What you are doing is identical to the 'virtual crystal approximation'
-- search the wien2k mailing list archive for this. Shortly said: do a
normal initialization first, and only afterwards change Z in case.struct
and case.in2 (not in case.inst). As far as I remember, this can be done
with 1
This is only because runafm is not guaranteed to be always correct (not
yet detected bugs etc.). To be safe, you should therefor continue
afterwards with a few iterations using runsp. If runafm was correct for
your case, nothing will change. If there was a bug (or if the material
wants to be
Which is the direction of the up- and down-spins with respect to the
crystallographic axes when a spin-polarized calculation is performed?
This is not defined as long as spin-orbit coupling is not included (to
avoid confusion, it would be better to speak about majority and minority
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Computational Materials Engineering (CME)
Center for Computational Engineering Science (CCES)
RWTH Aachen University
Mauerstrasse 5
DE-52064 Aachen
Germany
e-mail: stefaan.cottenier
The parameter NUME defines the maximal number of eigenvalues and, as
it is said in the User's Guide, has to be increased for unitcells
with large number of electrons. How are the number of eigenvalues
and the number of electrons related? Is it true that the two
quantities are
{1} - (26 Pmc21)
or
{2} - (11 P21/m).
The total FM energy of {1} is -152655.214439 Ry
and that of {2} is -152655.214842 Ry
The precision of both calculations was 0.01 Ry since all the figures
after the point are important for me.
That looks like a difference that is
of 3.14 mb on the Co atom.
So what do you think is wrong, here?
Thanks in advance
Bothina
___
Wien mailing list
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Computational
switch in1new N means that, after Nth iteration, the program will
update in1 file at every iteration. Hence when you do a run with
in1new N and want to continue it with other parameters, still using
in1new may affect your in1 file.
You're right, Hashemi, I had a misconception here. The
However, after using x supercell, upon reaching the 'x lapw2 -qtl'
section of the calculation I have persistently encountered the error
'segmentation fault'. Any advice as to solving this problem would be
greatly appreciated.
See http://www.ghfecher.de/Fecher_CompileIntel.pdf , in
, Jul 25, 2008 at 10:18 AM, Stefaan Cottenier
stefaan.cottenier at fys.kuleuven.be wrote:
Dear wien2k community,
I ran into a case that gave a QTL-B error in the first iteration.
Following the FAQ, I therefore set the default 0.30 linearization energy
to about 0.2 Ry below the :FER
Thanks Peter and Laurence. The suggestion on core states/Rmt value seem
to solve it. Here are the results of the tests both of you suggested:
I've two suspicions:
a) Some problem with the struct file. It could be identical positions of
one atom, wrong symmetry operations, wrong
Laurence Marks wrote:
Wow, to me this is a clear red flag -- you have 10 too many electrons.
All looks fine here too (data taken from the diverging run with LAPW):
:NEC01: NUCLEAR AND ELECTRONIC CHARGE 2063.0 2073.45604 0.99496
:NEC02: NUCLEAR AND ELECTRONIC CHARGE
Hello again,
I have been too optimistic, yesterday. The reported problem
(eigenvalues below...) did indeed disappear when I modified the
sphere radii and/or put deep semi-core states in the core, as reported
yesterday. But when I applied the same modification to a Cu atom at a
different
: *** [pairhess] Error 1
SRC_qtl/compile.msg:make: *** [qtl] Error 1
SRC_structeditor/SRC_ncmsymmetry/compile.msg:make: *** [ncmsymmetry] Error 1
--
Stefaan Cottenier
Computational Materials Engineering (CME)
Center for Computational Engineering Science (CCES)
RWTH Aachen University
Mauerstrasse
It does give out the EFG results. It's so fast because I am just
trying a very simple example, Indium. To calculate the EFG, can I
just run lapw2 alone or do I need run SCF first? Thank you for your
help.
Of course you have to do the scf cycle first. This is like asking: in
order
I got lots of remarks: 'LOOP WAS VECTORIZED', though.
That is not an error, just information. Look at the end of
siteconfig_lapw for which programs have errors, and then look into the
compile.msg file in the SRC_* directory of that program to see what the
error really is. Concentrate on
I wish to calculate cohesive energy of CsCl using FP-LAPW. Can you
please guide me about the file which consist it.
See http://www.wien2k.at/reg_user/faq/cohesive.html
Stefaan
Disclaimer: http://www.kuleuven.be/cwis/email_disclaimer.htm
As you run only dstart (and not x dstart -c -up/dn), you seem to have a
nonspinpolarized run. But you use runsp.
Stefaan
Udai Pratap Verma wrote:
Dear wien2k user's I am getting some error message during optimization
of lattice parameter.
My case spin polarised.
I have edit optimize.job
Dear wien2k community,
I encounter a warning in the output of symmetry, see below. At first
sight this has no harmful consequence, this case runs (mostly) fine. Do
I have to worry about this?
Thanks,
Stefaan
Original case.struct (one out of 10 inequivalent positions):
Peter Blaha wrote:
This is just an information.
It finds the highest symmetry element (S4) along x.
Then it takes the first 2, which is, however, also along x and thus
the program detects that these directions are not orthogonal. Thus the
program looks for another 2, finds it along y, and
Dear wien2k community,
I want to come back to this thread, as I did not yet succeed to identify
what is really going on.
To summarize the original problem: a crash in lapw2 for impurities in
Ge, with very large (actually **) QTL-B warnings and (sometimes)
Eigenvalues below warnings in
The Wien2k in the particular case of tungsten automatically generates next
case.inst file.
***
W
Xe 5
4, 3,3.0 N
4, 3,3.0 N
4,-4,4.0 N
4,-4,4.0 N
5, 2,2.0 N
5, 2,1.0 N
5,-3,1.0 N
5,-3,0.0 N
6,-1,1.0 N
6,-1,1.0 N
End of Input
End of
Thanks for the explanations, but the magnetic moment of tungsten in the
ground state
should be zero in the contrast with occupation of the d-orbital's in
case.inst.
What is the reason of that.
You're probably confusing spin moment (S) and total moment (J). For a
d-orbital with 4
I want to learn how to calculate 4f electron, I do it as FAQ showed:
Open core treatment of 4f(5f) electron?? but there is something error after
I modified the case.inc case.in1 case.in2:
first, it shows SELECT error, so I using small mixer parameter;
but it shows Fermi error now, and then
I am working on the magnetic properties of rare earth?iron
compounds. I have a question in structure optimization.
How to set the U and J parameters when using LDA+U method, since U
and J can?t be calculated by ab initio way? So I just set U=J=0. If
it is reasonable, then is it
I tried to calculate the EFGs in a Ba compound which has body centered
orthorombic space group but I am confused about the printout of the EFGs.
Can you tell me the relation between the printout V_{11}, V_{22} and V_{33}
and the EFGs of V_{aa}, V_{bb}, and V_{cc}, where a, b, c are the 3
Do what it asks you to do:
Check file compile.msg in the corresponding SRC_* directory for the
compilation log and more info on any compilation problem.
Look for instance in SRC_lapw1/compile.msg and read the detailed error
messages there.
Stefaan
Disclaimer:
I recently installed wien2k_09 on my PC having core 2 quad 2.83 GHz cpu. The
program is using only 25%cpu. Any suggestion to increase the usage of cpu.
Should I use parallel configuration to use all four cpu.
Obviously yes. Provide a .machines file with four identical entries, and
use the -p
___
Wien mailing list
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
NEW EMAIL
Stefaan Cottenier
Center for Molecular Modeling
Ghent University
Proeftuinstraat 86
BE-9000 Gent
Belgium
http://molmod.Ugent.be
email: Stefaan . Cottenier
I wanted to compute the TOTAL DOS for a non-spin-orbit spin-polarized
calculation (FM and AFM)
(...)
I expected case.dos1evup and case.dos1evdn plots to look exactly the same
but they do not.
??? For a ferromagnetic calculation, the up and dn DOS must be
different. Otherwise, how could you
I am working with antiferromagnetic calculus and I would like to know
how to modify case inst. Does anybody have an example?
See the FAQ: http://www.wien2k.at/reg_user/faq/afm.html
Stefaan
I performed spin-polarized calculations on NdTiO3 compound and as
excepted the fermi level lies at the 4f states (due to the strong
localisation).
(Probably a word is missing in your last sentence, which gives it the
opposite meaning? == de-localization) The reason why LDA puts the 4f
Regarding the two different values of Ef, I checked case.inorb and it
seems ok. U is applied only on the f states of Nd:
Yes, that file seems to be fine.
1 2 0 nmod, natorb, ipr
PRATT 1.0BROYD/PRATT, mixing
1 1 3
://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 Zwijnaarde
Belgium
http://molmod.Ugent.be
email: Stefaan . Cottenier /at/ UGent . be
The following message appears even when I have taken 816 k-points
However the same value of the total energy comes that is -56165.959
QTL-B VALUE .EQ.2.21775 in Band of energy1.39668 ATOM=1 L=
3
Most likely no ghostbands, but adjust Energy-parameters or use -in1ef /
I do have f-states in my case.
I want to know if it is advisable to take these f-states in the valence and
do the calculation.
Would it be more accurate?
Moreover, during lstart, we give -6.0 Ry as the separation energy between
core and valence.
If we put -4.5 Ry, then does it mean
When constructing a case.struct file using w2web, the lattice constants
entered using the unit of Angstrom will be converted Bohr in the saved
file, but the label above the lattice constant in case.struct file is
kept as unit=ang. Is this intentional?
Yes, it is. This label is only meant
://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
___
Wien mailing list
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark
Since it is one of the limitations of Wien2k, I would like to know if
negative atomic positions are permissible in Wien2k.
No. But that is no problem, just take the complement (-0.38 == +0.62)
Stefaan
However, for calling the supercell program, a valid struct file has to
be present.
This struct file is the one for the completely ordered UZr2 structure --
hence you do have this file. The rest will be clear from the
self-explanatory questions which the supercell program will ask you
(have
However, w2web converts negative coordinates automatically to positive
ones.
I didn't know that (spending 99% of the time at the command line). Smart
w2web!
Stefaan
Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 Zwijnaarde
Belgium
http://molmod.Ugent.be
email: Stefaan . Cottenier /at/ UGent . be
The descriptions for esepermin and eseper0 in case.in2 file in userguid
and in DFT and family ... sec 6.1.4 are different, which one is correct?
Indeed, the names were incorrectly switched. Whenever such a situation
arises: it is the usersguide which is correct.
When I want to do a spin
There are not many mails (in the mailing list) on the construction of
supercell in Wien2k. Probably, it is so user-friendly I guess. However,
for a beginner like me, I would like to get a step by step introduction
to construction of supercell and its implementation in Wien2k. I could
not
In which case the energy parameter is different for d and f orbitals?
In those cases where you do have valence f-electrons, or when the
f-states are only slightly above E_fermi.
If they are kept same and that is what I usually do,
Don't make such decisions yourself, unless you have a good
I hope you remember that you gave the suggestion of changing the energy
parameter from 0.90 to 1.3. (my earlier mail on some errors)
No, I don't remember that ;-)
After you suggested that, I have kept the energy parameter for d and f
orbitals as 1.30 (1.20 also is quite a good value, the
I am new user . I am trying to find the energy of Zr(hcp) metal when
lattice parameter are too long more than 10A but for such big lattice
constant scf cycle is not running and showed an error message in
lapw0. Is it installation problem while it is running for real lattice
parameter.
For
I am running wien version wien2k 08_03
(consider upgrading -- this version is almost 2 years old, and you miss
quite some features and fixes)
I have been trying to simulate hcp Tb for weeks, no matter whatever
I did (including change the parameters and use different method such as
The reason I use *kpoints = 1000* is because I refered to S.
Cottenier's book ---Density Functional Theory and the Family of
(L)APW-methods: a step-by-step introduction, it uses kpoints = 912 for
hcp-Cd
That is in the irreducible part of the Brillouin zone (= number of
lines in
Comments are pasted at the relevant places:
After a regular GGA+SO scf, commamd line: *runsp -ec 0.0001 -cc
0.0001 -so -i 1000*
then i got some results as follows:
:ENE:-46876.608343 Ry
:MMTOT: 11.92563 uB
:MMI001: 5.81891 uB
I think there was a misunderstanding about my first question:
case.scfdmup
*
Spin-polarized + s-o calculation, M|| 0.000 0.000 1.000
Calculation of X, X=c*Xr(r)*Xls(l,s)
Xr(r)= I
Xls(l,s) = L(dzeta)
Before my new problems, I didn't agree with one of your point in
last email about the free Tb atom, you said:
free Tb atom f^9s^2 ,the free atom has (7-2)+(+3+2)=10 mu_B for
f-electrons only, and an extra 1 mu_B by the d-electron (ferromagnetic
intra-atomic 5d-4f coupling)
at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 ZWIJNAARDE
Belgium
http://molmod.Ugent.be
email: Stefaan.Cottenier /at/ UGent.be
We consider that the stable ground state of a metal is bcc. The fcc
structure is the high temperature phase. To calculate the enthalpy of
transformation of the fcc to bcc, we consider the following
Enthalpy of transformation =ENE(fcc)-ENE(bcc)
Now for this above equation, do we have to
Is there any way out to simultaneously optimize the lattice parameters and
the internal coordinates in w2web?
You might read the structure optimization notes at
http://www.wien2k.at/reg_user/textbooks/ (in particular Sec. 5)
Stefaan
1. I want optimized positions in case of experimentally known crystal
structures. Does it really help? Is it worth doing? I may be wrong or may be
doing what is not required.
2. I want to do only internal coordinates optimization for metastable
phases. Is it incomplete?
It all depends
Addendum: you can take the intermediate output, put them into a
spreadsheet such as Excel and plot the dos yourself with some
broadening -- it works but is not so convenient.
Two comments on this:
1) you can specify a broadening in case.int (see Sec. 8.1.3 of the UG)
2) there is a very
Do this thought experiment: take a structure with, say, 5 different
inequivalent positions for the same element, and then do something
unphysical: replace on one of the positions only the element by the next
element in the periodic table. Would that really matter? Well...
Or do the following
/.
___
Wien mailing list
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 Zwijnaarde
Belgium
http://molmod.Ugent.be
email: Stefaan
___
Wien mailing list
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark
But then how to tackle with the point you raised
(point no.2)
One thing would be to vary c/a with constant volume (option 2), but then I
do not have a priori information on the optimized parameters.
So what? The total energy tells you in which direction you have to
change the volume
Read your error message before asking:
forrtl: severe (64): input conversion error, unit 20, file
/group5/cg/sghosh/WIEN2k/lapw/U-Zr2_DELTA/U-Zr2_DELTA.struct
You probably made a typo in that file (one space too much, or a decimal
point at the wrong place,...)
Stefaan
I have a paramagnetic unit cell with a Re with an electron spin of 1
and three other non-paramagnetic ions. I have built a supercell and
have run these calculations a few times using various number of kpoints,
magnetic calculations with antiferromagnetic calculations, etc. However,
I
Then it asked if we have to choose a new struct file, I chose no.
Choose yes. nn 'knows' this better than you. Although this step is
somewhat redundant, sgroup will make the better choice, irrespective of
having accepted this change or not.
When I clicked on view outputsgroup
The
I have two queries
1. Initially I took 2x2x2 cell.
2. Does it make sense to choose a 3x3x3 cell for the same? To see if ENE
changes. I had taken 2 points in xkgen.
How can we know? It all depends on what you want to do, and on what you
have tested in terms of convergence/accuracy
was run and it did not give any errors. (Removed # from x
dstart only)
When I chose energy vs volume in plot; it gave a linear variation and not
like what is given in the UG guide for TiC.
Can you please tell me if I have done any mistake?
Suddhasattwa Ghosh
--
Stefaan Cottenier
I am trying to run SCF in NaCl phase. Following error in dstart is reported
'DSTART' - can't open unit:
15
'DSTART' -filename:
cdo.in2c
'DSTART' - status: old form:
://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 Zwijnaarde
Belgium
http://molmod.Ugent.be
email: Stefaan . Cottenier /at/ UGent . be
?id=60969
___
Wien mailing list
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular
at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 Zwijnaarde
Belgium
http://molmod.Ugent.be
email: Stefaan . Cottenier /at/ UGent . be
I have a basic question regarding DFT. Say
for some system we calculate antiferromagnetic, ferromagnetic and non
spin polarized state and by comparing energy we find that the
antiferromagnetic state is the ground state. Now as ferromagnetic and
non spin
But is your reply indicating that...
the excited states *may be* those states having higher energybut it
is *not sure* that whether the states having higher energy will be the
excited states of the system??..Please assure me that this is the
meaning of your reply...
help would be of great use.
Suddhasattwa Ghosh
___
Wien mailing list
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
But I guess, I did not address my question properly.
My SCF gave an error when I added a LO for L=2.
Even with this, it works here.
Once you have added this LO, you should drop -in1new (it would overwrite
case.in1 without re-adding the LO).
Stefaan
20.547 0.000 CONT 1
21.20020.001 CONT 1
With such lines in case.in1 you MUST get ghostbands.
But not with
20.547 0.000 CONT 1
21.20020.000 CONT 1
, right? (this helps a lot in order to get a smooth energy-vs-volume
curve for bcc-Fe, which is rather
(1) I read the step by step DFT theory written by S. Cottenier,
and it said EFG is a very sensitive quantity, and *if this one converge,
other quantities will usually converge,too.* My question is: *Is this
usually true during the convergence check of RKM or kmesh, espeically
for
Probably the magnetism got lost during your vasp calculation. Is it
possible to do fixed-spin-moment calculations in vasp? If so, do the
vasp calculation with a fixed moment of 2.5 mu_B, and use the result of
the latter calculation as starting point of a regular vasp scf-cycle.
Another way to
When the RMT is set to be smaller and keep the value of RMT*KMAX the
same, there will be more plane waves in Wien. On the other hand, VASP is
package using a plan wave basis, so I think the results of the two
package will be almost the same when the RMT set to be smaller.
Good attempt,
In sec. 4.5.8 at the top of page 50, it reads:
cp case.in0 case.in0_grr and change indxc to 50
It is not clear from this sentence whether the change has to be made in
case.in0 or case.in0_grr (in the latter, it turns out, as the
alternative leads to an immediate crash, for luck).
A more
My question is regarding the spin structure for a SDW calculation. As
far my knowledge, the unit cell need to be extended in a particular
direction, equivalent or greater than the wave vector, i.e. in case
of Cr, the unit cell length has to be 50 A, which is the magnitude of
the wave vector.
Now, that is taken care of, I still have another puzzling situation. I
want to make a 2*2*2 super cell of Silicon.
If I repeat the steps
Type F Then specify Si atoms using fractional coordinates (should be
16 atoms in total, I used material studio to visualize it is correct and
transfer
Wien at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 Zwijnaarde
Belgium
http://molmod.Ugent.be
email: Stefaan . Cottenier /at/ UGent . be
I have run BeO lattice case (space group P63mc) using WIEN2K code and
found that the Be 1s state energy is = -6.204169219 Ry and the electron
density at Be nucleus (RTO001) due to 1s core state is = 34.428627.
(just to fill out a small detail: the fact that you are able in this
case to
to you for sparing your valuable time for me.
looking forward to your answer very eagerly.
With kind Regards and thanks
--
SANJAY KUMAR SINGH
RESEARCH SCHOLAR
CONDENSED MATTER THEORY GROUP
SCHOOL OF STUDIES IN PHYSICS
JIWAJI UNIVERSITY
GWALIOR -474011 (M.P) INDIA
--
Stefaan
at zeus.theochem.tuwien.ac.at
http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 Zwijnaarde
Belgium
http://molmod.Ugent.be
email: Stefaan . Cottenier /at/ UGent . be
I woluld like to know how to calculate the enthalpy of formation for
Fe2Ti???
See for instance http://dx.doi.org/10.1103/PhysRevB.73.144104 (Eq. 1)
Stefaan
Thank you for the mail. In fact, I had used the option after I saved the
structure file. I had initialized SCF before I did geometry
optimization. If there was a problem in the overlapping spheres, x nn
would have given an error during SCF. It did not, and SCF converged in
21 cycles. SCF
://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
--
Stefaan Cottenier
Center for Molecular Modeling (CMM)
Ghent University
Technologiepark 903 (2nd floor)
BE-9052 Zwijnaarde
Belgium
http://molmod.Ugent.be
email: Stefaan . Cottenier /at/ UGent . be
The purpose of my calculations is to get isotropic and anisotropic
hyperfine parameters for my system using WIE2K code. I use this
command runsp_lapw -p -ec 0.0001 -cc 0.0001 -NI on
supercomputer in out institute. When i check the case.scf output
file , i can just find Fermi contact
As you mention 'x lapw1' and 'x lapwso' (and not 'run_lapw -so'): is
your goal to make a k-mesh test by inspecting convergence of the
non-selfconsistent eigenvalues of the first scf-iteration as a function
of k-mesh density? (this is indeed a reasonable alternative for a k-mesh
test using
Could there be any known
(but obscure) reason why lapw1para would not be able to write to its files,
but lapw0para would?
With k-point parallelization, lapw0 runs serially on the machine where
you have started the job. It does not need ssh. Only lapw1 and lapw2
are run parallelly.
In
My aim is to calculated case of MnF2 which has antiferromagnetic
configuration. I have defined struct file using Cmmm space group to
distinguish Mn atoms and set initial configuration in case.inst file (I
have flipped spins for one Mn to get antiferromagnetism) but my results
strongly
As I understand the orbital occupation numbers are obtained from the
integrated DOS (up to Fermi level) in the file case.outputt.
I have the following questions, please:
1. Is there any other file that contain information about the orbital
occupation numbers?
grep :QTL case.scf (and look to
Both variants will work. Variant b) can save you a little bit of time,
but is in a few situations not necessarily stable (that depends on the
state of the program at the moment of the crash).
Anyway, in your case, with a crash in lap0, it will not matter at all:
the execution time of lapw0 is
forrtl :severe(64) : input conversion error , unit 5, file
./root/./test_so.inso
'input conversion error' : probably a typo in case.inso ?
Stefaan
Verify whether your muffin tin spheres have not become almost touching
(x nn, watch the screen output, or look in case.outputnn).
If that does not help, please send us
grep :FOR case.scf_mini
grep :POS case.scf_mini
Stefaan
However the other problem is not yet resolved. In STRUCTGEN of TiC I
give the values of lattice parameters a=b=c=4.328A, which after 2-3
steps on w2web automatically show
Mode of calc=RELA, unit=ang
8.178738 8.178738 8.178738 90.00 90.00 90.00
I am not able to resolve this
This error message is perhaps a bit misleading. Note that the actual
message is about R0, not about RMT:
WARNING: R0 for atom 1 Z= 31.00 too big
Stefaan
after a first SCF cycle I inspected the .scf file and found the warning:
---
QTL-B VALUE .EQ. 2.54381 in Band of energy -0.94774 ATOM= 2 L= 0
Most likely no ghostbands, but adjust Energy-parameters or use -in1ef /
-in1new
WARNING: R0 for atom -4 Z= 83.00 too big
With that I reduced the muffin tin radius for that atom but
eventually I got the
A similar confusion appeared in this list a couple of weeks ago: the
warning is about R0 (=the first radial grid point), so why do you
change de muffin tin radius
1 - 100 of 295 matches
Mail list logo