Re: [Wien] band gap for structure with a defect

2023-09-13 Thread Natalia Andreeva
Thanks a lot

On Wed, Sep 13, 2023 at 8:56 PM Peter Blaha 
wrote:

> In addition to what Igor said:
>
> If you want a reasonable gap for the bulk, you can use   mBJ+U (with a
> small U of a few eV).
>
> Still, for your cell, you won't get an insulator (also doped Si is
> "metallic" and conducting, otherwise a computer would not work ...).
>
> PS: Draw the DOS and compare with the undoped DOS. Maybe you understand
> then better.
>
>
> Am 13.09.2023 um 19:19 schrieb Natalia Andreeva:
> > Dear WIEN2k users,
> >
> > I am calculating the band gap of bulk BaTiO3 using the LDA+U with PBE
> > functional. For the values below, the band gap was 2.002 eV (which I
> > can explain by the choice of the PBE functional). When I moved to a
> > supercell with a defect (oxygen vacancy, supercell dimensions 2x2x1),
> > the band gap became 0.0 eV.
> > I tried to increase the Hubbard parameter U. For example, for bulk
> > calculations with U=1.121 Ry = 15.252 eV, the band gap was 3.391 eV.
> > However, running with the same parameters for a supercell with a
> > defect gave a calculated value of 0.889 eV.
> > I have the following questions:
> > 1. Why does the band gap decrease so much when going from bulk to
> > supercell with a defect?
> > 2. Is it worth changing the PBE functional to another one if the band
> > gap for bulk is less than the experimental one?
> > 3. If I continue the calculations on PBE+U, how can I improve the values?
> >
> > With Best Regards,
> > Natalia
> >
> >
> > ___
> > Wien mailing list
> > Wien@zeus.theochem.tuwien.ac.at
> > http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
> > SEARCH the MAILING-LIST at:
> http://www.mail-archive.com/wien@zeus.theochem.tuwien.ac.at/index.html
>
> --
> ---
> Peter Blaha,  Inst. f. Materials Chemistry, TU Vienna, A-1060 Vienna
> Phone: +43-158801165300
> Email: peter.bl...@tuwien.ac.at
> WWW:   http://www.imc.tuwien.ac.at  WIEN2k: http://www.wien2k.at
> -
>
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>


-- 
Best Regards,
Natalia Andreeva.
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Re: [Wien] band gap for structure with a defect

2023-09-13 Thread Natalia Andreeva
Thank you very much

On Wed, Sep 13, 2023 at 8:32 PM Igor I Mazin  wrote:

> 1. Undoped BaTiO3 is an insulator. An oxygen vacancy introduces electron
> doping. When you dope an insulator, you get a metal. In a metal, the gap
> is zero.
> 2. U=15 eV is an insanely large and unphysical value. You are better off
> with no U at all. For small doping (small concentration of vacancies)
> Hubbard correlations are irrelevant.
> 3. 2x2x1 with one vacancy is doping of 0.5 e per formula unit. This is
> unphysically large (like, by three orders of magnitude) and I would not
> trust a single number from this simulation. Check
>
> https://journals.aps.org/prresearch/abstract/10.1103/PhysRevResearch.5.033080
>
> On 9/13/2023 13:19, Natalia Andreeva wrote:
> > Dear WIEN2k users,
> >
> > I am calculating the band gap of bulk BaTiO3 using the LDA+U with PBE
> > functional. For the values below, the band gap was 2.002 eV (which I can
> > explain by the choice of the PBE functional). When I moved to a
> > supercell with a defect (oxygen vacancy, supercell dimensions 2x2x1),
> > the band gap became 0.0 eV.
> > I tried to increase the Hubbard parameter U. For example, for bulk
> > calculations with U=1.121 Ry = 15.252 eV, the band gap was 3.391 eV.
> > However, running with the same parameters for a supercell with a defect
> > gave a calculated value of 0.889 eV.
> > I have the following questions:
> > 1. Why does the band gap decrease so much when going from bulk to
> > supercell with a defect?
> > 2. Is it worth changing the PBE functional to another one if the band
> > gap for bulk is less than the experimental one?
> > 3. If I continue the calculations on PBE+U, how can I improve the values?
> >
> > With Best Regards,
> > Natalia
> >
> >
> > ___
> > Wien mailing list
> > Wien@zeus.theochem.tuwien.ac.at
> > http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
> > SEARCH the MAILING-LIST at:
> http://www.mail-archive.com/wien@zeus.theochem.tuwien.ac.at/index.html
>
> --
> Igor Mazin, Prof. of Advanced Studies
> Quantum Science and Engineering Center
> Department of Physics and Astronomy
> George Mason University
> phone 1-703-503-8152 (h)
> http://mason.gmu.edu/~imazin2
> ___
> Wien mailing list
> Wien@zeus.theochem.tuwien.ac.at
> http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
> SEARCH the MAILING-LIST at:
> http://www.mail-archive.com/wien@zeus.theochem.tuwien.ac.at/index.html
>


-- 
Best Regards,
Natalia Andreeva.
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Re: [Wien] band gap for structure with a defect

2023-09-13 Thread Peter Blaha

In addition to what Igor said:

If you want a reasonable gap for the bulk, you can use   mBJ+U (with a 
small U of a few eV).


Still, for your cell, you won't get an insulator (also doped Si is 
"metallic" and conducting, otherwise a computer would not work ...).


PS: Draw the DOS and compare with the undoped DOS. Maybe you understand 
then better.



Am 13.09.2023 um 19:19 schrieb Natalia Andreeva:

Dear WIEN2k users,

I am calculating the band gap of bulk BaTiO3 using the LDA+U with PBE 
functional. For the values below, the band gap was 2.002 eV (which I 
can explain by the choice of the PBE functional). When I moved to a 
supercell with a defect (oxygen vacancy, supercell dimensions 2x2x1), 
the band gap became 0.0 eV.
I tried to increase the Hubbard parameter U. For example, for bulk 
calculations with U=1.121 Ry = 15.252 eV, the band gap was 3.391 eV. 
However, running with the same parameters for a supercell with a 
defect gave a calculated value of 0.889 eV.

I have the following questions:
1. Why does the band gap decrease so much when going from bulk to 
supercell with a defect?
2. Is it worth changing the PBE functional to another one if the band 
gap for bulk is less than the experimental one?

3. If I continue the calculations on PBE+U, how can I improve the values?

With Best Regards,
Natalia


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--
---
Peter Blaha,  Inst. f. Materials Chemistry, TU Vienna, A-1060 Vienna
Phone: +43-158801165300
Email: peter.bl...@tuwien.ac.at
WWW:   http://www.imc.tuwien.ac.at  WIEN2k: http://www.wien2k.at
-

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Re: [Wien] band gap for structure with a defect

2023-09-13 Thread Igor I Mazin
1. Undoped BaTiO3 is an insulator. An oxygen vacancy introduces electron 
doping. When you dope an insulator, you get a metal. In a metal, the gap 
is zero.
2. U=15 eV is an insanely large and unphysical value. You are better off 
with no U at all. For small doping (small concentration of vacancies) 
Hubbard correlations are irrelevant.
3. 2x2x1 with one vacancy is doping of 0.5 e per formula unit. This is 
unphysically large (like, by three orders of magnitude) and I would not 
trust a single number from this simulation. Check 
https://journals.aps.org/prresearch/abstract/10.1103/PhysRevResearch.5.033080

On 9/13/2023 13:19, Natalia Andreeva wrote:
> Dear WIEN2k users,
> 
> I am calculating the band gap of bulk BaTiO3 using the LDA+U with PBE 
> functional. For the values below, the band gap was 2.002 eV (which I can 
> explain by the choice of the PBE functional). When I moved to a 
> supercell with a defect (oxygen vacancy, supercell dimensions 2x2x1), 
> the band gap became 0.0 eV.
> I tried to increase the Hubbard parameter U. For example, for bulk 
> calculations with U=1.121 Ry = 15.252 eV, the band gap was 3.391 eV. 
> However, running with the same parameters for a supercell with a defect 
> gave a calculated value of 0.889 eV.
> I have the following questions:
> 1. Why does the band gap decrease so much when going from bulk to 
> supercell with a defect?
> 2. Is it worth changing the PBE functional to another one if the band 
> gap for bulk is less than the experimental one?
> 3. If I continue the calculations on PBE+U, how can I improve the values?
> 
> With Best Regards,
> Natalia
> 
> 
> ___
> Wien mailing list
> Wien@zeus.theochem.tuwien.ac.at
> http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
> SEARCH the MAILING-LIST at:  
> http://www.mail-archive.com/wien@zeus.theochem.tuwien.ac.at/index.html

-- 
Igor Mazin, Prof. of Advanced Studies
Quantum Science and Engineering Center
Department of Physics and Astronomy
George Mason University
phone 1-703-503-8152 (h)
http://mason.gmu.edu/~imazin2
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