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.Version 10.1.4.5 of ABINIT, released Sep 2024.
.(MPI version, prepared for a x86_64_linux_gnu13.2 computer)
.Copyright (C) 1998-2025 ABINIT group .
ABINIT comes with ABSOLUTELY NO WARRANTY.
It is free software, and you are welcome to redistribute it
under certain conditions (GNU General Public License,
see ~abinit/COPYING or http://www.gnu.org/copyleft/gpl.txt).
ABINIT is a project of the Universite Catholique de Louvain,
Corning Inc. and other collaborators, see ~abinit/doc/developers/contributors.txt .
Please read https://docs.abinit.org/theory/acknowledgments for suggested
acknowledgments of the ABINIT effort.
For more information, see https://www.abinit.org .
.Starting date : Fri 13 Sep 2024.
- ( at 19h11 )
- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/v5_t96-t97-t98-t99/t96.abi
- output file -> t96.abo
- root for input files -> t96i
- root for output files -> t96o
DATASET 1 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 1.
intxc = 0 ionmov = 0 iscf = 7 lmnmax = 2
lnmax = 2 mgfft = 16 mpssoang = 3 mqgrid = 3001
natom = 1 nloc_mem = 1 nspden = 2 nspinor = 1
nsppol = 2 nsym = 48 n1xccc = 2501 ntypat = 1
occopt = 7 xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
mpw = 69 nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 3.446 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.238 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 2 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 2 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 3.801 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 3 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 3 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 3.801 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 4 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 4 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 3.801 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 5 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 5 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 4.122 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 6 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 6 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 4.122 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 7 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 7 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 4.122 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 8 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 8 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 4.122 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 9 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 9 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 4.122 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
DATASET 10 : space group Fm -3 m (#225); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 10 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 7
xclevel = 1
- mband = 14 mffmem = 1 mkmem = 8
- mkqmem = 8 mk1mem = 8 mpw = 138
nfft = 4096 nkpt = 8
================================================================================
P This job should need less than 4.122 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.474 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
================================================================================
--------------------------------------------------------------------------------
------------- Echo of variables that govern the present computation ------------
--------------------------------------------------------------------------------
-
- outvars: echo of selected default values
- iomode0 = 0 , fftalg0 =512 , wfoptalg0 = 0
-
- outvars: echo of global parameters not present in the input file
- max_nthreads = 0
-
-outvars: echo values of preprocessed input variables --------
acell 7.0000000000E+00 7.0000000000E+00 7.0000000000E+00 Bohr
amu 5.86900000E+01
asr 0
chneut 0
ecut 1.00000000E+01 Hartree
- fftalg 512
getwfk1 0
getwfk2 1
getwfk3 1
getwfk4 1
getwfk5 1
getwfk6 1
getwfk7 1
getwfk8 1
getwfk9 1
getwfk10 1
istwfk1 2 3 6 7 4 5 8 9
istwfk2 1 1 1 1 1 1 1 1
istwfk3 1 1 1 1 1 1 1 1
istwfk4 1 1 1 1 1 1 1 1
istwfk5 1 1 1 1 1 1 1 1
istwfk6 1 1 1 1 1 1 1 1
istwfk7 1 1 1 1 1 1 1 1
istwfk8 1 1 1 1 1 1 1 1
istwfk9 1 1 1 1 1 1 1 1
istwfk10 1 1 1 1 1 1 1 1
jdtset 1 2 3 4 5 6 7 8 9 10
kpt 0.00000000E+00 0.00000000E+00 0.00000000E+00
5.00000000E-01 0.00000000E+00 0.00000000E+00
0.00000000E+00 5.00000000E-01 0.00000000E+00
5.00000000E-01 5.00000000E-01 0.00000000E+00
0.00000000E+00 0.00000000E+00 5.00000000E-01
5.00000000E-01 0.00000000E+00 5.00000000E-01
0.00000000E+00 5.00000000E-01 5.00000000E-01
5.00000000E-01 5.00000000E-01 5.00000000E-01
kptopt 3
kptrlatt 2 0 0 0 2 0 0 0 2
kptrlen 9.89949494E+00
P mkmem 8
P mkqmem 8
P mk1mem 8
natom 1
nband 14
nbdbuf 4
ndtset 10
ngfft 16 16 16
nkpt 8
nline1 8
nline2 4
nline3 4
nline4 4
nline5 4
nline6 4
nline7 4
nline8 4
nline9 4
nline10 4
nnsclo1 2
nnsclo2 0
nnsclo3 0
nnsclo4 0
nnsclo5 0
nnsclo6 0
nnsclo7 0
nnsclo8 0
nnsclo9 0
nnsclo10 0
nqpt1 0
nqpt2 1
nqpt3 1
nqpt4 1
nqpt5 1
nqpt6 1
nqpt7 1
nqpt8 1
nqpt9 1
nqpt10 1
nspden 2
nsppol 2
nstep 800
nsym 48
ntypat 1
occ 1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
occopt 7
optdriver1 0
optdriver2 1
optdriver3 1
optdriver4 1
optdriver5 1
optdriver6 1
optdriver7 1
optdriver8 1
optdriver9 1
optdriver10 1
prtdos1 2
prtdos2 0
prtdos3 0
prtdos4 0
prtdos5 0
prtdos6 0
prtdos7 0
prtdos8 0
prtdos9 0
prtdos10 0
prtpot1 0
prtpot2 1
prtpot3 1
prtpot4 1
prtpot5 1
prtpot6 1
prtpot7 1
prtpot8 1
prtpot9 1
prtpot10 1
qpt1 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt2 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt3 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt4 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt5 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt6 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt7 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt8 5.00000000E-01 5.00000000E-01 0.00000000E+00
qpt9 5.00000000E-01 5.00000000E-01 0.00000000E+00
qpt10 5.00000000E-01 5.00000000E-01 0.00000000E+00
rfdir1 1 1 1
rfdir2 1 0 0
rfdir3 0 1 0
rfdir4 0 0 1
rfdir5 1 0 0
rfdir6 0 1 0
rfdir7 0 0 1
rfdir8 1 0 0
rfdir9 0 1 0
rfdir10 0 0 1
rfphon1 0
rfphon2 1
rfphon3 1
rfphon4 1
rfphon5 1
rfphon6 1
rfphon7 1
rfphon8 1
rfphon9 1
rfphon10 1
rprim 0.0000000000E+00 5.0000000000E-01 5.0000000000E-01
5.0000000000E-01 0.0000000000E+00 5.0000000000E-01
5.0000000000E-01 5.0000000000E-01 0.0000000000E+00
spgroup 225
spinat1 0.0000000000E+00 0.0000000000E+00 2.0000000000E-01
spinat2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat3 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat4 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat5 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat6 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat7 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat8 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat9 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat10 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
symrel 1 0 0 0 1 0 0 0 1 -1 0 0 0 -1 0 0 0 -1
0 -1 1 0 -1 0 1 -1 0 0 1 -1 0 1 0 -1 1 0
-1 0 0 -1 0 1 -1 1 0 1 0 0 1 0 -1 1 -1 0
0 1 -1 1 0 -1 0 0 -1 0 -1 1 -1 0 1 0 0 1
-1 0 0 -1 1 0 -1 0 1 1 0 0 1 -1 0 1 0 -1
0 -1 1 1 -1 0 0 -1 0 0 1 -1 -1 1 0 0 1 0
1 0 0 0 0 1 0 1 0 -1 0 0 0 0 -1 0 -1 0
0 1 -1 0 0 -1 1 0 -1 0 -1 1 0 0 1 -1 0 1
-1 0 1 -1 1 0 -1 0 0 1 0 -1 1 -1 0 1 0 0
0 -1 0 1 -1 0 0 -1 1 0 1 0 -1 1 0 0 1 -1
1 0 -1 0 0 -1 0 1 -1 -1 0 1 0 0 1 0 -1 1
0 1 0 0 0 1 1 0 0 0 -1 0 0 0 -1 -1 0 0
1 0 -1 0 1 -1 0 0 -1 -1 0 1 0 -1 1 0 0 1
0 -1 0 0 -1 1 1 -1 0 0 1 0 0 1 -1 -1 1 0
-1 0 1 -1 0 0 -1 1 0 1 0 -1 1 0 0 1 -1 0
0 1 0 1 0 0 0 0 1 0 -1 0 -1 0 0 0 0 -1
0 0 -1 0 1 -1 1 0 -1 0 0 1 0 -1 1 -1 0 1
1 -1 0 0 -1 1 0 -1 0 -1 1 0 0 1 -1 0 1 0
0 0 1 1 0 0 0 1 0 0 0 -1 -1 0 0 0 -1 0
-1 1 0 -1 0 0 -1 0 1 1 -1 0 1 0 0 1 0 -1
0 0 1 0 1 0 1 0 0 0 0 -1 0 -1 0 -1 0 0
1 -1 0 0 -1 0 0 -1 1 -1 1 0 0 1 0 0 1 -1
0 0 -1 1 0 -1 0 1 -1 0 0 1 -1 0 1 0 -1 1
-1 1 0 -1 0 1 -1 0 0 1 -1 0 1 0 -1 1 0 0
tolvrs1 0.00000000E+00
tolvrs2 1.00000000E-05
tolvrs3 1.00000000E-05
tolvrs4 1.00000000E-05
tolvrs5 1.00000000E-05
tolvrs6 1.00000000E-05
tolvrs7 1.00000000E-05
tolvrs8 1.00000000E-05
tolvrs9 1.00000000E-05
tolvrs10 1.00000000E-05
tolwfr1 1.00000000E-14
tolwfr2 0.00000000E+00
tolwfr3 0.00000000E+00
tolwfr4 0.00000000E+00
tolwfr5 0.00000000E+00
tolwfr6 0.00000000E+00
tolwfr7 0.00000000E+00
tolwfr8 0.00000000E+00
tolwfr9 0.00000000E+00
tolwfr10 0.00000000E+00
tsmear 1.00000000E-03 Hartree
typat 1
wtk 0.12500 0.12500 0.12500 0.12500 0.12500 0.12500
0.12500 0.12500
znucl 28.00000
================================================================================
chkinp: Checking input parameters for consistency, jdtset= 1.
chkinp: Checking input parameters for consistency, jdtset= 2.
chkinp: Checking input parameters for consistency, jdtset= 3.
chkinp: Checking input parameters for consistency, jdtset= 4.
chkinp: Checking input parameters for consistency, jdtset= 5.
chkinp: Checking input parameters for consistency, jdtset= 6.
chkinp: Checking input parameters for consistency, jdtset= 7.
chkinp: Checking input parameters for consistency, jdtset= 8.
chkinp: Checking input parameters for consistency, jdtset= 9.
chkinp: Checking input parameters for consistency, jdtset= 10.
================================================================================
== DATASET 1 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 1, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 69, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 0, ionmov: 0, optcell: 0, iscf: 7, paral_kgb: 0, }
...
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.27076
getcut : COMMENT -
Note that boxcut > 2.2 ; recall that boxcut=Gcut(box)/Gcut(sphere) = 2
is sufficient for exact treatment of convolution.
Such a large boxcut is a waste : you could raise ecut
e.g. ecut= 12.890912 Hartrees makes boxcut=2
--- Pseudopotential description ------------------------------------------------
- pspini: atom type 1 psp file is /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/PseudosTM_pwteter/28ni.pspnc
- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/PseudosTM_pwteter/28ni.pspnc
- Troullier-Martins psp for element Ni Thu Oct 27 17:35:45 EDT 1994
- 28.00000 10.00000 940714 znucl, zion, pspdat
1 1 2 0 2001 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
0 3.208 7.754 0 2.9454613 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
1 1.322 4.017 1 2.9454613 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
2 19.888 25.467 1 2.2939080 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
1.28166113122492 4.34983513722262 7.99170458696768 rchrg,fchrg,qchrg
pspatm : epsatm= 55.54189636
--- l ekb(1:nproj) -->
1 0.797683
2 -7.688688
pspatm: atomic psp has been read and splines computed
5.55418964E+02 ecore*ucvol(ha*bohr**3)
--------------------------------------------------------------------------------
_setup2: Arith. and geom. avg. npw (full set) are 129.625 129.182
================================================================================
--- !BeginCycle
iteration_state: {dtset: 1, }
solver: {iscf: 7, nstep: 800, nline: 8, wfoptalg: 0, }
tolerances: {tolwfr: 1.00E-14, }
...
iter Etot(hartree) deltaE(h) residm vres2 magn
ETOT 1 -35.773220506268 -3.58E+01 1.79E-02 4.96E+01 0.500
ETOT 2 -35.798029380427 -2.48E-02 3.47E-06 4.74E+00 0.501
ETOT 3 -35.800714952205 -2.69E-03 1.58E-10 2.59E-02 0.500
ETOT 4 -35.800740240201 -2.53E-05 2.30E-13 9.72E-04 0.518
ETOT 5 -35.800911149545 -1.71E-04 9.19E-15 1.66E-02 0.634
At SCF step 5 max residual= 9.19E-15 < tolwfr= 1.00E-14 =>converged.
Cartesian components of stress tensor (hartree/bohr^3)
sigma(1 1)= 8.12979825E-02 sigma(3 2)= 0.00000000E+00
sigma(2 2)= 8.12979825E-02 sigma(3 1)= 0.00000000E+00
sigma(3 3)= 8.12979825E-02 sigma(2 1)= 0.00000000E+00
--- !ResultsGS
iteration_state: {dtset: 1, }
comment : Summary of ground state results
lattice_vectors:
- [ 0.0000000, 3.5000000, 3.5000000, ]
- [ 3.5000000, 0.0000000, 3.5000000, ]
- [ 3.5000000, 3.5000000, 0.0000000, ]
lattice_lengths: [ 4.94975, 4.94975, 4.94975, ]
lattice_angles: [ 60.000, 60.000, 60.000, ] # degrees, (23, 13, 12)
lattice_volume: 8.5750000E+01
convergence: {deltae: -1.709E-04, res2: 1.663E-02, residm: 9.187E-15, diffor: null, }
etotal : -3.58009111E+01
entropy : 0.00000000E+00
fermie : 1.41755898E-01
cartesian_stress_tensor: # hartree/bohr^3
- [ 8.12979825E-02, 0.00000000E+00, 0.00000000E+00, ]
- [ 0.00000000E+00, 8.12979825E-02, 0.00000000E+00, ]
- [ 0.00000000E+00, 0.00000000E+00, 8.12979825E-02, ]
pressure_GPa: -2.3919E+03
xred :
- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Ni]
cartesian_forces: # hartree/bohr
- [ -0.00000000E+00, -0.00000000E+00, -0.00000000E+00, ]
force_length_stats: {min: 0.00000000E+00, max: 0.00000000E+00, mean: 0.00000000E+00, }
...
Integrated electronic and magnetization densities in atomic spheres:
---------------------------------------------------------------------
Radius=ratsph(iatom), smearing ratsm= 0.0000. Diff(up-dn)=approximate z local magnetic moment.
Atom Radius up_density dn_density Total(up+dn) Diff(up-dn)
1 2.00000 3.851830 3.232297 7.084127 0.619533
---------------------------------------------------------------------
Sum: 3.851830 3.232297 7.084127 0.619533
Total magnetization (from the atomic spheres): 0.619533
Total magnetization (exact up - dn): 0.634140
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 20.830E-16; max= 91.867E-16
reduced coordinates (array xred) for 1 atoms
0.000000000000 0.000000000000 0.000000000000
rms dE/dt= 0.0000E+00; max dE/dt= 0.0000E+00; dE/dt below (all hartree)
1 0.000000000000 0.000000000000 0.000000000000
cartesian coordinates (angstrom) at end:
1 0.00000000000000 0.00000000000000 0.00000000000000
cartesian forces (hartree/bohr) at end:
1 -0.00000000000000 -0.00000000000000 -0.00000000000000
frms,max,avg= 0.0000000E+00 0.0000000E+00 0.000E+00 0.000E+00 0.000E+00 h/b
cartesian forces (eV/Angstrom) at end:
1 -0.00000000000000 -0.00000000000000 -0.00000000000000
frms,max,avg= 0.0000000E+00 0.0000000E+00 0.000E+00 0.000E+00 0.000E+00 e/A
length scales= 7.000000000000 7.000000000000 7.000000000000 bohr
= 3.704240460130 3.704240460130 3.704240460130 angstroms
prteigrs : about to open file t96o_DS1_EIG
Fermi (or HOMO) energy (hartree) = 0.14176 Average Vxc (hartree)= -0.53902
Magnetization (Bohr magneton)= 6.34140429E-01
Total spin up = 5.31707021E+00 Total spin down = 4.68292979E+00
Eigenvalues (hartree) for nkpt= 8 k points, SPIN UP:
kpt# 1, nband= 14, wtk= 0.12500, kpt= 0.0000 0.0000 0.0000 (reduced coord)
-0.55555 -0.08557 -0.08557 -0.08557 0.12053 0.12053 0.58502 0.68024
0.68024 0.68024 0.71107 1.09736 1.09736 1.09736
occupation numbers for kpt# 1
1.00000 1.00000 1.00000 1.00000 1.00000 1.00000 0.00000 0.00000
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
prteigrs : prtvol=0 or 1, do not print more k-points.
Eigenvalues (hartree) for nkpt= 8 k points, SPIN DOWN:
kpt# 1, nband= 14, wtk= 0.12500, kpt= 0.0000 0.0000 0.0000 (reduced coord)
-0.54818 -0.06808 -0.06808 -0.06808 0.14132 0.14132 0.59541 0.68995
0.68995 0.68995 0.71238 1.10213 1.10213 1.10213
occupation numbers for kpt# 1
1.00000 1.00000 1.00000 1.00000 0.73172 0.73172 0.00000 0.00000
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
prteigrs : prtvol=0 or 1, do not print more k-points.
--- !EnergyTerms
iteration_state : {dtset: 1, }
comment : Components of total free energy in Hartree
kinetic : 2.06086471075274E+01
hartree : 2.49712711396610E+00
xc : -1.34494341012913E+01
Ewald energy : -3.27490148150987E+01
psp_core : 6.47718907985571E+00
local_psp : -3.62793224724037E+00
non_local_psp : -1.55571569251450E+01
internal : -3.58005747874260E+01
'-kT*entropy' : -3.36362118939307E-04
total_energy : -3.58009111495450E+01
total_energy_eV : -9.74192335828022E+02
band_energy : -1.02410270479720E+00
...
Cartesian components of stress tensor (hartree/bohr^3)
sigma(1 1)= 8.12979825E-02 sigma(3 2)= 0.00000000E+00
sigma(2 2)= 8.12979825E-02 sigma(3 1)= 0.00000000E+00
sigma(3 3)= 8.12979825E-02 sigma(2 1)= 0.00000000E+00
-Cartesian components of stress tensor (GPa) [Pressure= -2.3919E+03 GPa]
- sigma(1 1)= 2.39186882E+03 sigma(3 2)= 0.00000000E+00
- sigma(2 2)= 2.39186882E+03 sigma(3 1)= 0.00000000E+00
- sigma(3 3)= 2.39186882E+03 sigma(2 1)= 0.00000000E+00
================================================================================
== DATASET 2 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 2, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.27076
getcut : COMMENT -
Note that boxcut > 2.2 ; recall that boxcut=Gcut(box)/Gcut(sphere) = 2
is sufficient for exact treatment of convolution.
Such a large boxcut is a waste : you could raise ecut
e.g. ecut= 12.890912 Hartrees makes boxcut=2
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 1 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Perturbation : displacement of atom 1 along direction 1
Found 4 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 5 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 2, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 131.90291570781 -2.768E+03 9.410E+00 9.969E+04
ETOT 2 30.285336106726 -1.016E+02 1.283E-01 2.020E+04
ETOT 3 0.41093603101589 -2.987E+01 2.056E-02 3.458E+01
ETOT 4 0.37133843573119 -3.960E-02 1.984E-05 4.306E-02
ETOT 5 0.37126856694576 -6.987E-05 8.303E-08 2.547E-03
ETOT 6 0.37126242718304 -6.140E-06 4.977E-09 1.586E-05
ETOT 7 0.37126239985727 -2.733E-08 3.335E-11 4.869E-06
At SCF step 7 vres2 = 4.87E-06 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 54.124E-13; max= 33.354E-12
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 3.07200671E+03 eigvalue= 1.75553465E+01 local= -3.82802622E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -1.45477322E+02 Hartree= 1.25088691E+02 xc= -4.05769902E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 4.93545908E+01 enl0= 5.88734391E+01 enl1= -5.65352097E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.89949913E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 0.00000000E+00
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582102E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.3712623999E+00 Ha. Also 2DEtotal= 0.101025636753E+02 eV
(2DErelax= -2.8994991270E+03 Ha. 2DEnonrelax= 2.8998703894E+03 Ha)
( non-var. 2DEtotal : 3.7124124977E-01 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 0.3712412498 0.0000000000
1 1 2 1 0.1856206249 0.0000000000
1 1 3 1 0.1856206249 0.0000000000
1 1 2 3 0.0000000000 0.0000000000
1 1 3 3 0.0000000000 0.0000000000
2 1 1 1 0.1856206249 0.0000000000
2 1 2 1 0.3712412498 0.0000000000
2 1 3 1 0.1856206249 0.0000000000
2 1 1 3 0.0000000000 0.0000000000
2 1 3 3 0.0000000000 0.0000000000
3 1 1 1 0.1856206249 0.0000000000
3 1 2 1 0.1856206249 0.0000000000
3 1 3 1 0.3712412498 0.0000000000
3 1 1 3 0.0000000000 0.0000000000
3 1 2 3 0.0000000000 0.0000000000
1 3 2 1 0.0000000000 0.0000000000
1 3 3 1 0.0000000000 0.0000000000
2 3 1 1 0.0000000000 0.0000000000
2 3 3 1 0.0000000000 0.0000000000
3 3 1 1 0.0000000000 0.0000000000
3 3 2 1 0.0000000000 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 0.0151527041 0.0000000000
1 1 2 1 -0.0000000000 0.0000000000
1 1 3 1 0.0000000000 0.0000000000
2 1 1 1 -0.0000000000 0.0000000000
2 1 2 1 0.0151527041 0.0000000000
2 1 3 1 -0.0000000000 0.0000000000
3 1 1 1 0.0000000000 0.0000000000
3 1 2 1 -0.0000000000 0.0000000000
3 1 3 1 0.0151527041 0.0000000000
Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.00000
Phonon energies in Hartree :
3.763422E-04 3.763422E-04 3.763422E-04
Phonon frequencies in cm-1 :
- 8.259757E+01 8.259757E+01 8.259757E+01
================================================================================
== DATASET 3 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 3, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.27076
getcut : COMMENT -
Note that boxcut > 2.2 ; recall that boxcut=Gcut(box)/Gcut(sphere) = 2
is sufficient for exact treatment of convolution.
Such a large boxcut is a waste : you could raise ecut
e.g. ecut= 12.890912 Hartrees makes boxcut=2
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 2 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Perturbation : displacement of atom 1 along direction 2
Found 4 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 5 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 131.98804425091 -2.768E+03 9.123E+00 9.972E+04
ETOT 2 30.311706674143 -1.017E+02 1.277E-01 2.022E+04
ETOT 3 0.41072319120948 -2.990E+01 2.057E-02 3.441E+01
ETOT 4 0.37133716441312 -3.939E-02 1.972E-05 4.351E-02
ETOT 5 0.37126683446022 -7.033E-05 8.478E-08 2.548E-03
ETOT 6 0.37126069229097 -6.142E-06 4.941E-09 1.616E-05
ETOT 7 0.37126065473930 -3.755E-08 3.488E-11 5.368E-07
At SCF step 7 vres2 = 5.37E-07 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 56.226E-13; max= 34.878E-12
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 3.07200671E+03 eigvalue= 1.75553463E+01 local= -3.82802622E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -1.45477320E+02 Hartree= 1.25088689E+02 xc= -4.05769898E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 4.93545923E+01 enl0= 5.88734396E+01 enl1= -5.65352098E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.89949913E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 0.00000000E+00
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582102E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.3712606547E+00 Ha. Also 2DEtotal= 0.101025161882E+02 eV
(2DErelax= -2.8994991287E+03 Ha. 2DEnonrelax= 2.8998703894E+03 Ha)
( non-var. 2DEtotal : 3.7124017116E-01 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 0.3712401712 0.0000000000
1 1 2 1 0.1856200856 0.0000000000
1 1 3 1 0.1856200856 0.0000000000
1 1 2 3 0.0000000000 0.0000000000
1 1 3 3 0.0000000000 0.0000000000
2 1 1 1 0.1856200856 0.0000000000
2 1 2 1 0.3712401712 0.0000000000
2 1 3 1 0.1856200856 0.0000000000
2 1 1 3 0.0000000000 0.0000000000
2 1 3 3 0.0000000000 0.0000000000
3 1 1 1 0.1856200856 0.0000000000
3 1 2 1 0.1856200856 0.0000000000
3 1 3 1 0.3712401712 0.0000000000
3 1 1 3 0.0000000000 0.0000000000
3 1 2 3 0.0000000000 0.0000000000
1 3 2 1 0.0000000000 0.0000000000
1 3 3 1 0.0000000000 0.0000000000
2 3 1 1 0.0000000000 0.0000000000
2 3 3 1 0.0000000000 0.0000000000
3 3 1 1 0.0000000000 0.0000000000
3 3 2 1 0.0000000000 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 0.0151526600 0.0000000000
1 1 2 1 0.0000000000 0.0000000000
1 1 3 1 -0.0000000000 0.0000000000
2 1 1 1 0.0000000000 0.0000000000
2 1 2 1 0.0151526600 0.0000000000
2 1 3 1 0.0000000000 0.0000000000
3 1 1 1 -0.0000000000 0.0000000000
3 1 2 1 0.0000000000 0.0000000000
3 1 3 1 0.0151526600 0.0000000000
Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.00000
Phonon energies in Hartree :
3.763417E-04 3.763417E-04 3.763417E-04
Phonon frequencies in cm-1 :
- 8.259745E+01 8.259745E+01 8.259745E+01
================================================================================
== DATASET 4 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 4, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.27076
getcut : COMMENT -
Note that boxcut > 2.2 ; recall that boxcut=Gcut(box)/Gcut(sphere) = 2
is sufficient for exact treatment of convolution.
Such a large boxcut is a waste : you could raise ecut
e.g. ecut= 12.890912 Hartrees makes boxcut=2
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 3 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Perturbation : displacement of atom 1 along direction 3
Found 4 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 5 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 4, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 131.91151024561 -2.768E+03 9.279E+00 9.970E+04
ETOT 2 30.288127502692 -1.016E+02 1.283E-01 2.020E+04
ETOT 3 0.41091152820255 -2.988E+01 2.056E-02 3.457E+01
ETOT 4 0.37133306788283 -3.958E-02 1.982E-05 4.309E-02
ETOT 5 0.37126317743324 -6.989E-05 8.320E-08 2.547E-03
ETOT 6 0.37125703889424 -6.139E-06 4.975E-09 1.576E-05
ETOT 7 0.37125701044980 -2.844E-08 3.335E-11 9.100E-07
At SCF step 7 vres2 = 9.10E-07 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 53.392E-13; max= 33.347E-12
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 3.07200672E+03 eigvalue= 1.75553464E+01 local= -3.82802622E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -1.45477322E+02 Hartree= 1.25088691E+02 xc= -4.05769903E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 4.93545924E+01 enl0= 5.88734393E+01 enl1= -5.65352099E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.89949913E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 0.00000000E+00
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582102E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.3712570104E+00 Ha. Also 2DEtotal= 0.101024170221E+02 eV
(2DErelax= -2.8994991324E+03 Ha. 2DEnonrelax= 2.8998703894E+03 Ha)
( non-var. 2DEtotal : 3.7123594048E-01 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 0.3712359405 0.0000000000
1 1 2 1 0.1856179702 0.0000000000
1 1 3 1 0.1856179702 0.0000000000
1 1 2 3 0.0000000000 0.0000000000
1 1 3 3 0.0000000000 0.0000000000
2 1 1 1 0.1856179702 0.0000000000
2 1 2 1 0.3712359405 0.0000000000
2 1 3 1 0.1856179702 0.0000000000
2 1 1 3 0.0000000000 0.0000000000
2 1 3 3 0.0000000000 0.0000000000
3 1 1 1 0.1856179702 0.0000000000
3 1 2 1 0.1856179702 0.0000000000
3 1 3 1 0.3712359405 0.0000000000
3 1 1 3 0.0000000000 0.0000000000
3 1 2 3 0.0000000000 0.0000000000
1 3 2 1 0.0000000000 0.0000000000
1 3 3 1 0.0000000000 0.0000000000
2 3 1 1 0.0000000000 0.0000000000
2 3 3 1 0.0000000000 0.0000000000
3 3 1 1 0.0000000000 0.0000000000
3 3 2 1 0.0000000000 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 0.0151524874 0.0000000000
1 1 2 1 -0.0000000000 0.0000000000
1 1 3 1 -0.0000000000 0.0000000000
2 1 1 1 -0.0000000000 0.0000000000
2 1 2 1 0.0151524874 0.0000000000
2 1 3 1 -0.0000000000 0.0000000000
3 1 1 1 -0.0000000000 0.0000000000
3 1 2 1 -0.0000000000 0.0000000000
3 1 3 1 0.0151524874 0.0000000000
Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.00000
Phonon energies in Hartree :
3.763395E-04 3.763395E-04 3.763395E-04
Phonon frequencies in cm-1 :
- 8.259698E+01 8.259698E+01 8.259698E+01
================================================================================
== DATASET 5 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 5, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.5000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.13120
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 1 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.500000 0.000000 0.000000
Perturbation : displacement of atom 1 along direction 1
Found 2 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 6 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 5, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 2299.3246757654 -8.235E+02 9.328E+00 4.664E+06
ETOT 2 1019.8116808751 -1.280E+03 1.985E+00 1.368E+06
ETOT 3 288.25959816179 -7.316E+02 4.899E-01 1.695E+04
ETOT 4 280.33102375494 -7.929E+00 4.016E-03 1.308E+01
ETOT 5 280.31326368886 -1.776E-02 1.366E-05 9.235E-01
ETOT 6 280.31226756711 -9.961E-04 4.538E-07 3.989E-02
ETOT 7 280.31222597529 -4.159E-05 1.452E-08 9.182E-03
ETOT 8 280.31222491467 -1.061E-06 5.028E-08 1.969E-02
ETOT 9 280.31221306433 -1.185E-05 8.709E-11 9.258E-04
ETOT 10 280.31221235958 -7.047E-07 1.412E-10 2.923E-06
At SCF step 10 vres2 = 2.92E-06 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 21.758E-12; max= 14.115E-11
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.78557964E+03 eigvalue= 1.65432059E+01 local= -3.62243192E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -5.49542247E+02 Hartree= 3.07052231E+02 xc= -4.69270802E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 7.40424387E+01 enl0= 6.84805812E+01 enl1= -5.13551334E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.84252776E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 2.22969642E+02
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582158E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.2803122124E+03 Ha. Also 2DEtotal= 0.762768321116E+04 eV
(2DErelax= -2.8425277638E+03 Ha. 2DEnonrelax= 3.1228399762E+03 Ha)
( non-var. 2DEtotal : 2.8031218274E+02 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 280.3121827434 0.0000000000
1 1 2 1 80.5362331426 0.0000000000
1 1 3 1 80.5362331426 0.0000000000
2 1 1 1 80.5362331426 -0.0000000000
3 1 1 1 80.5362331426 -0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
Phonon wavevector (reduced coordinates) : 0.50000 0.00000 0.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00
chkph3 : WARNING -
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
================================================================================
== DATASET 6 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 6, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.5000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.13120
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 2 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.500000 0.000000 0.000000
Perturbation : displacement of atom 1 along direction 2
The set of symmetries contains only one element for this perturbation.
symkpt : not enough symmetry to change the number of k points.
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 6, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 368.72165189740 -2.548E+03 1.079E+01 1.536E+05
ETOT 2 247.78835158460 -1.209E+02 2.059E-01 5.795E+04
ETOT 3 161.16265362150 -8.663E+01 4.088E-02 7.406E+01
ETOT 4 161.07251088270 -9.014E-02 3.539E-05 9.356E-02
ETOT 5 161.07236595413 -1.449E-04 1.288E-07 5.195E-03
ETOT 6 161.07235370570 -1.225E-05 9.915E-09 1.589E-03
ETOT 7 161.07235238968 -1.316E-06 8.079E-10 5.531E-05
ETOT 8 161.07235237305 -1.663E-08 2.314E-11 4.529E-05
ETOT 9 161.07235235300 -2.005E-08 3.226E-13 1.338E-05
ETOT 10 161.07235234463 -8.367E-09 1.898E-13 7.149E-08
At SCF step 10 vres2 = 7.15E-08 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 24.710E-15; max= 18.978E-14
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.89664646E+03 eigvalue= 1.80843404E+01 local= -3.66294953E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -1.63658391E+02 Hartree= 1.29800205E+02 xc= -4.06745940E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 5.65704732E+01 enl0= 6.10558907E+01 enl1= -5.34671725E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.75518782E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 1.63897982E+01
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582118E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.1610723523E+03 Ha. Also 2DEtotal= 0.438300160888E+04 eV
(2DErelax= -2.7551878197E+03 Ha. 2DEnonrelax= 2.9162601721E+03 Ha)
( non-var. 2DEtotal : 1.6107235239E+02 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 2 1 80.5362208658 -0.0000000000
1 1 3 1 80.5362208658 -0.0000000000
2 1 1 1 80.5362208658 0.0000000000
2 1 2 1 161.0723523852 0.0000000000
2 1 3 1 80.5361123609 0.0000000000
3 1 1 1 80.5362208658 0.0000000000
3 1 2 1 80.5361123609 -0.0000000000
3 1 3 1 161.0723523852 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
Phonon wavevector (reduced coordinates) : 0.50000 0.00000 0.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00
chkph3 : WARNING -
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
================================================================================
== DATASET 7 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 7, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.5000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.13120
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 3 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.500000 0.000000 0.000000
Perturbation : displacement of atom 1 along direction 3
The set of symmetries contains only one element for this perturbation.
symkpt : not enough symmetry to change the number of k points.
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 7, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 369.35167830840 -2.547E+03 1.162E+01 1.539E+05
ETOT 2 248.21222387841 -1.211E+02 2.473E-01 5.823E+04
ETOT 3 161.15966512133 -8.705E+01 5.559E-02 7.178E+01
ETOT 4 161.07252040902 -8.714E-02 3.431E-05 9.993E-02
ETOT 5 161.07236431655 -1.561E-04 1.385E-07 4.722E-03
ETOT 6 161.07235099677 -1.332E-05 1.179E-08 3.549E-04
ETOT 7 161.07235044029 -5.565E-07 4.663E-10 6.245E-05
ETOT 8 161.07235073801 2.977E-07 2.688E-11 5.817E-04
ETOT 9 161.07235037386 -3.641E-07 1.866E-12 7.660E-07
At SCF step 9 vres2 = 7.66E-07 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 33.346E-14; max= 18.659E-13
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.89664648E+03 eigvalue= 1.80843411E+01 local= -3.66294954E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -1.63658417E+02 Hartree= 1.29800230E+02 xc= -4.06745997E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 5.65704724E+01 enl0= 6.10558881E+01 enl1= -5.34671726E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.75518782E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 1.63897982E+01
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582118E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.1610723504E+03 Ha. Also 2DEtotal= 0.438300155526E+04 eV
(2DErelax= -2.7551878217E+03 Ha. 2DEnonrelax= 2.9162601721E+03 Ha)
( non-var. 2DEtotal : 1.6107233435E+02 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 2 1 80.5361043389 -0.0000000000
1 1 3 1 80.5361043389 -0.0000000000
2 1 1 1 80.5361043389 0.0000000000
2 1 2 1 161.0723343519 0.0000000000
2 1 3 1 80.5361503078 0.0000000000
3 1 1 1 80.5361043389 0.0000000000
3 1 2 1 80.5361503078 -0.0000000000
3 1 3 1 161.0723343519 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
Phonon wavevector (reduced coordinates) : 0.50000 0.00000 0.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00
chkph3 : WARNING -
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
================================================================================
== DATASET 8 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 8, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.5000 0.5000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.13357
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 1 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.500000 0.500000 0.000000
Perturbation : displacement of atom 1 along direction 1
Found 2 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 6 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 8, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 1252.9022581923 -1.798E+03 1.054E+01 1.754E+06
ETOT 2 599.29951034323 -6.536E+02 9.444E-01 5.274E+05
ETOT 3 207.32906275740 -3.920E+02 1.687E-01 3.066E+03
ETOT 4 204.81948580399 -2.510E+00 1.397E-03 1.815E+02
ETOT 5 204.67506317284 -1.444E-01 5.994E-05 1.288E-01
ETOT 6 204.67696233938 1.899E-03 1.642E-07 2.412E+00
ETOT 7 204.67509053119 -1.872E-03 9.062E-10 2.306E-01
ETOT 8 204.67488056298 -2.100E-04 1.674E-08 6.798E-04
ETOT 9 204.67487948400 -1.079E-06 8.135E-10 4.247E-05
ETOT 10 204.67487963203 1.480E-07 3.557E-11 6.165E-05
ETOT 11 204.67487942480 -2.072E-07 2.193E-12 6.827E-06
At SCF step 11 vres2 = 6.83E-06 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 39.846E-14; max= 21.934E-13
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.86895768E+03 eigvalue= 1.71932034E+01 local= -3.71834443E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -4.21324986E+02 Hartree= 2.51466657E+02 xc= -4.73100021E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 5.90698808E+01 enl0= 6.82880598E+01 enl1= -5.27033741E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.84583136E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 1.50635903E+02
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582156E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.2046748794E+03 Ha. Also 2DEtotal= 0.556948671053E+04 eV
(2DErelax= -2.8458313596E+03 Ha. 2DEnonrelax= 3.0505062391E+03 Ha)
( non-var. 2DEtotal : 2.0467504010E+02 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 204.6750401019 0.0000000000
1 1 2 1 132.2068882357 0.0000000000
1 1 3 1 72.4681518662 0.0000000000
2 1 1 1 132.2068882357 0.0000000000
2 1 2 1 204.6750401019 0.0000000000
2 1 3 1 72.4681518662 0.0000000000
3 1 1 1 72.4681518662 0.0000000000
3 1 2 1 72.4681518662 0.0000000000
3 1 3 1 144.9363037324 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 5.9157674993 0.0000000000
1 1 2 1 -0.0000000000 0.0000000000
1 1 3 1 -0.0000000000 0.0000000000
2 1 1 1 -0.0000000000 0.0000000000
2 1 2 1 5.9157674993 0.0000000000
2 1 3 1 -0.0000000000 0.0000000000
3 1 1 1 -0.0000000000 0.0000000000
3 1 2 1 -0.0000000000 0.0000000000
3 1 3 1 10.7923990396 0.0000000000
Phonon wavevector (reduced coordinates) : 0.50000 0.50000 0.00000
Phonon energies in Hartree :
7.436070E-03 7.436070E-03 1.004377E-02
Phonon frequencies in cm-1 :
- 1.632029E+03 1.632029E+03 2.204353E+03
================================================================================
== DATASET 9 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 9, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.5000 0.5000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.13357
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 2 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.500000 0.500000 0.000000
Perturbation : displacement of atom 1 along direction 2
Found 2 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 6 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 9, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 1256.0458288146 -1.794E+03 8.791E+00 1.758E+06
ETOT 2 601.50208284568 -6.545E+02 9.464E-01 5.303E+05
ETOT 3 207.29890616257 -3.942E+02 1.694E-01 3.021E+03
ETOT 4 204.81938333174 -2.480E+00 1.388E-03 1.813E+02
ETOT 5 204.67506327370 -1.443E-01 5.986E-05 1.304E-01
ETOT 6 204.67626500944 1.202E-03 1.668E-07 1.601E+00
ETOT 7 204.67518770136 -1.077E-03 7.850E-10 3.459E-01
ETOT 8 204.67487876455 -3.089E-04 1.676E-08 6.818E-04
ETOT 9 204.67487768362 -1.081E-06 8.162E-10 4.240E-05
ETOT 10 204.67487773075 4.713E-08 3.802E-11 3.484E-05
ETOT 11 204.67487763801 -9.274E-08 1.638E-12 1.004E-05
ETOT 12 204.67487760494 -3.307E-08 3.868E-12 5.938E-07
At SCF step 12 vres2 = 5.94E-07 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 58.639E-14; max= 38.683E-13
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.86895778E+03 eigvalue= 1.71932038E+01 local= -3.71834452E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -4.21325218E+02 Hartree= 2.51466880E+02 xc= -4.73100332E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 5.90698787E+01 enl0= 6.82880507E+01 enl1= -5.27033745E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.84583136E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 1.50635903E+02
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582156E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.2046748776E+03 Ha. Also 2DEtotal= 0.556948666101E+04 eV
(2DErelax= -2.8458313615E+03 Ha. 2DEnonrelax= 3.0505062391E+03 Ha)
( non-var. 2DEtotal : 2.0467490323E+02 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 204.6749032267 0.0000000000
1 1 2 1 132.2067995589 0.0000000000
1 1 3 1 72.4681036678 0.0000000000
2 1 1 1 132.2067995589 0.0000000000
2 1 2 1 204.6749032267 0.0000000000
2 1 3 1 72.4681036678 0.0000000000
3 1 1 1 72.4681036678 0.0000000000
3 1 2 1 72.4681036678 0.0000000000
3 1 3 1 144.9362073357 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 5.9157635647 0.0000000000
1 1 2 1 -0.0000000000 -0.0000000000
1 1 3 1 -0.0000000000 -0.0000000000
2 1 1 1 -0.0000000000 -0.0000000000
2 1 2 1 5.9157635647 0.0000000000
2 1 3 1 0.0000000000 0.0000000000
3 1 1 1 -0.0000000000 0.0000000000
3 1 2 1 -0.0000000000 -0.0000000000
3 1 3 1 10.7923918007 0.0000000000
Phonon wavevector (reduced coordinates) : 0.50000 0.50000 0.00000
Phonon energies in Hartree :
7.436067E-03 7.436067E-03 1.004377E-02
Phonon frequencies in cm-1 :
- 1.632028E+03 1.632028E+03 2.204353E+03
================================================================================
== DATASET 10 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 10, }
dimensions: {natom: 1, nkpt: 8, mband: 14, nsppol: 2, nspinor: 1, nspden: 2, mpw: 138, }
cutoff_energies: {ecut: 10.0, pawecutdg: -1.0, }
electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-03, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: new Teter (4/93) with spin-polarized option - ixc=1
Citation for XC functional:
S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 3.5000000 3.5000000 G(1)= -0.1428571 0.1428571 0.1428571
R(2)= 3.5000000 0.0000000 3.5000000 G(2)= 0.1428571 -0.1428571 0.1428571
R(3)= 3.5000000 3.5000000 0.0000000 G(3)= 0.1428571 0.1428571 -0.1428571
Unit cell volume ucvol= 8.5750000E+01 bohr^3
Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.5000 0.5000 0.0000 ngfft= 16 16 16
ecut(hartree)= 10.000 => boxcut(ratio)= 2.13357
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 3 ipert= 1
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.500000 0.500000 0.000000
Perturbation : displacement of atom 1 along direction 3
Found 2 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 6 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.000000E+01 and 1.000000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 10, }
solver: {iscf: 7, nstep: 800, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-05, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 571.40944342510 -2.386E+03 1.379E+01 3.927E+05
ETOT 2 374.38513705079 -1.970E+02 5.101E-01 1.849E+05
ETOT 3 145.36907078243 -2.290E+02 1.155E-01 3.996E+02
ETOT 4 144.93657375792 -4.325E-01 2.092E-04 2.110E-01
ETOT 5 144.93630192243 -2.718E-04 3.582E-07 8.606E-02
ETOT 6 144.95578643154 1.948E-02 8.690E-09 2.283E+01
ETOT 7 144.93619373510 -1.959E-02 1.254E-08 1.031E-03
ETOT 8 144.93619207557 -1.660E-06 1.568E-09 1.293E-04
ETOT 9 144.93619199449 -8.108E-08 3.739E-11 3.543E-06
At SCF step 9 vres2 = 3.54E-06 < tolvrs= 1.00E-05 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 58.114E-13; max= 37.389E-12
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.93521020E+03 eigvalue= 1.72062088E+01 local= -3.76428317E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -2.44185411E+02 Hartree= 1.68524675E+02 xc= -4.40162084E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 4.82697313E+01 enl0= 6.39353495E+01 enl1= -5.38121774E+03
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.81270152E+03
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 6.24027983E+01 fr.nonlo= 2.82708556E+03 Ewald= 5.77673534E+01
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.66582136E+02 frxc 2 = 1.76964137E+02
Resulting in :
2DEtotal= 0.1449361920E+03 Ha. Also 2DEtotal= 0.394391435557E+04 eV
(2DErelax= -2.8127015168E+03 Ha. 2DEnonrelax= 2.9576377088E+03 Ha)
( non-var. 2DEtotal : 1.4493613262E+02 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 1 72.4677177888 -0.0000000000
2 1 3 1 72.4677177888 0.0000000000
3 1 1 1 72.4677177888 0.0000000000
3 1 2 1 72.4677177888 -0.0000000000
3 1 3 1 144.9361326185 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
Phonon wavevector (reduced coordinates) : 0.50000 0.50000 0.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00
chkph3 : WARNING -
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
== END DATASET(S) ==============================================================
================================================================================
-outvars: echo values of variables after computation --------
acell 7.0000000000E+00 7.0000000000E+00 7.0000000000E+00 Bohr
amu 5.86900000E+01
asr 0
chneut 0
ecut 1.00000000E+01 Hartree
etotal1 -3.5800911150E+01
etotal2 3.7126239986E-01
etotal3 3.7126065474E-01
etotal4 3.7125701045E-01
etotal5 2.8031221236E+02
etotal6 1.6107235234E+02
etotal7 1.6107235037E+02
etotal8 2.0467487942E+02
etotal9 2.0467487760E+02
etotal10 1.4493619199E+02
fcart1 -0.0000000000E+00 -0.0000000000E+00 -0.0000000000E+00
fcart2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart3 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart4 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart5 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart6 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart7 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart8 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart9 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart10 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
- fftalg 512
getwfk1 0
getwfk2 1
getwfk3 1
getwfk4 1
getwfk5 1
getwfk6 1
getwfk7 1
getwfk8 1
getwfk9 1
getwfk10 1
istwfk1 2 3 6 7 4 5 8 9
istwfk2 1 1 1 1 1 1 1 1
istwfk3 1 1 1 1 1 1 1 1
istwfk4 1 1 1 1 1 1 1 1
istwfk5 1 1 1 1 1 1 1 1
istwfk6 1 1 1 1 1 1 1 1
istwfk7 1 1 1 1 1 1 1 1
istwfk8 1 1 1 1 1 1 1 1
istwfk9 1 1 1 1 1 1 1 1
istwfk10 1 1 1 1 1 1 1 1
jdtset 1 2 3 4 5 6 7 8 9 10
kpt 0.00000000E+00 0.00000000E+00 0.00000000E+00
5.00000000E-01 0.00000000E+00 0.00000000E+00
0.00000000E+00 5.00000000E-01 0.00000000E+00
5.00000000E-01 5.00000000E-01 0.00000000E+00
0.00000000E+00 0.00000000E+00 5.00000000E-01
5.00000000E-01 0.00000000E+00 5.00000000E-01
0.00000000E+00 5.00000000E-01 5.00000000E-01
5.00000000E-01 5.00000000E-01 5.00000000E-01
kptopt 3
kptrlatt 2 0 0 0 2 0 0 0 2
kptrlen 9.89949494E+00
P mkmem 8
P mkqmem 8
P mk1mem 8
natom 1
nband 14
nbdbuf 4
ndtset 10
ngfft 16 16 16
nkpt 8
nline1 8
nline2 4
nline3 4
nline4 4
nline5 4
nline6 4
nline7 4
nline8 4
nline9 4
nline10 4
nnsclo1 2
nnsclo2 0
nnsclo3 0
nnsclo4 0
nnsclo5 0
nnsclo6 0
nnsclo7 0
nnsclo8 0
nnsclo9 0
nnsclo10 0
nqpt1 0
nqpt2 1
nqpt3 1
nqpt4 1
nqpt5 1
nqpt6 1
nqpt7 1
nqpt8 1
nqpt9 1
nqpt10 1
nspden 2
nsppol 2
nstep 800
nsym 48
ntypat 1
occ 1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.567070
0.567070 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.567070
0.567070 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.567070
0.567070 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.567070
0.567070 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.731719 0.731719
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 0.000000
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
0.000000 0.000000
occopt 7
optdriver1 0
optdriver2 1
optdriver3 1
optdriver4 1
optdriver5 1
optdriver6 1
optdriver7 1
optdriver8 1
optdriver9 1
optdriver10 1
prtdos1 2
prtdos2 0
prtdos3 0
prtdos4 0
prtdos5 0
prtdos6 0
prtdos7 0
prtdos8 0
prtdos9 0
prtdos10 0
prtpot1 0
prtpot2 1
prtpot3 1
prtpot4 1
prtpot5 1
prtpot6 1
prtpot7 1
prtpot8 1
prtpot9 1
prtpot10 1
qpt1 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt2 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt3 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt4 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt5 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt6 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt7 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt8 5.00000000E-01 5.00000000E-01 0.00000000E+00
qpt9 5.00000000E-01 5.00000000E-01 0.00000000E+00
qpt10 5.00000000E-01 5.00000000E-01 0.00000000E+00
rfdir1 1 1 1
rfdir2 1 0 0
rfdir3 0 1 0
rfdir4 0 0 1
rfdir5 1 0 0
rfdir6 0 1 0
rfdir7 0 0 1
rfdir8 1 0 0
rfdir9 0 1 0
rfdir10 0 0 1
rfphon1 0
rfphon2 1
rfphon3 1
rfphon4 1
rfphon5 1
rfphon6 1
rfphon7 1
rfphon8 1
rfphon9 1
rfphon10 1
rprim 0.0000000000E+00 5.0000000000E-01 5.0000000000E-01
5.0000000000E-01 0.0000000000E+00 5.0000000000E-01
5.0000000000E-01 5.0000000000E-01 0.0000000000E+00
spgroup 225
spinat1 0.0000000000E+00 0.0000000000E+00 2.0000000000E-01
spinat2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat3 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat4 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat5 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat6 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat7 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat8 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat9 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
spinat10 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten1 8.1297982544E-02 8.1297982544E-02 8.1297982544E-02
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten3 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten4 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten5 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten6 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten7 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten8 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten9 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten10 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
symrel 1 0 0 0 1 0 0 0 1 -1 0 0 0 -1 0 0 0 -1
0 -1 1 0 -1 0 1 -1 0 0 1 -1 0 1 0 -1 1 0
-1 0 0 -1 0 1 -1 1 0 1 0 0 1 0 -1 1 -1 0
0 1 -1 1 0 -1 0 0 -1 0 -1 1 -1 0 1 0 0 1
-1 0 0 -1 1 0 -1 0 1 1 0 0 1 -1 0 1 0 -1
0 -1 1 1 -1 0 0 -1 0 0 1 -1 -1 1 0 0 1 0
1 0 0 0 0 1 0 1 0 -1 0 0 0 0 -1 0 -1 0
0 1 -1 0 0 -1 1 0 -1 0 -1 1 0 0 1 -1 0 1
-1 0 1 -1 1 0 -1 0 0 1 0 -1 1 -1 0 1 0 0
0 -1 0 1 -1 0 0 -1 1 0 1 0 -1 1 0 0 1 -1
1 0 -1 0 0 -1 0 1 -1 -1 0 1 0 0 1 0 -1 1
0 1 0 0 0 1 1 0 0 0 -1 0 0 0 -1 -1 0 0
1 0 -1 0 1 -1 0 0 -1 -1 0 1 0 -1 1 0 0 1
0 -1 0 0 -1 1 1 -1 0 0 1 0 0 1 -1 -1 1 0
-1 0 1 -1 0 0 -1 1 0 1 0 -1 1 0 0 1 -1 0
0 1 0 1 0 0 0 0 1 0 -1 0 -1 0 0 0 0 -1
0 0 -1 0 1 -1 1 0 -1 0 0 1 0 -1 1 -1 0 1
1 -1 0 0 -1 1 0 -1 0 -1 1 0 0 1 -1 0 1 0
0 0 1 1 0 0 0 1 0 0 0 -1 -1 0 0 0 -1 0
-1 1 0 -1 0 0 -1 0 1 1 -1 0 1 0 0 1 0 -1
0 0 1 0 1 0 1 0 0 0 0 -1 0 -1 0 -1 0 0
1 -1 0 0 -1 0 0 -1 1 -1 1 0 0 1 0 0 1 -1
0 0 -1 1 0 -1 0 1 -1 0 0 1 -1 0 1 0 -1 1
-1 1 0 -1 0 1 -1 0 0 1 -1 0 1 0 -1 1 0 0
tolvrs1 0.00000000E+00
tolvrs2 1.00000000E-05
tolvrs3 1.00000000E-05
tolvrs4 1.00000000E-05
tolvrs5 1.00000000E-05
tolvrs6 1.00000000E-05
tolvrs7 1.00000000E-05
tolvrs8 1.00000000E-05
tolvrs9 1.00000000E-05
tolvrs10 1.00000000E-05
tolwfr1 1.00000000E-14
tolwfr2 0.00000000E+00
tolwfr3 0.00000000E+00
tolwfr4 0.00000000E+00
tolwfr5 0.00000000E+00
tolwfr6 0.00000000E+00
tolwfr7 0.00000000E+00
tolwfr8 0.00000000E+00
tolwfr9 0.00000000E+00
tolwfr10 0.00000000E+00
tsmear 1.00000000E-03 Hartree
typat 1
wtk 0.12500 0.12500 0.12500 0.12500 0.12500 0.12500
0.12500 0.12500
znucl 28.00000
================================================================================
- Timing analysis has been suppressed with timopt=0
================================================================================
Suggested references for the acknowledgment of ABINIT usage.
The users of ABINIT have little formal obligations with respect to the ABINIT group
(those specified in the GNU General Public License, http://www.gnu.org/copyleft/gpl.txt).
However, it is common practice in the scientific literature,
to acknowledge the efforts of people that have made the research possible.
In this spirit, please find below suggested citations of work written by ABINIT developers,
corresponding to implementations inside of ABINIT that you have used in the present run.
Note also that it will be of great value to readers of publications presenting these results,
to read papers enabling them to understand the theoretical formalism and details
of the ABINIT implementation.
For information on why they are suggested, see also https://docs.abinit.org/theory/acknowledgments.
-
- [1] The Abinit project: Impact, environment and recent developments.
- Computer Phys. Comm. 248, 107042 (2020).
- X.Gonze, B. Amadon, G. Antonius, F.Arnardi, L.Baguet, J.-M.Beuken,
- J.Bieder, F.Bottin, J.Bouchet, E.Bousquet, N.Brouwer, F.Bruneval,
- G.Brunin, T.Cavignac, J.-B. Charraud, Wei Chen, M.Cote, S.Cottenier,
- J.Denier, G.Geneste, Ph.Ghosez, M.Giantomassi, Y.Gillet, O.Gingras,
- D.R.Hamann, G.Hautier, Xu He, N.Helbig, N.Holzwarth, Y.Jia, F.Jollet,
- W.Lafargue-Dit-Hauret, K.Lejaeghere, M.A.L.Marques, A.Martin, C.Martins,
- H.P.C. Miranda, F.Naccarato, K. Persson, G.Petretto, V.Planes, Y.Pouillon,
- S.Prokhorenko, F.Ricci, G.-M.Rignanese, A.H.Romero, M.M.Schmitt, M.Torrent,
- M.J.van Setten, B.Van Troeye, M.J.Verstraete, G.Zerah and J.W.Zwanzig
- Comment: the fifth generic paper describing the ABINIT project.
- Note that a version of this paper, that is not formatted for Computer Phys. Comm.
- is available at https://www.abinit.org/sites/default/files/ABINIT20.pdf .
- The licence allows the authors to put it on the Web.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze2020
-
- [2] First-principles responses of solids to atomic displacements and homogeneous electric fields:,
- implementation of a conjugate-gradient algorithm. X. Gonze, Phys. Rev. B55, 10337 (1997).
- Comment: Non-vanishing rfphon and/or rfelfd, in the norm-conserving case.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze1997
-
- [3] Dynamical matrices, Born effective charges, dielectric permittivity tensors, and ,
- interatomic force constants from density-functional perturbation theory,
- X. Gonze and C. Lee, Phys. Rev. B55, 10355 (1997).
- Comment: Non-vanishing rfphon and/or rfelfd, in the norm-conserving case.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze1997a
-
- [4] ABINIT: Overview, and focus on selected capabilities
- J. Chem. Phys. 152, 124102 (2020).
- A. Romero, D.C. Allan, B. Amadon, G. Antonius, T. Applencourt, L.Baguet,
- J.Bieder, F.Bottin, J.Bouchet, E.Bousquet, F.Bruneval,
- G.Brunin, D.Caliste, M.Cote,
- J.Denier, C. Dreyer, Ph.Ghosez, M.Giantomassi, Y.Gillet, O.Gingras,
- D.R.Hamann, G.Hautier, F.Jollet, G. Jomard,
- A.Martin,
- H.P.C. Miranda, F.Naccarato, G.Petretto, N.A. Pike, V.Planes,
- S.Prokhorenko, T. Rangel, F.Ricci, G.-M.Rignanese, M.Royo, M.Stengel, M.Torrent,
- M.J.van Setten, B.Van Troeye, M.J.Verstraete, J.Wiktor, J.W.Zwanziger, and X.Gonze.
- Comment: a global overview of ABINIT, with focus on selected capabilities .
- Note that a version of this paper, that is not formatted for J. Chem. Phys
- is available at https://www.abinit.org/sites/default/files/ABINIT20_JPC.pdf .
- The licence allows the authors to put it on the Web.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#romero2020
-
- [5] Recent developments in the ABINIT software package.
- Computer Phys. Comm. 205, 106 (2016).
- X.Gonze, F.Jollet, F.Abreu Araujo, D.Adams, B.Amadon, T.Applencourt,
- C.Audouze, J.-M.Beuken, J.Bieder, A.Bokhanchuk, E.Bousquet, F.Bruneval
- D.Caliste, M.Cote, F.Dahm, F.Da Pieve, M.Delaveau, M.Di Gennaro,
- B.Dorado, C.Espejo, G.Geneste, L.Genovese, A.Gerossier, M.Giantomassi,
- Y.Gillet, D.R.Hamann, L.He, G.Jomard, J.Laflamme Janssen, S.Le Roux,
- A.Levitt, A.Lherbier, F.Liu, I.Lukacevic, A.Martin, C.Martins,
- M.J.T.Oliveira, S.Ponce, Y.Pouillon, T.Rangel, G.-M.Rignanese,
- A.H.Romero, B.Rousseau, O.Rubel, A.A.Shukri, M.Stankovski, M.Torrent,
- M.J.Van Setten, B.Van Troeye, M.J.Verstraete, D.Waroquier, J.Wiktor,
- B.Xu, A.Zhou, J.W.Zwanziger.
- Comment: the fourth generic paper describing the ABINIT project.
- Note that a version of this paper, that is not formatted for Computer Phys. Comm.
- is available at https://www.abinit.org/sites/default/files/ABINIT16.pdf .
- The licence allows the authors to put it on the Web.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze2016
-
- Proc. 0 individual time (sec): cpu= 5.8 wall= 5.8
================================================================================
Calculation completed.
.Delivered 4 WARNINGs and 41 COMMENTs to log file.
+Overall time at end (sec) : cpu= 5.8 wall= 5.8
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