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- From: "Gao Tao" <gaotaoscu@hotmail.com>
- To: forum@abinit.org
- Subject: Informations are missing in the DDB
- Date: Sun, 23 Jul 2006 18:42:05 +0800
Dr. Sir,
I am a new user of ABINIT package, and met a problem when using the ABINIT to calculate the phonon band structures and thermodynamical properties for LaNi5. The error appeared at the step of computating interatomic force constants,and the error information is as follow:
symdm9 : ERROR -
Informations are missing in the DDB.
The dynamical matrix number 17 cannot be built,
since no blok with wavevector 0.000000E+00 0.000000E+00 2.500000E-01
has been found.
Action : add the required blok in the DDB, or modify your input file.
I do not know what is wrong with my input files. Would you like to help and let me know which input file should be corrected? and which parameter should be adjusted?
Thanks in advance!
the input files are
1.trf2_4.in
2.trf2_1.in
1.trf2_4.in
!Input file for the ifc code. Analysis of the AlAs DDB
!Flags
ifcflag 1 ! Interatomic force constant flag
!Wavevector grid number 1 (coarse grid, from DDB)
brav 4 ! Bravais Lattice : 1-S.C., 2-F.C., 3-B.C., 4-Hex.)
ngqpt 4 4 4 ! Monkhorst-Pack indices
nqshft 1 ! number of q-points in repeated basic q-cell
q1shft 3*0.0
!Effective charges
asr 1 ! Acoustic Sum Rule. 1 => imposed asymetrically
chneut 1 ! Charge neutrality requirement for effective charges.
!Interatomic force constant info
dipdip 1 ! Dipole-dipole interaction treatment
ifcana 1 ! Analysis of the IFCs
ifcout 20 ! Number of IFC's written in the output, per atom
natifc 1 ! Number of atoms in the cell for which ifc's are analysed
atifc 1 ! List of atoms
2.trf2_1 is as follow,
trf2_1.in,
# Crystalline LaNi5 : computation of the phonon spectrum
ndtset 10
#Set 1 : ground state self-consistency
getwfk1 0 # Cancel default
kptopt1 1 # Automatic generation of k points, taking
# into account the symmetry
nqpt1 0 # Cancel default
tolvrs1 1.0d-18 # SCF stopping criterion (modify default)
rfphon1 0 # Cancel default
#Q vectors for all datasets
#Complete set of symmetry-inequivalent qpt chosen to be commensurate
# with kpt mesh so that only one set of GS wave functions is needed.
#Generated automatically by running GS calculation with kptopt=1,
# nshift=0, shiftk=0 0 0 (to include gamma) and taking output kpt set
# file as qpt set. Set nstep=1 so only one iteration runs.
nqpt 1 # One qpt for each dataset (only 0 or 1 allowed)
# This is the default for all datasets and must
# be explicitly turned off for dataset 1.
qpt2 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt3 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt4 2.50000000E-01 0.00000000E+00 0.00000000E+00
qpt5 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt6 2.50000000E-01 2.50000000E-01 0.00000000E+00
qpt7 5.00000000E-01 2.50000000E-01 0.00000000E+00
qpt8 -2.50000000E-01 2.50000000E-01 0.00000000E+00
qpt9 5.00000000E-01 5.00000000E-01 0.00000000E+00
qpt10 -2.50000000E-01 5.00000000E-01 2.50000000E-01
#Set 2 : Response function calculation of d/dk wave function
iscf2 -3 # Need this non-self-consistent option for d/dk
kptopt2 2 # Modify default to use time-reversal symmetry
rfphon2 0 # Cancel default
rfelfd2 2 # Calculate d/dk wave function only
tolvrs2 0.0 # Cancel default for d/dk
tolwfr2 1.0d-22 # Use wave function residual criterion instead
#Set 3 : Response function calculation of Q=0 phonons and electric field pert.
getddk3 2 # d/dk wave functions from last dataset
kptopt3 2 # Modify default to use time-reversal symmetry
rfelfd3 3 # Electric-field perturbation response only
#Sets 4-10 : Finite-wave-vector phonon calculations (defaults for all datasets)
getwfk 1 # Use GS wave functions from dataset1
kptopt 3 # Need full k-point set for finite-Q response
rfphon 1 # Do phonon response
rfatpol 1 2 # Treat displacements of all atoms
rfdir 1 1 1 # Do all directions (symmetry will be used)
tolvrs 1.0d-8 # This default is active for sets 3-10
#######################################################################
#Common input variables
#Definition of the unit cell
acell 9.486 9.486 7.527 # the length of primitive vecter(in Bohr)
angdeg 90 90 120
spgroup 191
#Definition of the atom types
ntypat 2 # There are two types of atom
znucl 57 28 # 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, type 1 is the La,
# type 2 is the Ni.
#Definition of the atoms
natom 6 # There are two atoms
typat 1 2 2 2 2 2 # The first is of type 1 (La), the second is of type 2 (Ni).
xred 0.0 0.0 0.0
1/3 2/3 0.0
2/3 1/3 0.0
1/2 0.0 1/2
0.0 1/2 1/2
1/2 1/2 1/2
#Gives the number of band, explicitely (do not take the default)
nband 28 occopt 3
#Exchange-correlation functional
ixc 1 # LDA Teter Pade parametrization
#Definition of the planewave basis set
ecut 3.0 # Maximal kinetic energy cut-off, in Hartree
#Definition of the k-point grid
ngkpt 4 4 4 nshiftk 4 # Use one copy of grid only (default)
shiftk 0.0 0.0 0.5 # This gives the usual fcc Monkhorst-Pack grid
0.0 0.5 0.0
0.5 0.0 0.0
0.5 0.5 0.5
#Definition of the SCF procedure
iscf 5 # Self-consistent calculation, using algorithm 5
nstep 25 # Maximal number of SCF cycles
diemac 9.0 # 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.
# The dielectric constant of AlAs is smaller that the
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- Informations are missing in the DDB, Gao Tao, 07/23/2006
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