laves AB2 type phase. The supercell contains 96 atoms
EIGENVALUES BELOW THE ENERGY -9.0
Please advise me as to how to proceed.
Thank you,
David.
Peter Blaha wrote:
You are doing k-parallel calc !
What says lse ?
Check the individual case.output2_xx files !
David
Dear All,
I am having a problem while attempting an scf calculation of Ag5Pb2O6.
In setting up the calculation the default RMT's mean that there is core
charge leakage from the large Pb atom if one uses the default separation
energy of 6.0Ry.
I have tried to get around this in two ways:
1) Set
Dear All,
I have changed the local rotation matrix for an atom in my system from
the default found by program SYMMETRY. I have determined what I think
the new L,M basis should be according to the prescription in reference
Kara and Kurki-Suonio 81.
In the UG it says Perform a run of LAPW1 and
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