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- From: <dat36@cam.ac.uk>
- To: forum@abinit.org
- Subject: [abinit-forum] Phonon Frequencies Problem
- Date: Mon, 4 May 2009 14:08:19 +0200 (CEST)
Dear All,
I am having trouble finding correct phonon frequencies at Gamma
for
the d-metal system Ag5Pb2O6. I have calculated them before in the CASTEP
plane-wave code and wanted to repeat the calucation in ABINIT as a sanity
check
before using ABINIT to consider more properties.
With the following input file I am able to calculate an accurate band
structure, and I then use the WFK file from the SCF calculation as the input
to
my response function calculation.
# Ag5Pb2O6 BS
#
# Computation of the band structure.
# First, a SCF density computation, then a non-SCF band structure calculation.
ndtset 2
#Dataset 1 : usual self-consistent calculation
kptopt1 1 # Option for the automatic generation of k points,
# taking into account the symmetry
nshiftk1 4
shiftk1 0.5 0.5 0.5 # These shifts will be the same for all grids
0.5 0.0 0.0
0.0 0.5 0.0
0.0 0.0 0.5
ngkpt1 8 8 8
prtden1 1 # Print the density, for use by dataset 2
toldfe1 1.0d-8
#Dataset 2 : the band structure
iscf2 -2
getden2 -1
kptopt2 -4
nband2 100
ndivk2 28 19 29 45 # 10, 12 and 17 divisions of the 3 segments,
delimited
# by 4 points.
kptbounds2 0.0 0.0 0.0
0.5 0.0 0.0
0.333333 0.333333 0.0
0.0 0.0 0.0
0.0 0.0 0.5
tolwfr2 1.0d-16
#enunit2 1 # Will output the eigenenergies in eV
#Definition of the unit cell
acell 3*1.8897 # This is equivalent to 1 Angstrom each
rprim
5.137609105410803 -2.966200000000002 0.000000000000000
0.000000000000000 5.932400000000000 0.000000000000000
0.000000000000000 0.000000000000000 6.410500000000000
#Definition of the atom types
ntypat 3
znucl 8 47 82
#Definition of the atoms
natom 13 # There are two atoms
typat 1 1 1 1 1 1 2 2 2 2 2 3 3
xred # This keyword indicate that the location of the atoms
# will follow, one triplet of number for each atom
0.6222000122070313 0.0000000000000001 0.6888999938964855
-0.0000000000000001 0.6222000122070313 0.6888999938964855
-0.6222000122070311 -0.6222000122070314 0.6888999938964854
-0.0000000000000001 -0.6222000122070314 -0.6888999938964855
-0.6222000122070311 0.0000000000000001 -0.6888999938964855
0.6222000122070313 0.6222000122070313 -0.6888999938964854
0.0000000000000000 0.0000000000000000 0.2413000017404568
0.0000000000000000 0.0000000000000000 -0.2413000017404568
0.5000000000000000 -0.0000000000000000 0.0000000000000000
0.0000000000000000 0.5000000000000001 0.0000000000000000
-0.5000000000000000 -0.5000000000000001 -0.0000000000000000
0.6666666666666667 0.3333333333333334 0.5000000000000001
-0.6666666666666667 -0.3333333333333334 -0.5000000000000001
#Definition of the planewave basis set
ecut 40.0 # Maximal kinetic energy cut-off, in Hartree
#Definition of the SCF procedure
nstep 100 # Maximal number of SCF cycles
# Although this is not mandatory, it is worth to
# precondition the SCF cycle. The model dielectric
# function used as the standard preconditioner
# is described in the "dielng" input variable section.
occopt 7
tsmear 0.007
The input for the response function calculation for the density matrix at
Gamma
is:
# Crystalline Ag5Pb2O6: computation of the dynamical matrix at Gamma
#
#Response-function calculation, with q=0
rfphon 1 # Will consider phonon-type perturbation
rfatpol 1 13 # All the atoms will be displaced
rfdir 1 1 1 # Along all reduced coordinate axis
nqpt 1 # One wavevector is to be considered
qpt 0 0 0 # This wavevector is q=0 (Gamma)
kptopt 2 # Automatic generation of k points, taking
# into account the time-reversal symmetry only
tolvrs 1.0d-8 # SCF stopping criterion
iscf 5 # Self-consistent calculation, using algorithm 5
irdwfk 1 # Read the ground-state wavefunctions
#######################################################################
#Common input variables
#Definition of the unit cell
acell 3*1.8897 # This is equivalent to 1 Angstrom each
rprim
5.137609105410803 -2.966200000000002 0.000000000000000
0.000000000000000 5.932400000000000 0.000000000000000
0.000000000000000 0.000000000000000 6.410500000000000
#Definition of the atom types
ntypat 3 # There is only one type of atom
znucl 8 47 82 # The keyword "znucl" refers to the atomic number of
the
# possible type(s) of atom. The pseudopotential(s)
# mentioned in the "files" file must correspond
# to the type(s) of atom. Here, the only type is Silicon.
#Definition of the atoms
natom 13 # There are two atoms
typat 1 1 1 1 1 1 2 2 2 2 2 3 3
xred # This keyword indicate that the location of the atoms
# will follow, one triplet of number for each atom
0.6222000122070313 0.0000000000000001 0.6888999938964855
-0.0000000000000001 0.6222000122070313 0.6888999938964855
-0.6222000122070311 -0.6222000122070314 0.6888999938964854
-0.0000000000000001 -0.6222000122070314 -0.6888999938964855
-0.6222000122070311 0.0000000000000001 -0.6888999938964855
0.6222000122070313 0.6222000122070313 -0.6888999938964854
0.0000000000000000 0.0000000000000000 0.2413000017404568
0.0000000000000000 0.0000000000000000 -0.2413000017404568
0.5000000000000000 -0.0000000000000000 0.0000000000000000
0.0000000000000000 0.5000000000000001 0.0000000000000000
-0.5000000000000000 -0.5000000000000001 -0.0000000000000000
0.6666666666666667 0.3333333333333334 0.5000000000000001
-0.6666666666666667 -0.3333333333333334 -0.5000000000000001
#Definition of the planewave basis set
ecut 40.0 # Maximal kinetic energy cut-off, in Hartree
diemac 1000000
#Definition of the SCF procedure
nstep 100 # Maximal number of SCF cycles
# Although this is not mandatory, it is worth to
# precondition the SCF cycle. The model dielectric
# function used as the standard preconditioner
# is described in the "dielng" input variable section.
occopt 7
tsmear 0.007
#Definition of the k-point grid
kptrlatt -4 4 4 # In cartesian coordinates, this grid is simple cubic,
and
4 -4 4 # actually corresponds to the so-called 8x8x8
Monkhorst-Pack grid.
4 4 -4 # It might as well be obtained through the use of
# ngkpt, nshiftk and shiftk .
#Gives the number of band, explicitely (do not take the default)
nband 70 # For an insulator (if described correctly as an
insulator
# by DFT), there is no need to include conduction
bands
# in response-function calculations
#Exchange-correlation functional
ixc 1 # LDA Teter Pade parametrization
I obtain the following phonon frequencies:
Phonon frequencies in cm-1 :
- 8.173847E+01 8.385767E+01 9.066616E+01 9.157959E+01 9.161629E+01
- 1.007493E+02 1.056726E+02 1.056770E+02 1.167382E+02 1.169064E+02
- 1.215102E+02 1.215114E+02 1.273660E+02 1.273693E+02 1.359495E+02
- 1.436825E+02 1.559343E+02 1.559382E+02 2.079336E+02 2.079848E+02
- 2.190082E+02 2.002110E+03 2.002542E+03 2.003094E+03 2.003199E+03
- 2.008633E+03 2.010303E+03 2.010572E+03 2.012517E+03 2.022057E+03
- 2.022089E+03 2.022721E+03 2.025986E+03 2.037439E+03 2.038421E+03
- 2.039042E+03 2.039143E+03 2.039784E+03 2.040022E+03
However, I expected to see three acoustic phonons and none above 500cm^-1.
There were two types of warning in the output file, for example:
-P-0000 hdr_check: WARNING -
-P-0000 input nkpt= 128 not equal disk file nkpt= 52
-P-0000 cgwf3: WARNING -
-P-0000 New trial energy at line 4 = -4.421412E+02
-P-0000 is higher than former: -4.421412E+02
Any help is much appreciated.
Thanks,
David Tompsett.
- [abinit-forum] Phonon Frequencies Problem, dat36, 05/04/2009
- Re: [abinit-forum] Phonon Frequencies Problem, matthieu verstraete, 05/04/2009
- Re: [abinit-forum] Phonon Frequencies Problem, David Tompsett, 05/05/2009
- Re: [abinit-forum] Phonon Frequencies Problem, Xavier Gonze, 05/05/2009
- Re: [abinit-forum] Phonon Frequencies Problem, matthieu verstraete, 05/05/2009
- Re: [abinit-forum] Phonon Frequencies Problem, Xavier Gonze, 05/05/2009
- Re: [abinit-forum] Phonon Frequencies Problem, David Tompsett, 05/05/2009
- Re: [abinit-forum] Phonon Frequencies Problem, matthieu verstraete, 05/04/2009
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