Structure of ZrO2 fluorite

Total energy, geometry optimization, DFT+U, spin....

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ilukacevic
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Location: Dept. of Physics, University J. J. Strossmayer, Osijek, Croatia
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Structure of ZrO2 fluorite

Post by ilukacevic » Wed Mar 17, 2010 8:40 am

Dear colleagues,

I'm trying to reproduce phonon frequencies at the X point of the BZ of ZrO2 fluorite. However, whatever I tried concerning the response function calculation, I failed.
Therefore, I am unsure if I am using the correct structure. Could anyone, please, help me and confirm that I'm using the correct structure. My input file is bellow.

Thank you all in advance!

Yours
Igor Lukacevic



# Crystalline ZrO2 - fluorite : computation of the response to atomic displacements, at q=X

ndtset 2

#Ground state calculation
kptopt1 1 # Automatic generation of k points, taking
# into account the symmetry
tolvrs1 1.0d-15 # SCF stopping criterion
iscf1 5 # Self-consistent calculation, using algorithm 5

#Response Function calculation : electric field perturbation and phonons
rfphon2 1 # Activate the calculation of the atomic dispacement perturbations
rfatpol2 1 3 # All the atoms will be displaced
rfdir2 1 1 1 # All directions are selected. However, symmetries will be used to decrease
# the number of perturbations, so only the x electric field is needed
# (and this explains why in the second dataset, rfdir was set to 1 0 0).
nqpt2 1
qpt2 0.0 0.5 0.5 # This is a calculation at X point

getwfk2 1 # Uses as input wfs the output wfs of the dataset 1

kptopt2 3 # Automatic generation of k points,
# no use of symmetries to decrease
# the size of the k point set.
tolvrs2 1.0d-8
iscf2 5 # Self-consistent calculation, using algorithm 5

#######################################################################
#Common input variables

#Definition of the unit cell
acell 3*9.47118842767
rprim 0.0 0.5 0.5
0.5 0.0 0.5
0.5 0.5 0.0

#Definition of the atom types
ntypat 2
znucl 40 8 8

#Definition of the atoms
natom 3
typat 1 2 2
xred 0.00 0.00 0.00
0.25 0.25 0.25
0.75 0.75 0.75

#Gives the number of band, explicitely (do not take the default)
nband 14

#Exchange-correlation functional
ixc 3

#Definition of the planewave basis set
ecut 100
ecutsm 0.5

#Definition of the k-point grid
ngkpt 3*10
nshiftk 4
shiftk 0.5 0.5 0.5
0.5 0.0 0.0
0.0 0.5 0.0
0.0 0.0 0.5

#Definition of the SCF procedure
nstep 100
diemac 4.0

mverstra
Posts: 655
Joined: Wed Aug 19, 2009 12:01 pm

Re: Structure of ZrO2 fluorite

Post by mverstra » Thu Mar 18, 2010 8:48 am

Hello Igor,

Your input looks more or less ok - what do you mean you "failed" to do the phonon run?

1) use iscf 7, it's better
2) your ecut is huge

Matthieu
Matthieu Verstraete
University of Liege, Belgium

mverstra
Posts: 655
Joined: Wed Aug 19, 2009 12:01 pm

Re: Structure of ZrO2 fluorite

Post by mverstra » Thu Mar 18, 2010 8:49 am

PS: znucl only need 2 values (nytpat=2)
Matthieu Verstraete
University of Liege, Belgium

ilukacevic
Posts: 271
Joined: Sat Jan 16, 2010 12:05 pm
Location: Dept. of Physics, University J. J. Strossmayer, Osijek, Croatia
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Re: Structure of ZrO2 fluorite

Post by ilukacevic » Fri Mar 19, 2010 8:30 am

Dear prof. Verstraete,

mverstra wrote:PS: znucl only need 2 values (nytpat=2)


Understood.

mverstra wrote:Your input looks more or less ok - what do you mean you "failed" to do the phonon run?

1) use iscf 7, it's better
2) your ecut is huge

Matthieu


It's not that the run failes - abinit works perfectly - but by "failed" I meant that, although I get an almost perfect agreement for phonons at Gamma point (and Z* and diel. const.), at any other point in the BZ I obtain almost complete inagreement. I have already posted my problems in the Response function section, but all the suggestions (ranging from rfasr and various tols to anaddb input file) failed to correct these errors.

I supposed that problem lies somewhere else and wanted to check if the structure itself is correct. For I have run out of ideas how to reproduce phonon dispersions in ZrO2 fluorite.

1) just to mention: iscf 5 is a leftover from the relaxation, which worked nicely with it; rf calc. works good with it also.
2) I deliberately put ecut to high, since I wanted to check the convergence of phonon freqs (this was a desperate run). Although I knew that good results are obtained with even ecut 40 for Teters' extended norm pseudos. I was just trying all the possibilities.


Thank You very much for confirmation! But this has two sides, since now I know that the structure is not the reason for terrible phonon dispersions.

Yours,

Igor Lukacevic

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