ows:
>
> I have extracted the energy values corresping to the maximum values of DOS
> in the up and down spin from the files case.dos1evup and case.dos1evdn and
> I have found the following values:
>
> E (max DOS up = 2.40) = - 0.95185 eV
> E (maxDOS dn = 2.80) = + 1.95977 eV
Hello again
I still waiting for a practical way to determine the exchange splitting or
the example of iron Fe and which files are necessary to do that
Bet regards
On Fri, 24 Apr 2020 at 16:42, Abderrahmane Reggad
wrote:
> Hello again
> I have adopted another procedure as follows:
>
= 2.80) = + 1.95977 eV
and I have calculated the exchange splitting from this formula dE= +
1.95977 - ( - 0.95185) = 2.91162 eV
Is correct ?
On Fri, 24 Apr 2020 at 14:54, Abderrahmane Reggad
wrote:
> Thanks Gerhard for the explanation but I couldn't apply the inforation to
> get t
14:52, Abderrahmane Reggad
wrote:
> Thanks Gerhard for the explanation but I couldn't apply the inforation to
> get the exchange splitting neither from the DOS nor from the band structure
>
> Now i have some questions about my idea using the DOS picture and I want
> from both of you
OS in energy until they overlap as much as
> possible. This shift is your exchange splitting.
>
> Am 24.04.2020 um 00:07 schrieb Abderrahmane Reggad:
> > Hello wien2k users
> >
> > I have calculated the DOS of the paramagnetic and ferromagnetic of 3d
> > transiti
Hello wien2k users
I have calculated the DOS of the paramagnetic and ferromagnetic of 3d
transition metals Ni , Fe and I want to determine the exchange splitting
between the paramagnetic and ferromagnetic states.
How to do that ?
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics
ith any xy plotting tool (Excel).
>
>
>
>
> Am 22.04.2020 um 17:14 schrieb Abderrahmane Reggad:
> > Hello wien users
> >
> > Is it possible to get the integrated DOS from the DOS calculation in
> > wien2k code which allows us to get from the spin polarized D
edI/AGM/v6LM18YIAIUQ2CKxzuiw910yQF5gTLp-wCNcBGAsYHQ/s1600/integrated%2BDOS%2Bof%2Biron.png>
--
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Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - A
.1103/PhysRevB.74.155108
>
> https://journals.aps.org/prb/abstract/10.1103/PhysRevB.80.235109
>
> https://journals.aps.org/prb/abstract/10.1103/PhysRevB.83.235118
>
>
> ------
> *From:* Wien on behalf of
> Abderrahmane Reggad
> *Sent:* Friday, April
tates, in the whole unitcell)
> Hybrid-DFT with alpha according your input and DFT-correlation according
> your choice (case.in0).
>
> Am 10.04.2020 um 16:14 schrieb Abderrahmane Reggad:
> > EECE is onsite hybrid or not ?
> >
> > Your meaning for hybrid (HYBR ) is to
EECE is onsite hybrid or not ?
Your meaning for hybrid (HYBR ) is to be applied inside LAPW spheres and is
different from I know
What about these 2 equations
Exc (EECE) =EDFTxc+α(EHFx−EDFTxc)
Exc (HYBR) =EDFTxc+α(EHFx−EDFTx)
On Fri, 10 Apr 2020 at 16:04, Abderrahmane Reggad
wrote:
> E
s for hybridization between
> the Hartree-Fock and DFT exchanges. I don't think that hybrid has been
> used for hybridization between exchange and correlation. At least not in
> the WIEN2k user's guide.
>
> FT
>
>
> ------
> *From:* Wie
. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
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order II has lattice parameters a = b = 2,96 A ,
14,53 A
I want to know which AFM order do you use
best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
e" is really not appropriate for this list in my
> opinion.
>
> On Sat, Feb 8, 2020 at 12:09 PM Abderrahmane Reggad
> wrote:
>
>> Hello wien users
>>
>> In a previous message Dr delamora have given me the procedure to create
>> the magnetic structure
110 plane (afm III) for
compounds like NiO in the NaCl structure.
I need the procedure to it
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
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Thanks Pr Blaha for the answer
Best regrds
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Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
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alculation"
Reference: https://www2.fkf.mpg.de/andersen/LMTODOC/node170.html
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)5618
Thanks Dr Gavin for the rich information and I will try to choose the
easiest way to do it.
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
://wien2k-algerien1970.blogspot.com/2016/09/the-full-version-of-conversgence-tests.html
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
Hello wien2k users
Is it possible to do parallel calculation with the FSM procedure ?
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
obtaining
good starting spin densities to be used in standard spin-polarized
calculations" and this is in agreement to what Pr Plaha said.
Second I have thank Pr Laurence for the alternative solution to the
convergence problem which exist in spin polarized calculations.
Best regards
--
Dr.
.
My question is how to do that ?
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
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Thanks Pr Blaha for the script and I will try it
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
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Thanks xavier for the interesting article and useful information
My new question is : what's the relationship between the unpaired electrons
and the orbital contribution. I think that the unpaired electrons are
always related to the spin contribution.
Best regards
--
Dr. Abderrahmane R
Since the ground state of the Au metal is non magnetic, does it mean that
the Au metal is diamagnetic or paramagnetic and why ?
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
Thanks Pr Blaha for your answer and now I have another question
Is there a possibility to do one calculation for many values of M using FSM
procedure as in case of the volume optimization ?
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn
Hello wien users
To study the magnetic phase transitions and the different magnetic phases
we use the FSM procedure.
My question is to which equation do we fit the results E(M) obtained by
this procedure and how to plot the energy surface in the M-V space?
Best regards
--
Dr. Abderrahmane
Thanks for the answers
The electronic structure of the Au is [Xe]4f145d106s1 and that of Au+ is [
Xe]4f145d10 . Does the fullness of the d orbitals which make the magnetic
moment of Au metal zero ? and what about the s electron in the 6 shell?
--
Dr. Abderrahmane Reggad
Engineering Physics
solution for a Fcc Au metal?
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
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http
ation converges
to a zero moment solution
which should be identical to the non spin polarized one.
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Al
Thanks Gerhard for the information
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
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to a zero moment solution
which should be identical to the non spin polarized one.
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Al
find the magnetic ground state?
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences, Ibn Khaldoun University, Tiaret, 14000,
Algeria
Tel: +213(0)561861963 - Algeria
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We know that at ambiant conditions the Bcc Fe is more stable that Fee Fe.
but our calculations are made at 0 K and 0 P.
Is the shift in atmospheric conditions correct to get the same results?
Best regards
--
Dr. Abderrahmane Reggad
Engineering Physics Laboratory
Faculty of Material Sciences
But Laurence , they are many definitions and classification in magnetic
language and I want to know which language is adopted in wien2k comuunity
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Thanks Delamora for your clarification
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Hello Wien2k users
Does the magnetic classification in the Wien2k community is done according
the atomic magnetic moment or the total magnetic moment?
>From the following magnetic states which one is magnetic and which one is
non magnetic?
Diamagnetic
Paramagnetic
Ferromagnetic
Antiferromagnetic
Hello again
here is the link for the package
https://wien2k-algerien1970.blogspot.com/2016/09/the-full-version-of-conversgence-tests.html
Good luck
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Try to follow the steps of 3 differents packages to calculate the elastic
properties in the following link and compare with the results in the blog.
https://wien2k-algerien1970.blogspot.com/2016/09/summarization-of-calculation-of-elastic.html
Good Luck
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Hello again
I have repeated the calculation using the low symmetry structure and i
found a close results to those of the monoclinic one.
I have checked the wyckoof positions and the symmetry operations of the
orthorhombic and the monoclinic structures and I have found that the later
is a subgrou
Thank you Lyudmila for you comment
As a last step I need from all of you to show me how to get the AFMIII
structure from the these two links and the following non magnetic structure
of NiS-MnP (orthorhombic):
https://ibb.co/nt2nFm
https://ibb.co/mqySFm
NiS-MnP
P LATTICE,NONEQUIV.ATOMS: 2
Thank you gavin for your answer
So my structure is ok
Best regards
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Dear Delamora
I still waiting for my answer
Best regards
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Thank you very Delamora
Now I still waiting for your answer on my question in this link about the
magnetic structure of the zinc blende structure
Re: [Wien] The magnetic structure for zinc blende non magnetic structure
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Sorry for the missed word "correct"
According to your example , you mean that the AFM structure may be correct
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Sorry for the missed word "correct"
According to your example , you mean that the AFM structure may be correct
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Thanks Delamora for your answer and this is not what i am looking for and I
am sorry that I couldn't communicate what I want.
My problem is as follows:
1- I am considering this non magnetic structure (orthorhombic )
* the non-magnetic structure is in this link
https://ibb.co/nt2nFm
* The struc
I see that you haven''t understood me this time
my question is as follows:
is it possible to get a monoclinic structure with orthorhombic lattice
parameters ?
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Hello again
Here is the 3 different AFM configurations
https://ibb.co/mqySFm
Here are the 4 independent Ni atoms
https://ibb.co/nt2nFm
Now the big problem lies in if is it possible tp get a monoclinic structure
(space group #11) with orthorhombic lattice parameters as we know that the
rhomb
Thank you pieper for your answer
I am studying the magnetic order of type III with Ni1,Ni2 up and Ni3, Ni4
down according the figure included.
This is the procedure that I adopted:
-supercell 1x1x1 P to make the 4 atoms Ni indepedent a
- I make the Ni1 and Ni2 to be the atom Ni1 and the atoms
Dear wien users
I am studing the magnetic structure of type III for a orthorhombic
structure.
After doing the supercell and labelling the independent atoms for spin-up
and spin-dn atoms and using the sgroup command I got the following
structure:
The space group of a monoclinic structure and the
Sorry the link is
http://wien2k-algerien1970.blogspot.com/2016/06/structural-and-magnetic-properties-of.html
2017-10-13 8:11 GMT+02:00 Abderrahmane Reggad :
> Dear Delamora
>
> It's up to now that I start to work with the magnetic structure of the
> zinc blende one.
>
&
Dear Delamora
It's up to now that I start to work with the magnetic structure of the zinc
blende one.
- The zinc blende structure for NiS has not been studied before and I am
studing the possibility of its existence.
- In the literature, I found that the magnetic ground phase of the zinc
blende
Dear Delamora and wien users
In a previous post about the magnetic structure of the non magnetic NaCl
structure of NiO, Dr Delamora provided us in detail how to get this
magnetic structure (
https://www.mail-archive.com/wien%40zeus.theochem.tuwien.ac.at/msg11519.html
).
Now I need the magnetic st
Thank you Gerhard for your advise
I read and I understand
What do you think if using the empirical parameters known give you
calculated values for band gap and magnetic moment ten times or more than
the experimental one.
Before using my value for alpha parameter, I used the alpha value equal to
Hi Lyudmila
I have forgotten to add the article link
http://www.sciencedirect.com/science/article/pii/S0921452617303915
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Hi Martin
I still confused and not convinced with my results.
It's not the band gap of NiS to take as the only criterion for the choice
of the amount of excact exchange, but also the experimental values of
magnetic moment. This amount allows me to get magnetic moment values close
to the experimen
Hi Lyudmila
in the following article I studied the 3 different possible orderings for
the NiAs structure for the NiS compound and I found that the I-type order
is the most stable which is consistent which all theoritical and
experimental results.
It's found also that all transition metal compoun
Hi Laurence
The amount of 0.05 of exact exchange is the value that gives a gap value
equal to the experimental one for nickel sulphide and close values for
magnetic moments for some 3d transition metal sulphides like CrS, FeS, CoS
and NiS.
You can check my article about the nickel sulphide
http:
Hi all
I have repeated the calculation using ec and cc criterion equal to 0.1
and 0.0001 respectively and I have found the magnetic moment to be lesser
with the value of 0.0002 MB.
Here are the input files
VS.struct
***
VS-hex
H LATTICE,NONEQUIV.ATOMS: 3
164_P-3m1
MODE OF CALC=R
Hi
Before doing the calculation again with the new energy and charge criterion
I let you this old article http://journals.jps.jp/doi/abs/10.1143/JPSJ.14.196
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Hi
Before doing the calculation again with the new energy and charge criterion
I let you this old article http://journals.jps.jp/doi/abs/10.1143/JPSJ.14.196
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Hi All
I have used the PBE+EECC calculation for 3 configurations: nm, fm and afm I
and I found that the afm I is the most stable.
The energy criterion and charge are 0.001 Ry and 0.001 e respectively.
I don't worry about if the material is really antiferromagnetic or
paramagnetic because of:
1-
Hi Gerhard
1- The charge criterion was 0.001 e
2- I didn't started from a converged PBE calculation
3- The amount of exact exchange use leads for results consistent with
experiment for the other 4 compounds.
5- Geometrical optimization leads to AFM 1 to be the most stable
6- i found only experimen
Hi Martin
The problem is that I want to know if it's possible to get a such value of
0.05 MB for atomic magnetic moment for the AFM state of vanadium sulphide
in NiAs structure.
Hafner and Hobbs have found all the calculations converged to the non
magnetic state because they have used the GGA met
I have made calculations for 5 3d transition metal sulphides with the
method PBE+EECE and I have found that all the results are ok with the
exception of the vanadium sulphide.
I have made 3 calculations (nm, fm and afmI ) to determine the magnetic
state for all the compounds and I found them to ha
Thanks martin
Experimentally they found that the vanadium sulphide is a pauli
paramagnetic but I have found it to be antiferromagnetic like other
transition metal sulphides but the magnetic moment value equals almost
zero despite the fact that vanadium has 3 inpaired electrons.
Best regards
_
Dear wien2k users
I have calculated the magnetic moment of vanadium sulphide in NiAs
structure using the EECE méthod with alpha parameter equals to 0.05.
despite the fact that the number of inpariated electrons is equal to 3 I
found that the magnetic moment of vanadium is equal to 0.05 MB which
thank you Martin Gerhard Peter and Laurence for the answers
I think the conclusion is as follows:
The high or the low spin configuration of an ion is selected within the
initialization and the best choice is appared in the result as in the case
of Fe2+ ion.
For the bond valence sums alternative
Hello again
I have found in the literature that the spin state configuration is like
the magnetic configuration. So we have to make 2 calculations: one for the
high spin configuration and another one for the low spin configuration and
we look after for the configuration more energetically stable.
Thank you victor for your answer
The Fe+2 ion in the NiAs structure has an octahedral ccordination and has a
high spin configuration.
In wien2k code, where have we to look to check if , for example, the iron
ion has a high spin configuration.
Best regards
Dear wien2k users
We know that the ion Fe+2 has a high spin configuration (3d6 (teg(4) eg(2))
because the crystal field effect..
How to check that from calculation ?
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uania for the articles
Best regards
2017-08-24 1:23 GMT+01:00 Abderrahmane Reggad :
> Thank you for all for the rich discussion
>
> If I introduce the Ni atom and I change the Z number to 27 or 26 it still
> nickel because the atom is ont only Z and I change Z the number of neutr
changes.
An other question: We suppose that the ionic state of NiO is a result from
the electron density , can we force this ionic state to be Ni+3S-3 and it's
yes how?
Best regards
2017-08-24 0:43 GMT+01:00 Abderrahmane Reggad :
> Hello
>
> The reason for my question is that I do
Hello
The reason for my question is that I don't how does a DFT code work and I
want to know if the ionic state is a result or an assumption.
Thank you for contribution to clarify the picture.
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Dear wien users
I want to simulate the NiO compound in its ionic state. We know that the Ni
and O atoms have in their neutral state the atomic numbers 28 and 8
respectively.
Now, if we want to study the ionic state of the compound Ni+2O-2, should we
modify the atomic numbers to Z=26 for Ni and Z=
Dear wien2k users
I have done structural optimization for orthorhombic structure using
OrthoOpt packge of Tomas Kana but it works well.
How to fix the problem?
Best regards
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Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 AL ATTAF AIN DEFLA
Tel: +
Hello
To optimize the tetragonal structure as for the hexagonal structure you can
use the 2D-optimize package included in the wien2k code as in the following
link:
https://wien2k-algerien1970.blogspot.com/2016/09/optimization-of-hexagonal-and.html
Good luck
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Laboratoire de Génie
You have right Dr gavin
When I have opened the link in another web browser I could get the new
version of userguide.I get the same version after I have delete the cash
data.
Thanks
Best regards
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Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 AL
Thanks Dr gavin for all
I still get the old version , I don't know why
Best regards
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Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 AL ATTAF AIN DEFLA
Tel: +213(0)561861963
Algerie
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Thank you Dr for your detailed explanation as usual.
Now, It becomes clear to me
But the link of the userguide is for that of WIEN2k 14.2 version.
Best regards
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Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 AL ATTAF AIN DEFLA
Tel: +213(0)56186196
Dear wien developpers
The new version of wien2k is arrived but there is no sufficient information
on how to use the new library LIBXC implemented and how to combine the
different functionals for exchange and correlation to get a result close to
the experimental one.
Best regards
--
Mr: A.Reggad
Thanks again Dr Gavin
* I see that the procedure in w2web is different from that of terminal
* I couldn't understand why
use x lapw1 -band -dn -orb when up is selected
and
use x lapw1 -band -up -orb when dn is selected
* Do we make one plot for both spins or one plot for every spin?
Best r
Thanks again Dr Gavin for the explanation
Since the total potential Vt is calculated by the program lapw0, we can
find in the repertory SRC_lapw0 how the diiferent parts are implemented and
their formulas.
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Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse:
Thanks again Dr Gavin for the explanation
Since the total potential Vt is calculated by the program lapw0, we can
find in the repertory SRC_lapw0 how the diiferent parts are implemented and
their formulas.
On other side, I think the new library LIBXC contains all the formulas of
the didderent par
Thank you Dr Gavin for the detailed explanation
Can we adopt this procedure for band structure
x lapw1(c) -band -up -orb # eece potential is included by orb
x lapw1(c) -band -dn -orb
x spaghetti (-c) -up
x spaghetti (-c) -dn
Best regards
--
Mr: A.Reggad
Laboratoire de Génie Physique
Hello again
According to the notes of Elias Assmann (
http://susi.theochem.tuwien.ac.at/reg_user/textbooks/WIEN2k_lecture-notes_2013/ldau.pdf)
the program flow of the EECE method is as follows:
runsp -eece
- lapw0 lapw1 -orb -up,dn
-lapw2 -up,dn
- lcore -up,dn
-lapwdm -up,dn
- lapw2 -eece -up,
Thank you again Dr Gavin for the answer
Effectively what you have said
The adding of the flag "-eece" doesn't make error but it doesn't make change
Best regards
--
Mr: A.Reggad
Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 AL ATTAF AIN DEFLA
Tel: +213(0)5618619
Yes I have read this subject but I am looking the formulas of GGA(PBE)
functional
Dr gavin has given a reference for the formulas for the energy parts but i
am still waiting for the potential parts.
Thank you Dr Gerhard for the effort
Best regards
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Mr: A.Reggad
Laboratoire de Génie Physique
I am sorry I have made mistake
The main script x_lapw has a flag " -eece " and the script x lapw1 doesn't
I don't know what's the difference between them
And about the difference between the x lapw1 and x lapw1 -eece commands
lies in the fact that the first is for standard method (gga or lda )
Thanks Dr Gavin for your answer
- The the -eece flag exists for the script x lapw ( page 58 of the
usetguide (
http://susi.theochem.tuwien.ac.at/reg_user/textbooks/usersguide.pdf ) and I
tried it and it works well.
- Even for spaghetti I have executed the following command and it doesn't
give err
Thank you Dr Gavin for your ansswer
It's what I am looking for .
What about the formulas of the potentials Pc and Px?
Best regards
--
Mr: A.Reggad
Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 AL ATTAF AIN DEFLA
Tel: +213(0)561861963
Algerie
___
Hello again
I have found the procedure for DFT+U and I have deduct that for onsite
hybrid as follows and I want to know if it's correct:
- *Band Structure*
1. copy case.klist (case= hcp,fcc,bcc,sc)
2. copy case.insp and enter the value of Efermi in case.scf2
3. verify Emin Emax (-
Dear wien users
What's the procedure used to calculate the band structure and DOS using the
onsite hybrid method.
Best regards
--
Mr: A.Reggad
Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 AL ATTAF AIN DEFLA
Tel: +213(0)561861963
Algerie
Thank you Mr Boulet for you reply.
I have already done this search and I couldn't find the formulas
implemented in the wien2k code for the functional PBE.
Pc(pbe),Px(pbe),Ec(pbe) and Ec(pbe)?
Best regards
--
Mr: A.Reggad
Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: B
Dear wien developpers
I need the formulas of the correlation and exchange potentials and energies
(Pc, Px, Ec and Ex) for the functional PBE implemented in the wien2k code .
Best regards
--
Mr: A.Reggad
Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 AL ATTAF AIN
For a beginner, and to use the 2Doptimize package with the method PBE+U he
has to following procedure:
- create a session using the w2web interface and put in the working
repertory the
following files:
* case.struct with reduction factor equals to more than
10 percent to re
Thank you Prof Laurence for the information
I have been knowing how to do that before until finding a converse
statement in the guide of the 2Doptimize package that have confused me.
Thank you again
--
Mr: A.Reggad
Laboratoire de Génie Physique
Université Ibn Khaldoun - Tiaret
Adresse: BP 144 A
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