[QE-users] Incosistent energy contributions for 2D system
Paolo Giannozzi
paolo.giannozzi at uniud.it
Thu Jul 25 19:11:31 CEST 2024
The "Hartree", "one-electron", "Ewald" contributions to the energy have
something in common: the G=0 contribution to the energy separately
diverges. Their sum however does not diverge for neutral cells. So one
subtracts out the diverging terms and is left with a finite G=0
contribution. This may however vary a lot between different structures,
even if the sum of the three contributions is quite the same as in this
case.
Paolo
On 25/07/2024 18:43, Lenz Fiedler wrote:
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>
> Dear QE users,
>
> I have a question regarding a 2D QE calculation. Consider a very simple
> bilayer graphene system, which I calculate either with a "big" (23
> Angstrom in z-direction) or "small" (17 Angstrom in z-direction) cell
> (Input files are at the end of the message). The C atoms are in two
> planes in x-y-direction.
>
> Now both calculations are the same except for their z-dimension. In the
> "small" case I make the cell a bit smaller in z-direction. I did careful
> calculations to determine by how much I can make it smaller without the
> total energy deviating too much from the original cell. The input I
> share here is still well within the range where the total energy error
> is very small. Of course, eventually one hits a point where there is a
> noticeable energy difference.
>
> Now to my question: I have noticed that for both calculations, total
> energies are essentially the same, but what differs quite drastically,
> are the individual energy contributions. Namely I get:
>
> "big":
> ! total energy = -48.18986746 Ry
> estimated scf accuracy < 0.00003985 Ry
> smearing contrib. (-TS) = -0.00000000 Ry
> internal energy E=F+TS = -48.18986746 Ry
>
> The total energy is F=E-TS. E is the sum of the following terms:
> one-electron contribution = -1245.11933758 Ry
> hartree contribution = 624.03689026 Ry
> xc contribution = -17.17420972 Ry
> ewald contribution = 590.06678957 Ry
>
> "small":
> ! total energy = -48.18985199 Ry
> estimated scf accuracy < 0.00007424 Ry
> smearing contrib. (-TS) = -0.00000000 Ry
> internal energy E=F+TS = -48.18985199 Ry
>
> The total energy is F=E-TS. E is the sum of the following terms:
> one-electron contribution = -759.11502918 Ry
> hartree contribution = 381.02359494 Ry
> xc contribution = -17.17243795 Ry
> ewald contribution = 347.07402021 Ry
>
>
> As you can see, the total energies match up nicely, but all other terms
> except for the XC energy are different. Is this by design? Is there a
> numerical reason for it? I am trying to come up with a way to determine
> the minimal vacuum in z-direction I have to leave below and above my
> graphene planes, and had originally only checked the total energy. Now I
> am wondering if this is enough?
>
> Kind regards
> Lenz Fiedler
> PhD student (Helmholtz-Zentrum Dresden-Rossendorf)
>
> PS: I also disabled "assume_isolated = '2D'" - I still see the same
> behavior, albeit with different numbers for the energy contributions,
> the total energies are still the same.
>
> Input files:
>
> (PSP taken from http://www.pseudo-dojo.org/index.html):
>
>
>
> "big":
> &CONTROL
> calculation = 'scf'
> verbosity = 'high'
> restart_mode = 'from_scratch'
> outdir = 'temp'
> prefix = 'C'
> pseudo_dir = './'
> /
> &SYSTEM
> ibrav = 0
> nbnd = 10
> ecutwfc = 80
> ecutrho = 320
> nosym = .true.
> noinv = .true.
> occupations = 'smearing'
> degauss = 0.0018874
> smearing = 'fermi-dirac'
> ntyp = 1
> nat = 4
> assume_isolated = '2D'
> /
> &ELECTRONS
> conv_thr = 7.599999999999999e-05
> mixing_mode = 'plain'
> mixing_beta = 0.1
> /
> &IONS
> /
> &CELL
> /
>
> ATOMIC_SPECIES
> C 12.011 C_ncsr_0.5_pbe.upf
>
> K_POINTS automatic
> 8 8 1 0 0 0
>
> CELL_PARAMETERS angstrom
> 2.4622899999999999 0.0000000000000000 0.0000000000000000
> 1.2310682316596653 2.1324961988004443 0.0000000000000000
> 0.0000000000000000 0.0000000000000000 23.3000000000000007
>
> ATOMIC_POSITIONS angstrom
> C 2.4622407526646328 0.0000426499239760 9.9535270000000011
> C 1.2310701657767995 0.7108036329841640 9.9532939999999996
> C 1.2310805438773487 2.1324748738384565 13.3464730000000014
> C 2.4620787720005488 1.4216712408542924 13.3467060000000011
>
>
> "small":
> same as big but with:
>
> CELL_PARAMETERS angstrom
> 2.4622899999999999 0.0000000000000000 0.0000000000000000
> 1.2310682316596653 2.1324961988004443 0.0000000000000000
> 0.0000000000000000 0.0000000000000000 17.3040246000000018
>
> ATOMIC_POSITIONS angstrom
> C 2.4622407526646328 0.0000426499239760 6.9555393000000016
> C 1.2310701657767995 0.7108036329841640 6.9553063000000002
> C 1.2310805438773487 2.1324748738384565 10.3484853000000019
> C 2.4620787720005488 1.4216712408542924 10.3487183000000016
>
> --
> Lenz Fiedler, M. Sc.
> PhD Candidate | Machine Learning for Materials Design
>
> Tel.: +49 3581 37523 55
> E-Mail: l.fiedler at hzdr.de
> https://www.casus.science
>
> CASUS - Center for Advanced Systems Understanding
> Helmholtz-Zentrum Dresden-Rossendorf e.V. (HZDR)
> Conrad-Schiedt-Straße 20
> 02826 Görlitz
>
> Vorstand: Prof. Dr. Sebastian M. Schmidt, Dr. Diana Stiller
> Vereinsregister: VR 1693 beim Amtsgericht Dresden
>
>
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--
Paolo Giannozzi, Dip. Scienze Matematiche Informatiche e Fisiche,
Univ. Udine, via delle Scienze 206, 33100 Udine Italy, +39-0432-558216
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