unit cell is not primitive
Posted: Fri Apr 19, 2013 2:50 pm
Dear abinit users,
I am trying to calculate some properties of Eu2(MoO4)3, but it give me error as following. can you help me for correct input file. My input file is following.
thanks a lot.
ERROR:
chkinp: ERROR -
Atoms number 1 and 5 are located at the same point of the unit cell
(periodic images are taken into account).
Action: change the coordinate of one of these atoms in the input file.
#My input file:
# Eu2(MoO43_Monoclinic (space group:C2/c) : computation of the total energy
# Convergence with respect to the number of k points.
ndtset 25
#Definition of the k-point grids
kptopt 1 # Option for the automatic generation of k points, taking
# into account the symmetry
#nshiftk 4
#shiftk 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 2 2 2 # Definition of the different grids
#ngkpt2 4 4 4
#ngkpt3 6 6 6
ngkpt4 8 8 8
ecut: 20 ecut+ 2
getwfk -1 # This is to speed up the calculation, by restarting
# from previous wavefunctions, transferred from the old
# to the new k-points.
#Definition of the unit cell
acell 14.29 21.68 21.575 # This is equivalent to 10.18 10.18 10.18
angdeg 90 109.3093 90
spgroup 15
brvltt -1
#Definition of the atom types
ntypat 3 # There is only one type of atom
znucl 63 42 8 # 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 68 # There are two atoms
typat 8*1 12*2 48*3 # They both are of type 1, that is, Silicon
xred # This keyword indicate that the location of the atoms
# will follow, one triplet of number for each atom
0.332560 0.377130 0.408920
0.667440 0.377130 0.091080
0.667440 0.622870 0.591080
0.332560 0.622870 0.908920
0.832560 0.877130 0.408920
0.167440 0.877130 0.091080
0.167440 0.122870 0.591080
0.832560 0.122870 0.908920
0.000000 0.129350 0.250000
0.000000 0.870650 0.750000
0.500000 0.629350 0.250000
0.500000 0.370650 0.750000
0.149180 0.388530 0.059420
0.850820 0.388530 0.440580
0.850820 0.611470 0.940580
0.149180 0.611470 0.559420
0.649180 0.888530 0.059420
0.350820 0.888530 0.440580
0.350820 0.111470 0.940580
0.649180 0.111470 0.559420
0.449300 0.208200 0.064200
0.550700 0.208200 0.435800
0.550700 0.791800 0.935800
0.449300 0.791800 0.564200
0.949300 0.708200 0.064200
0.050700 0.708200 0.435800
0.050700 0.291800 0.935800
0.949300 0.291800 0.564200
0.136300 0.211200 0.387200
0.863700 0.211200 0.112800
0.863700 0.788800 0.612800
0.136300 0.788800 0.887200
0.636300 0.711200 0.387200
0.363700 0.711200 0.112800
0.363700 0.288800 0.612800
0.636300 0.288800 0.887200
0.250300 0.313200 0.198200
0.749700 0.313200 0.301800
0.749700 0.686800 0.801800
0.250300 0.686800 0.698200
0.750300 0.813200 0.198200
0.249700 0.813200 0.301800
0.249700 0.186800 0.801800
0.750300 0.186800 0.698200
0.346300 0.461100 0.039200
0.653700 0.461100 0.460800
0.653700 0.538900 0.960800
0.346300 0.538900 0.539200
0.846300 0.961100 0.039200
0.153700 0.961100 0.460800
0.153700 0.038900 0.960800
0.846300 0.038900 0.539200
0.033300 0.475200 0.394200
0.966700 0.475200 0.105800
0.966700 0.524800 0.605800
0.033300 0.524800 0.894200
0.533300 0.975200 0.394200
0.466700 0.975200 0.105800
0.466700 0.024800 0.605800
0.533300 0.024800 0.894200
0.449300 0.208200 0.064200
0.550700 0.208200 0.435800
0.550700 0.791800 0.935800
0.449300 0.791800 0.564200
0.949300 0.708200 0.064200
0.050700 0.708200 0.435800
0.050700 0.291800 0.935800
0.949300 0.291800 0.564200
#Definition of the planewave basis set
#ecut 8.0 # Maximal kinetic energy cut-off, in Hartree
#Definition of the SCF procedure
nstep 1000 # Maximal number of SCF cycles
toldfe 1.0d-6 # Will stop when, twice in a row, the difference
# between two consecutive evaluations of total energy
# differ by less than toldfe (in Hartree)
#diemac 12.0 # 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.
# Here, we follow the prescription for bulk silicon.
I am trying to calculate some properties of Eu2(MoO4)3, but it give me error as following. can you help me for correct input file. My input file is following.
thanks a lot.
ERROR:
chkinp: ERROR -
Atoms number 1 and 5 are located at the same point of the unit cell
(periodic images are taken into account).
Action: change the coordinate of one of these atoms in the input file.
#My input file:
# Eu2(MoO43_Monoclinic (space group:C2/c) : computation of the total energy
# Convergence with respect to the number of k points.
ndtset 25
#Definition of the k-point grids
kptopt 1 # Option for the automatic generation of k points, taking
# into account the symmetry
#nshiftk 4
#shiftk 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 2 2 2 # Definition of the different grids
#ngkpt2 4 4 4
#ngkpt3 6 6 6
ngkpt4 8 8 8
ecut: 20 ecut+ 2
getwfk -1 # This is to speed up the calculation, by restarting
# from previous wavefunctions, transferred from the old
# to the new k-points.
#Definition of the unit cell
acell 14.29 21.68 21.575 # This is equivalent to 10.18 10.18 10.18
angdeg 90 109.3093 90
spgroup 15
brvltt -1
#Definition of the atom types
ntypat 3 # There is only one type of atom
znucl 63 42 8 # 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 68 # There are two atoms
typat 8*1 12*2 48*3 # They both are of type 1, that is, Silicon
xred # This keyword indicate that the location of the atoms
# will follow, one triplet of number for each atom
0.332560 0.377130 0.408920
0.667440 0.377130 0.091080
0.667440 0.622870 0.591080
0.332560 0.622870 0.908920
0.832560 0.877130 0.408920
0.167440 0.877130 0.091080
0.167440 0.122870 0.591080
0.832560 0.122870 0.908920
0.000000 0.129350 0.250000
0.000000 0.870650 0.750000
0.500000 0.629350 0.250000
0.500000 0.370650 0.750000
0.149180 0.388530 0.059420
0.850820 0.388530 0.440580
0.850820 0.611470 0.940580
0.149180 0.611470 0.559420
0.649180 0.888530 0.059420
0.350820 0.888530 0.440580
0.350820 0.111470 0.940580
0.649180 0.111470 0.559420
0.449300 0.208200 0.064200
0.550700 0.208200 0.435800
0.550700 0.791800 0.935800
0.449300 0.791800 0.564200
0.949300 0.708200 0.064200
0.050700 0.708200 0.435800
0.050700 0.291800 0.935800
0.949300 0.291800 0.564200
0.136300 0.211200 0.387200
0.863700 0.211200 0.112800
0.863700 0.788800 0.612800
0.136300 0.788800 0.887200
0.636300 0.711200 0.387200
0.363700 0.711200 0.112800
0.363700 0.288800 0.612800
0.636300 0.288800 0.887200
0.250300 0.313200 0.198200
0.749700 0.313200 0.301800
0.749700 0.686800 0.801800
0.250300 0.686800 0.698200
0.750300 0.813200 0.198200
0.249700 0.813200 0.301800
0.249700 0.186800 0.801800
0.750300 0.186800 0.698200
0.346300 0.461100 0.039200
0.653700 0.461100 0.460800
0.653700 0.538900 0.960800
0.346300 0.538900 0.539200
0.846300 0.961100 0.039200
0.153700 0.961100 0.460800
0.153700 0.038900 0.960800
0.846300 0.038900 0.539200
0.033300 0.475200 0.394200
0.966700 0.475200 0.105800
0.966700 0.524800 0.605800
0.033300 0.524800 0.894200
0.533300 0.975200 0.394200
0.466700 0.975200 0.105800
0.466700 0.024800 0.605800
0.533300 0.024800 0.894200
0.449300 0.208200 0.064200
0.550700 0.208200 0.435800
0.550700 0.791800 0.935800
0.449300 0.791800 0.564200
0.949300 0.708200 0.064200
0.050700 0.708200 0.435800
0.050700 0.291800 0.935800
0.949300 0.291800 0.564200
#Definition of the planewave basis set
#ecut 8.0 # Maximal kinetic energy cut-off, in Hartree
#Definition of the SCF procedure
nstep 1000 # Maximal number of SCF cycles
toldfe 1.0d-6 # Will stop when, twice in a row, the difference
# between two consecutive evaluations of total energy
# differ by less than toldfe (in Hartree)
#diemac 12.0 # 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.
# Here, we follow the prescription for bulk silicon.