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abinit/tests/tutorespfn/Refs/tpolarization_2.abo

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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 19h03 )
- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/tutorespfn_tpolarization_2-tpolarization_3/tpolarization_2.abi
- output file -> tpolarization_2.abo
- root for input files -> tpolarization_2i
- root for output files -> tpolarization_2o
DATASET 1 : space group F-4 3 m (#216); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 1.
intxc = 0 ionmov = 0 iscf = 7 lmnmax = 6
lnmax = 6 mgfft = 16 mpssoang = 3 mqgrid = 3001
natom = 2 nloc_mem = 1 nspden = 1 nspinor = 1
nsppol = 1 nsym = 24 n1xccc = 2501 ntypat = 2
occopt = 1 xclevel = 1
- mband = 4 mffmem = 1 mkmem = 28
mpw = 174 nfft = 4096 nkpt = 28
================================================================================
P This job should need less than 2.843 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.299 Mbytes ; DEN or POT disk file : 0.033 Mbytes.
================================================================================
DATASET 2 : space group F-4 3 m (#216); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 2.
intxc = 0 ionmov = 0 iscf = -2 lmnmax = 6
lnmax = 6 mgfft = 16 mpssoang = 3 mqgrid = 3001
natom = 2 nloc_mem = 1 nspden = 1 nspinor = 1
nsppol = 1 nsym = 24 n1xccc = 2501 ntypat = 2
occopt = 1 xclevel = 1
- mband = 4 mffmem = 1 mkmem = 432
mpw = 174 nfft = 4096 nkpt = 432
================================================================================
P This job should need less than 7.684 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 4.590 Mbytes ; DEN or POT disk file : 0.033 Mbytes.
================================================================================
DATASET 3 : space group F-4 3 m (#216); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 3 (RF).
intxc = 0 iscf = 7 lmnmax = 6 lnmax = 6
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 2
nloc_mem = 1 nspden = 1 nspinor = 1 nsppol = 1
nsym = 24 n1xccc = 2501 ntypat = 2 occopt = 1
xclevel = 1
- mband = 4 mffmem = 1 mkmem = 432
- mkqmem = 432 mk1mem = 432 mpw = 174
nfft = 4096 nkpt = 432
================================================================================
P This job should need less than 17.803 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 4.590 Mbytes ; DEN or POT disk file : 0.033 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 7.2728565836E+00 7.2728565836E+00 7.2728565836E+00 Bohr
amu 3.09737620E+01 2.69815390E+01
berryopt1 0
berryopt2 -2
berryopt3 0
dilatmx 1.05000000E+00
ecut 5.00000000E+00 Hartree
ecutsm 5.00000000E-01 Hartree
- fftalg 512
getddk1 0
getddk2 0
getddk3 2
getden1 0
getden2 1
getden3 0
getwfk1 0
getwfk2 1
getwfk3 2
iscf1 7
iscf2 -2
iscf3 7
ixc -1012
jdtset 1 2 3
kpt1 -8.33333333E-02 -1.66666667E-01 0.00000000E+00
-8.33333333E-02 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -2.50000000E-01 0.00000000E+00
-8.33333333E-02 -2.50000000E-01 8.33333333E-02
-8.33333333E-02 5.00000000E-01 0.00000000E+00
-1.66666667E-01 -4.16666667E-01 0.00000000E+00
-8.33333333E-02 -4.16666667E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -3.33333333E-01 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 1.66666667E-01
-8.33333333E-02 3.33333333E-01 0.00000000E+00
-1.66666667E-01 4.16666667E-01 0.00000000E+00
-2.50000000E-01 5.00000000E-01 0.00000000E+00
-1.66666667E-01 5.00000000E-01 8.33333333E-02
-3.33333333E-01 -4.16666667E-01 0.00000000E+00
-2.50000000E-01 -4.16666667E-01 8.33333333E-02
-1.66666667E-01 -4.16666667E-01 1.66666667E-01
-8.33333333E-02 -4.16666667E-01 2.50000000E-01
-8.33333333E-02 1.66666667E-01 0.00000000E+00
-1.66666667E-01 2.50000000E-01 0.00000000E+00
-2.50000000E-01 3.33333333E-01 0.00000000E+00
-3.33333333E-01 4.16666667E-01 0.00000000E+00
-4.16666667E-01 5.00000000E-01 0.00000000E+00
-3.33333333E-01 5.00000000E-01 8.33333333E-02
-2.50000000E-01 5.00000000E-01 1.66666667E-01
-8.33333333E-02 0.00000000E+00 0.00000000E+00
-2.50000000E-01 0.00000000E+00 0.00000000E+00
-4.16666667E-01 0.00000000E+00 0.00000000E+00
kpt2 -8.33333333E-02 -1.66666667E-01 0.00000000E+00
-1.66666667E-01 -8.33333333E-02 0.00000000E+00
-8.33333333E-02 -8.33333333E-02 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -2.50000000E-01 0.00000000E+00
-8.33333333E-02 -2.50000000E-01 8.33333333E-02
-2.50000000E-01 -1.66666667E-01 0.00000000E+00
-1.66666667E-01 -1.66666667E-01 8.33333333E-02
-8.33333333E-02 -1.66666667E-01 1.66666667E-01
-3.33333333E-01 -8.33333333E-02 0.00000000E+00
-2.50000000E-01 -8.33333333E-02 8.33333333E-02
-1.66666667E-01 -8.33333333E-02 1.66666667E-01
-8.33333333E-02 -8.33333333E-02 2.50000000E-01
-8.33333333E-02 5.00000000E-01 0.00000000E+00
-1.66666667E-01 -4.16666667E-01 0.00000000E+00
-8.33333333E-02 -4.16666667E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -3.33333333E-01 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 1.66666667E-01
-3.33333333E-01 -2.50000000E-01 0.00000000E+00
-2.50000000E-01 -2.50000000E-01 8.33333333E-02
-1.66666667E-01 -2.50000000E-01 1.66666667E-01
-8.33333333E-02 -2.50000000E-01 2.50000000E-01
-4.16666667E-01 -1.66666667E-01 0.00000000E+00
-3.33333333E-01 -1.66666667E-01 8.33333333E-02
-2.50000000E-01 -1.66666667E-01 1.66666667E-01
-1.66666667E-01 -1.66666667E-01 2.50000000E-01
-8.33333333E-02 -1.66666667E-01 3.33333333E-01
5.00000000E-01 -8.33333333E-02 0.00000000E+00
-4.16666667E-01 -8.33333333E-02 8.33333333E-02
-3.33333333E-01 -8.33333333E-02 1.66666667E-01
-2.50000000E-01 -8.33333333E-02 2.50000000E-01
-1.66666667E-01 -8.33333333E-02 3.33333333E-01
-8.33333333E-02 -8.33333333E-02 4.16666667E-01
-8.33333333E-02 3.33333333E-01 0.00000000E+00
-1.66666667E-01 4.16666667E-01 0.00000000E+00
-8.33333333E-02 4.16666667E-01 8.33333333E-02
-2.50000000E-01 5.00000000E-01 0.00000000E+00
-1.66666667E-01 5.00000000E-01 8.33333333E-02
-8.33333333E-02 5.00000000E-01 1.66666667E-01
-3.33333333E-01 -4.16666667E-01 0.00000000E+00
-2.50000000E-01 -4.16666667E-01 8.33333333E-02
-1.66666667E-01 -4.16666667E-01 1.66666667E-01
-8.33333333E-02 -4.16666667E-01 2.50000000E-01
-4.16666667E-01 -3.33333333E-01 0.00000000E+00
-3.33333333E-01 -3.33333333E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 1.66666667E-01
-1.66666667E-01 -3.33333333E-01 2.50000000E-01
-8.33333333E-02 -3.33333333E-01 3.33333333E-01
5.00000000E-01 -2.50000000E-01 0.00000000E+00
kpt3 -8.33333333E-02 -1.66666667E-01 0.00000000E+00
-1.66666667E-01 -8.33333333E-02 0.00000000E+00
-8.33333333E-02 -8.33333333E-02 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -2.50000000E-01 0.00000000E+00
-8.33333333E-02 -2.50000000E-01 8.33333333E-02
-2.50000000E-01 -1.66666667E-01 0.00000000E+00
-1.66666667E-01 -1.66666667E-01 8.33333333E-02
-8.33333333E-02 -1.66666667E-01 1.66666667E-01
-3.33333333E-01 -8.33333333E-02 0.00000000E+00
-2.50000000E-01 -8.33333333E-02 8.33333333E-02
-1.66666667E-01 -8.33333333E-02 1.66666667E-01
-8.33333333E-02 -8.33333333E-02 2.50000000E-01
-8.33333333E-02 5.00000000E-01 0.00000000E+00
-1.66666667E-01 -4.16666667E-01 0.00000000E+00
-8.33333333E-02 -4.16666667E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -3.33333333E-01 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 1.66666667E-01
-3.33333333E-01 -2.50000000E-01 0.00000000E+00
-2.50000000E-01 -2.50000000E-01 8.33333333E-02
-1.66666667E-01 -2.50000000E-01 1.66666667E-01
-8.33333333E-02 -2.50000000E-01 2.50000000E-01
-4.16666667E-01 -1.66666667E-01 0.00000000E+00
-3.33333333E-01 -1.66666667E-01 8.33333333E-02
-2.50000000E-01 -1.66666667E-01 1.66666667E-01
-1.66666667E-01 -1.66666667E-01 2.50000000E-01
-8.33333333E-02 -1.66666667E-01 3.33333333E-01
5.00000000E-01 -8.33333333E-02 0.00000000E+00
-4.16666667E-01 -8.33333333E-02 8.33333333E-02
-3.33333333E-01 -8.33333333E-02 1.66666667E-01
-2.50000000E-01 -8.33333333E-02 2.50000000E-01
-1.66666667E-01 -8.33333333E-02 3.33333333E-01
-8.33333333E-02 -8.33333333E-02 4.16666667E-01
-8.33333333E-02 3.33333333E-01 0.00000000E+00
-1.66666667E-01 4.16666667E-01 0.00000000E+00
-8.33333333E-02 4.16666667E-01 8.33333333E-02
-2.50000000E-01 5.00000000E-01 0.00000000E+00
-1.66666667E-01 5.00000000E-01 8.33333333E-02
-8.33333333E-02 5.00000000E-01 1.66666667E-01
-3.33333333E-01 -4.16666667E-01 0.00000000E+00
-2.50000000E-01 -4.16666667E-01 8.33333333E-02
-1.66666667E-01 -4.16666667E-01 1.66666667E-01
-8.33333333E-02 -4.16666667E-01 2.50000000E-01
-4.16666667E-01 -3.33333333E-01 0.00000000E+00
-3.33333333E-01 -3.33333333E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 1.66666667E-01
-1.66666667E-01 -3.33333333E-01 2.50000000E-01
-8.33333333E-02 -3.33333333E-01 3.33333333E-01
5.00000000E-01 -2.50000000E-01 0.00000000E+00
outvar_i_n : Printing only first 50 k-points.
kptopt1 1
kptopt2 2
kptopt3 2
kptrlatt 6 -6 6 -6 6 6 -6 -6 6
kptrlen 6.17122345E+01
P mkmem1 28
P mkmem2 432
P mkmem3 432
P mkqmem1 28
P mkqmem2 432
P mkqmem3 432
P mk1mem1 28
P mk1mem2 432
P mk1mem3 432
natom 2
nband1 4
nband2 4
nband3 4
nbdbuf1 0
nbdbuf2 2
nbdbuf3 0
ndtset 3
ngfft 16 16 16
nkpt1 28
nkpt2 432
nkpt3 432
nstep1 8
nstep2 30
nstep3 8
nsym 24
ntypat 2
occ1 2.000000 2.000000 2.000000 2.000000
occ3 2.000000 2.000000 2.000000 2.000000
optdriver1 0
optdriver2 0
optdriver3 1
prtden1 1
prtden2 0
prtden3 0
prteig 0
prtpot1 0
prtpot2 0
prtpot3 1
prtwf1 1
prtwf2 1
prtwf3 0
rfelfd1 0
rfelfd2 0
rfelfd3 3
rfphon1 0
rfphon2 0
rfphon3 1
rfstrs1 0
rfstrs2 0
rfstrs3 3
rprim 0.0000000000E+00 7.0710678119E-01 7.0710678119E-01
7.0710678119E-01 0.0000000000E+00 7.0710678119E-01
7.0710678119E-01 7.0710678119E-01 0.0000000000E+00
shiftk 5.00000000E-01 5.00000000E-01 5.00000000E-01
spgroup 216
symrel 1 0 0 0 1 0 0 0 1 0 -1 1 0 -1 0 1 -1 0
-1 0 0 -1 0 1 -1 1 0 0 1 -1 1 0 -1 0 0 -1
-1 0 0 -1 1 0 -1 0 1 0 -1 1 1 -1 0 0 -1 0
1 0 0 0 0 1 0 1 0 0 1 -1 0 0 -1 1 0 -1
-1 0 1 -1 1 0 -1 0 0 0 -1 0 1 -1 0 0 -1 1
1 0 -1 0 0 -1 0 1 -1 0 1 0 0 0 1 1 0 0
1 0 -1 0 1 -1 0 0 -1 0 -1 0 0 -1 1 1 -1 0
-1 0 1 -1 0 0 -1 1 0 0 1 0 1 0 0 0 0 1
0 0 -1 0 1 -1 1 0 -1 1 -1 0 0 -1 1 0 -1 0
0 0 1 1 0 0 0 1 0 -1 1 0 -1 0 0 -1 0 1
0 0 1 0 1 0 1 0 0 1 -1 0 0 -1 0 0 -1 1
0 0 -1 1 0 -1 0 1 -1 -1 1 0 -1 0 1 -1 0 0
tolvrs1 1.00000000E-18
tolvrs2 0.00000000E+00
tolvrs3 1.00000000E-12
tolwfr1 0.00000000E+00
tolwfr2 1.00000000E-22
tolwfr3 0.00000000E+00
typat 1 2
wtk1 0.02778 0.02778 0.02778 0.05556 0.02778 0.02778
0.05556 0.02778 0.05556 0.05556 0.02778 0.02778
0.02778 0.05556 0.02778 0.05556 0.05556 0.05556
0.02778 0.02778 0.02778 0.02778 0.02778 0.05556
0.05556 0.00926 0.00926 0.00926
wtk2 0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231
wtk3 0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231
outvars : Printing only first 50 k-points.
xangst 1.3606961663E+00 1.3606961663E+00 1.3606961663E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
xcart 2.5713431044E+00 2.5713431044E+00 2.5713431044E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
xred 2.5000000000E-01 2.5000000000E-01 2.5000000000E-01
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
znucl 15.00000 13.00000
================================================================================
chkinp: Checking input parameters for consistency, jdtset= 1.
chkinp: Checking input parameters for consistency, jdtset= 2.
chkinp: Checking input parameters for consistency, jdtset= 3.
================================================================================
== DATASET 1 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 1, }
dimensions: {natom: 2, nkpt: 28, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 174, }
cutoff_energies: {ecut: 5.0, pawecutdg: -1.0, }
electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
meta: {optdriver: 0, ionmov: 0, optcell: 0, iscf: 7, paral_kgb: 0, }
...
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 5.1426862 5.1426862 G(1)= -0.0972255 0.0972255 0.0972255
R(2)= 5.1426862 0.0000000 5.1426862 G(2)= 0.0972255 -0.0972255 0.0972255
R(3)= 5.1426862 5.1426862 0.0000000 G(3)= 0.0972255 0.0972255 -0.0972255
Unit cell volume ucvol= 2.7201952E+02 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)= 5.513 => boxcut(ratio)= 2.08150
--- Pseudopotential description ------------------------------------------------
- pspini: atom type 1 psp file is /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/Psdj_nc_sr_04_pw_std_psp8/P.psp8
- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/Psdj_nc_sr_04_pw_std_psp8/P.psp8
- P ONCVPSP-3.3.0 r_core= 1.46089 1.55067 1.70594
- 15.00000 5.00000 171102 znucl, zion, pspdat
8 -1012 2 4 600 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
5.99000000000000 5.00000000000000 0.00000000000000 rchrg,fchrg,qchrg
nproj 2 2 2
extension_switch 1
pspatm : epsatm= 7.03163490
--- l ekb(1:nproj) -->
0 6.795192 1.078292
1 3.452929 0.907117
2 -3.024864 -0.802189
pspatm: atomic psp has been read and splines computed
- pspini: atom type 2 psp file is /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/Psdj_nc_sr_04_pw_std_psp8/Al.psp8
- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/Psdj_nc_sr_04_pw_std_psp8/Al.psp8
- Al ONCVPSP-3.3.0 r_core= 1.76802 1.76802 1.70587
- 13.00000 3.00000 171102 znucl, zion, pspdat
8 -1012 2 4 600 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
5.99000000000000 5.00000000000000 0.00000000000000 rchrg,fchrg,qchrg
nproj 2 2 2
extension_switch 1
pspatm : epsatm= 0.57439192
--- l ekb(1:nproj) -->
0 5.725870 0.726131
1 6.190420 0.914022
2 -4.229503 -0.925599
pspatm: atomic psp has been read and splines computed
6.08482146E+01 ecore*ucvol(ha*bohr**3)
--------------------------------------------------------------------------------
_setup2: Arith. and geom. avg. npw (full set) are 167.843 167.817
================================================================================
--- !BeginCycle
iteration_state: {dtset: 1, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-18, }
...
iter Etot(hartree) deltaE(h) residm vres2
ETOT 1 -9.2741672565630 -9.274E+00 1.231E-02 3.673E+00
ETOT 2 -9.2840973975341 -9.930E-03 1.956E-05 1.584E-01
ETOT 3 -9.2844340680046 -3.367E-04 2.699E-06 4.366E-03
ETOT 4 -9.2844384858110 -4.418E-06 1.995E-08 1.255E-04
ETOT 5 -9.2844385675779 -8.177E-08 3.534E-10 1.028E-06
ETOT 6 -9.2844385681275 -5.496E-10 2.392E-12 3.274E-08
ETOT 7 -9.2844385681497 -2.219E-11 1.120E-13 4.768E-10
ETOT 8 -9.2844385681503 -6.448E-13 3.472E-15 1.668E-12
Cartesian components of stress tensor (hartree/bohr^3)
sigma(1 1)= 2.09491882E-10 sigma(3 2)= 0.00000000E+00
sigma(2 2)= 2.09491882E-10 sigma(3 1)= 0.00000000E+00
sigma(3 3)= 2.09491882E-10 sigma(2 1)= 0.00000000E+00
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 1.668E-12 exceeds tolvrs= 1.000E-18
--- !ResultsGS
iteration_state: {dtset: 1, }
comment : Summary of ground state results
lattice_vectors:
- [ 0.0000000, 5.1426862, 5.1426862, ]
- [ 5.1426862, 0.0000000, 5.1426862, ]
- [ 5.1426862, 5.1426862, 0.0000000, ]
lattice_lengths: [ 7.27286, 7.27286, 7.27286, ]
lattice_angles: [ 60.000, 60.000, 60.000, ] # degrees, (23, 13, 12)
lattice_volume: 2.7201952E+02
convergence: {deltae: -6.448E-13, res2: 1.668E-12, residm: 3.472E-15, diffor: null, }
etotal : -9.28443857E+00
entropy : 0.00000000E+00
fermie : 1.47753464E-01
cartesian_stress_tensor: # hartree/bohr^3
- [ 2.09491882E-10, 0.00000000E+00, 0.00000000E+00, ]
- [ 0.00000000E+00, 2.09491882E-10, 0.00000000E+00, ]
- [ 0.00000000E+00, 0.00000000E+00, 2.09491882E-10, ]
pressure_GPa: -6.1635E-06
xred :
- [ 2.5000E-01, 2.5000E-01, 2.5000E-01, P]
- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Al]
cartesian_forces: # hartree/bohr
- [ -0.00000000E+00, -0.00000000E+00, -0.00000000E+00, ]
- [ -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 density in atomic spheres:
------------------------------------------------
Atom Sphere_radius Integrated_density
1 2.00000 2.91222120
2 2.00000 0.97937928
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 16.346E-16; max= 34.722E-16
reduced coordinates (array xred) for 2 atoms
0.250000000000 0.250000000000 0.250000000000
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
2 0.000000000000 0.000000000000 0.000000000000
cartesian coordinates (angstrom) at end:
1 1.36069616633626 1.36069616633626 1.36069616633626
2 0.00000000000000 0.00000000000000 0.00000000000000
cartesian forces (hartree/bohr) at end:
1 -0.00000000000000 -0.00000000000000 -0.00000000000000
2 -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
2 -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= 7.272856583600 7.272856583600 7.272856583600 bohr
= 3.848629945385 3.848629945385 3.848629945385 angstroms
Fermi (or HOMO) energy (hartree) = 0.14775 Average Vxc (hartree)= -0.34161
Eigenvalues (hartree) for nkpt= 28 k points:
kpt# 1, nband= 4, wtk= 0.02778, kpt= -0.0833 -0.1667 0.0000 (reduced coord)
-0.24355 0.09966 0.13340 0.13823
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 : 3.34100500982041E+00
hartree : 8.79639261038836E-01
xc : -3.16747630870939E+00
Ewald energy : -8.74753884992007E+00
psp_core : 2.23690616503296E-01
local_psp : -3.33508360180407E+00
non_local_psp : 1.52132530492065E+00
total_energy : -9.28443856815034E+00
total_energy_eV : -2.52642421802528E+02
band_energy : -4.47113294174973E-02
...
Cartesian components of stress tensor (hartree/bohr^3)
sigma(1 1)= 2.09491882E-10 sigma(3 2)= 0.00000000E+00
sigma(2 2)= 2.09491882E-10 sigma(3 1)= 0.00000000E+00
sigma(3 3)= 2.09491882E-10 sigma(2 1)= 0.00000000E+00
-Cartesian components of stress tensor (GPa) [Pressure= -6.1635E-06 GPa]
- sigma(1 1)= 6.16346292E-06 sigma(3 2)= 0.00000000E+00
- sigma(2 2)= 6.16346292E-06 sigma(3 1)= 0.00000000E+00
- sigma(3 3)= 6.16346292E-06 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: 2, nkpt: 432, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 174, }
cutoff_energies: {ecut: 5.0, pawecutdg: -1.0, }
electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
meta: {optdriver: 0, ionmov: 0, optcell: 0, iscf: -2, paral_kgb: 0, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
mkfilename : getden/=0, take file _DEN from output of DATASET 1.
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 5.1426862 5.1426862 G(1)= -0.0972255 0.0972255 0.0972255
R(2)= 5.1426862 0.0000000 5.1426862 G(2)= 0.0972255 -0.0972255 0.0972255
R(3)= 5.1426862 5.1426862 0.0000000 G(3)= 0.0972255 0.0972255 -0.0972255
Unit cell volume ucvol= 2.7201952E+02 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)= 5.513 => boxcut(ratio)= 2.08150
--------------------------------------------------------------------------------
-inwffil : will read wavefunctions from disk file tpolarization_2o_DS1_WFK
initberry: for direction 1, nkstr = 6, nstr = 144
initberry: for direction 2, nkstr = 6, nstr = 144
initberry: for direction 3, nkstr = 6, nstr = 144
================================================================================
Non-SCF case, kpt 1 ( -0.08333 -0.16667 0.00000), residuals and eigenvalues=
1.96E-23 4.63E-23 6.08E-23 5.08E-22
-2.4355E-01 9.9660E-02 1.3340E-01 1.3823E-01
prteigrs : prtvol=0 or 1, do not print more k-points.
Computing the polarization (Berry phase) for reciprocal vector:
0.16667 0.00000 0.00000 (in reduced coordinates)
-0.01620 0.01620 0.01620 (in cartesian coordinates - atomic units)
Number of strings: 144
Number of k points in string: 6
Computing the ddk (Berry phase) for reciprocal vector:
0.16667 0.00000 0.00000 (in reduced coordinates)
-0.01620 0.01620 0.01620 (in cartesian coordinates - atomic units)
Mean square residual over all n,k,spin= 00.000E+00; max= 00.000E+00
Computing the polarization (Berry phase) for reciprocal vector:
0.00000 0.16667 0.00000 (in reduced coordinates)
0.01620 -0.01620 0.01620 (in cartesian coordinates - atomic units)
Number of strings: 144
Number of k points in string: 6
Computing the ddk (Berry phase) for reciprocal vector:
0.00000 0.16667 0.00000 (in reduced coordinates)
0.01620 -0.01620 0.01620 (in cartesian coordinates - atomic units)
Mean square residual over all n,k,spin= 00.000E+00; max= 00.000E+00
Computing the polarization (Berry phase) for reciprocal vector:
0.00000 0.00000 0.16667 (in reduced coordinates)
0.01620 0.01620 -0.01620 (in cartesian coordinates - atomic units)
Number of strings: 144
Number of k points in string: 6
Computing the ddk (Berry phase) for reciprocal vector:
0.00000 0.00000 0.16667 (in reduced coordinates)
0.01620 0.01620 -0.01620 (in cartesian coordinates - atomic units)
Mean square residual over all n,k,spin= 00.000E+00; max= 00.000E+00
Polarization in cartesian coordinates (a.u.):
(the sum of the electronic and ionic Berry phase has been folded into [-1, 1])
Electronic berry phase: 0.000000000E+00 0.000000000E+00 0.000000000E+00
Ionic: 0.000000000E+00 0.000000000E+00 0.000000000E+00
Total: 0.000000000E+00 0.000000000E+00 0.000000000E+00
Polarization in cartesian coordinates (C/m^2):
(the sum of the electronic and ionic Berry phase has been folded into [-1, 1])
Electronic berry phase: 0.000000000E+00 0.000000000E+00 0.000000000E+00
Ionic: 0.000000000E+00 0.000000000E+00 0.000000000E+00
Total: 0.000000000E+00 0.000000000E+00 0.000000000E+00
--- !ResultsGS
iteration_state: {dtset: 2, }
comment : Summary of ground state results
lattice_vectors:
- [ 0.0000000, 5.1426862, 5.1426862, ]
- [ 5.1426862, 0.0000000, 5.1426862, ]
- [ 5.1426862, 5.1426862, 0.0000000, ]
lattice_lengths: [ 7.27286, 7.27286, 7.27286, ]
lattice_angles: [ 60.000, 60.000, 60.000, ] # degrees, (23, 13, 12)
lattice_volume: 2.7201952E+02
convergence: {deltae: 0.000E+00, res2: 0.000E+00, residm: 9.629E-23, diffor: 0.000E+00, }
etotal : -9.28443857E+00
entropy : 0.00000000E+00
fermie : 1.47753464E-01
cartesian_stress_tensor: null
pressure_GPa: null
xred :
- [ 2.5000E-01, 2.5000E-01, 2.5000E-01, P]
- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Al]
cartesian_forces: null
force_length_stats: {min: null, max: null, mean: null, }
...
Integrated electronic density in atomic spheres:
------------------------------------------------
Atom Sphere_radius Integrated_density
1 2.00000 2.91222120
2 2.00000 0.97937928
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 39.721E-24; max= 96.291E-24
reduced coordinates (array xred) for 2 atoms
0.250000000000 0.250000000000 0.250000000000
0.000000000000 0.000000000000 0.000000000000
cartesian coordinates (angstrom) at end:
1 1.36069616633626 1.36069616633626 1.36069616633626
2 0.00000000000000 0.00000000000000 0.00000000000000
length scales= 7.272856583600 7.272856583600 7.272856583600 bohr
= 3.848629945385 3.848629945385 3.848629945385 angstroms
Eigenvalues (hartree) for nkpt= 432 k points:
kpt# 1, nband= 4, wtk= 0.00231, kpt= -0.0833 -0.1667 0.0000 (reduced coord)
-0.24355 0.09966 0.13340 0.13823
prteigrs : prtvol=0 or 1, do not print more k-points.
================================================================================
== DATASET 3 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 3, }
dimensions: {natom: 2, nkpt: 432, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 174, }
cutoff_energies: {ecut: 5.0, pawecutdg: -1.0, }
electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
meta: {optdriver: 1, rfelfd: 3, rfphon: 1, rfstrs: 3, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 2.
mkfilename : getddk/=0, take file _1WF from output of DATASET 2.
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 5.1426862 5.1426862 G(1)= -0.0972255 0.0972255 0.0972255
R(2)= 5.1426862 0.0000000 5.1426862 G(2)= 0.0972255 -0.0972255 0.0972255
R(3)= 5.1426862 5.1426862 0.0000000 G(3)= 0.0972255 0.0972255 -0.0972255
Unit cell volume ucvol= 2.7201952E+02 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)= 5.513 => boxcut(ratio)= 2.08150
--------------------------------------------------------------------------------
symkchk : k-point set has full space-group symmetry.
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 1 ipert= 1
2) idir= 1 ipert= 2
3) idir= 1 ipert= 4
4) idir= 1 ipert= 5
5) idir= 2 ipert= 5
6) idir= 3 ipert= 5
7) idir= 1 ipert= 6
8) idir= 2 ipert= 6
9) idir= 3 ipert= 6
================================================================================
The perturbation idir= 2 ipert= 1 is
symmetric of a previously calculated perturbation.
So, its SCF calculation is not needed.
The perturbation idir= 3 ipert= 1 is
symmetric of a previously calculated perturbation.
So, its SCF calculation is not needed.
The perturbation idir= 2 ipert= 2 is
symmetric of a previously calculated perturbation.
So, its SCF calculation is not needed.
The perturbation idir= 3 ipert= 2 is
symmetric of a previously calculated perturbation.
So, its SCF calculation is not needed.
The perturbation idir= 2 ipert= 4 is
symmetric of a previously calculated perturbation.
So, its SCF calculation is not needed.
The perturbation idir= 3 ipert= 4 is
symmetric of a previously calculated perturbation.
So, its SCF calculation is not needed.
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 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 234 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 5.9819217360381 -1.562E+02 3.241E-01 9.326E+01
ETOT 2 5.6097918088114 -3.721E-01 1.253E-03 1.213E+00
ETOT 3 5.6037858985470 -6.006E-03 2.675E-05 1.095E-01
ETOT 4 5.6035167184823 -2.692E-04 5.105E-07 2.544E-03
ETOT 5 5.6035119067435 -4.812E-06 1.054E-08 1.783E-05
ETOT 6 5.6035118704983 -3.625E-08 1.461E-10 4.093E-07
ETOT 7 5.6035118698680 -6.304E-10 1.803E-12 1.069E-08
ETOT 8 5.6035118698446 -2.333E-11 3.894E-14 2.870E-10
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 2.870E-10 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 80.418E-16; max= 38.938E-15
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 1.71679181E+02 eigvalue= -8.64074620E+00 local= -1.30494874E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -1.00729546E+02 Hartree= 4.20402984E+01 xc= -1.44739669E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 9.64749406E+01 enl1= -2.12440119E+02
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -1.56584832E+02
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 4.27717848E+01 fr.nonlo= 1.10588066E+02 Ewald= 1.22177108E+01
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -1.72960963E+01 frxc 2 = 1.39068791E+01
Resulting in :
2DEtotal= 0.5603511870E+01 Ha. Also 2DEtotal= 0.152479312454E+03 eV
(2DErelax= -1.5658483210E+02 Ha. 2DEnonrelax= 1.6218834397E+02 Ha)
( non-var. 2DEtotal : 5.6035117682E+00 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Perturbation : displacement of atom 2 along direction 1
Found 2 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 234 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 5.6476193513465 -2.497E+01 3.105E-02 1.153E+01
ETOT 2 5.6047506528418 -4.287E-02 2.805E-04 1.729E-01
ETOT 3 5.6042324568496 -5.182E-04 3.424E-06 5.740E-03
ETOT 4 5.6042191253671 -1.333E-05 5.005E-08 1.588E-04
ETOT 5 5.6042187944954 -3.309E-07 8.827E-10 1.169E-06
ETOT 6 5.6042187917949 -2.700E-09 1.521E-11 2.047E-08
ETOT 7 5.6042187917429 -5.205E-11 1.485E-13 3.569E-10
ETOT 8 5.6042187917422 -6.395E-13 3.169E-15 9.477E-12
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 9.477E-12 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 45.334E-17; max= 31.685E-16
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.34536647E+01 eigvalue= -4.05140335E-01 local= -1.57197505E+01
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = 4.43872950E+00 Hartree= 3.38007917E+00 xc= -1.62178142E+00
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 1.59240791E+01 enl1= -5.44610312E+01
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.50111510E+01
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= -1.52983623E+01 fr.nonlo= 3.49191663E+01 Ewald= 1.22177108E+01
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -5.14901927E+00 frxc 2 = 3.92587424E+00
Resulting in :
2DEtotal= 0.5604218792E+01 Ha. Also 2DEtotal= 0.152498548778E+03 eV
(2DErelax= -2.5011151001E+01 Ha. 2DEnonrelax= 3.0615369792E+01 Ha)
( non-var. 2DEtotal : 5.6042189570E+00 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Perturbation : homogeneous electric field along direction 1
The set of symmetries contains only one element for this perturbation.
symkpt : not enough symmetry to change the number of k points.
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
- dfpt_looppert: read the DDK wavefunctions from file: tpolarization_2o_DS2_1WF7
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 -121.62952632510 -1.216E+02 1.207E+00 2.675E+03
ETOT 2 -132.23434290027 -1.060E+01 3.173E-02 2.595E+01
ETOT 3 -132.37736333905 -1.430E-01 6.325E-04 1.339E+00
ETOT 4 -132.38078294131 -3.420E-03 6.856E-06 2.857E-02
ETOT 5 -132.38083549446 -5.255E-05 1.168E-07 4.693E-04
ETOT 6 -132.38083677524 -1.281E-06 3.117E-09 2.046E-05
ETOT 7 -132.38083682523 -5.000E-08 1.041E-10 3.668E-07
ETOT 8 -132.38083682587 -6.357E-10 1.079E-12 5.277E-09
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 5.277E-09 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 31.957E-14; max= 10.795E-13
Seven components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 3.43539753E+02 eigvalue= -5.96887804E+01 local= -2.57555778E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
dotwf= -2.64761649E+02 Hartree= 2.05628325E+01 xc= -1.12136309E+01
7,8,9: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 9.67364161E+01 enl1= 0.00000000E+00
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -1.32380837E+02
No Ewald or frozen-wf contrib.: the relaxation energy is the total one
2DEtotal= -0.1323808368E+03 Ha. Also 2DEtotal= -0.360226576658E+04 eV
( non-var. 2DEtotal : -1.3238082437E+02 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Found 8 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 63 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 2.1466730921679 -1.983E+01 9.660E-01 2.132E+02
ETOT 2 1.3604905588292 -7.862E-01 1.254E-03 1.117E+01
ETOT 3 1.3244509970749 -3.604E-02 4.657E-05 3.715E-01
ETOT 4 1.3236184956762 -8.325E-04 1.294E-06 4.865E-03
ETOT 5 1.3236107804648 -7.715E-06 1.617E-08 7.303E-05
ETOT 6 1.3236106028851 -1.776E-07 1.766E-10 9.666E-07
ETOT 7 1.3236106002450 -2.640E-09 4.188E-12 2.920E-08
ETOT 8 1.3236106001844 -6.064E-11 8.241E-14 5.357E-10
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 5.357E-10 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 18.870E-15; max= 82.408E-15
Seventeen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.23378663E+01 eigvalue= -2.05283585E-01 local= -3.55057557E+00
4,5,6,7: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = 5.59187957E-01 Hartree= 1.13632184E+00 xc= -4.89367751E-01
kin1= -3.75034830E+01
8,9,10: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 1.34195643E+00 enl1= -4.27873329E+00
1-10 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.06521106E+01
11,12,13 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.hart= -4.64499017E-01 fr.kin= 2.02424027E+01 fr.loc= 3.10467979E+00
14,15,16 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.nonl= 2.55333690E+00 fr.xc= -3.37835985E-01 Ewald= -3.34605377E+00
17 Non-relaxation contributions : pseudopotential core energy
pspcore= 2.23690617E-01
Resulting in :
2DEtotal= 0.1323610600E+01 Ha. Also 2DEtotal= 0.360172761228E+02 eV
(2DErelax= -2.0652110605E+01 Ha. 2DEnonrelax= 2.1975721205E+01 Ha)
( non-var. 2DEtotal : 1.3236107163E+00 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Found 8 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 63 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 2.1464989620897 -1.983E+01 9.660E-01 2.132E+02
ETOT 2 1.3604702636673 -7.860E-01 1.254E-03 1.116E+01
ETOT 3 1.3244511472886 -3.602E-02 4.656E-05 3.715E-01
ETOT 4 1.3236185107520 -8.326E-04 1.295E-06 4.864E-03
ETOT 5 1.3236107961617 -7.715E-06 1.619E-08 7.308E-05
ETOT 6 1.3236106184715 -1.777E-07 1.765E-10 9.653E-07
ETOT 7 1.3236106158382 -2.633E-09 4.181E-12 2.914E-08
ETOT 8 1.3236106157777 -6.056E-11 8.243E-14 5.341E-10
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 5.341E-10 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 18.836E-15; max= 82.429E-15
Seventeen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.23378663E+01 eigvalue= -2.05283585E-01 local= -3.55057557E+00
4,5,6,7: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = 5.59187956E-01 Hartree= 1.13632184E+00 xc= -4.89367750E-01
kin1= -3.75034829E+01
8,9,10: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 1.34195643E+00 enl1= -4.27873329E+00
1-10 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.06521106E+01
11,12,13 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.hart= -4.64499017E-01 fr.kin= 2.02424027E+01 fr.loc= 3.10467979E+00
14,15,16 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.nonl= 2.55333690E+00 fr.xc= -3.37835985E-01 Ewald= -3.34605377E+00
17 Non-relaxation contributions : pseudopotential core energy
pspcore= 2.23690617E-01
Resulting in :
2DEtotal= 0.1323610616E+01 Ha. Also 2DEtotal= 0.360172765471E+02 eV
(2DErelax= -2.0652110571E+01 Ha. 2DEnonrelax= 2.1975721187E+01 Ha)
( non-var. 2DEtotal : 1.3236107332E+00 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Found 8 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 63 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 2.1464889131017 -1.983E+01 9.660E-01 2.132E+02
ETOT 2 1.3604714341588 -7.860E-01 1.254E-03 1.116E+01
ETOT 3 1.3244512330362 -3.602E-02 4.656E-05 3.715E-01
ETOT 4 1.3236185231935 -8.327E-04 1.295E-06 4.864E-03
ETOT 5 1.3236108079077 -7.715E-06 1.620E-08 7.310E-05
ETOT 6 1.3236106302138 -1.777E-07 1.765E-10 9.632E-07
ETOT 7 1.3236106275937 -2.620E-09 4.165E-12 2.909E-08
ETOT 8 1.3236106275335 -6.014E-11 8.259E-14 5.342E-10
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 5.342E-10 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 18.654E-15; max= 82.594E-15
Seventeen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.23378662E+01 eigvalue= -2.05283585E-01 local= -3.55057557E+00
4,5,6,7: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = 5.59187956E-01 Hartree= 1.13632184E+00 xc= -4.89367750E-01
kin1= -3.75034828E+01
8,9,10: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 1.34195643E+00 enl1= -4.27873329E+00
1-10 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -2.06521105E+01
11,12,13 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.hart= -4.64499017E-01 fr.kin= 2.02424026E+01 fr.loc= 3.10467979E+00
14,15,16 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.nonl= 2.55333690E+00 fr.xc= -3.37835985E-01 Ewald= -3.34605377E+00
17 Non-relaxation contributions : pseudopotential core energy
pspcore= 2.23690617E-01
Resulting in :
2DEtotal= 0.1323610628E+01 Ha. Also 2DEtotal= 0.360172768670E+02 eV
(2DErelax= -2.0652110542E+01 Ha. 2DEnonrelax= 2.1975721169E+01 Ha)
( non-var. 2DEtotal : 1.3236107457E+00 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Found 4 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 126 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 1.5365103418205 -8.723E+00 3.303E-01 2.069E+02
ETOT 2 0.91849267791560 -6.180E-01 6.411E-04 4.874E+00
ETOT 3 0.90684887718722 -1.164E-02 2.524E-05 2.458E-01
ETOT 4 0.90635118510959 -4.977E-04 5.702E-07 6.164E-03
ETOT 5 0.90634026521035 -1.092E-05 2.079E-08 4.847E-05
ETOT 6 0.90634017400942 -9.120E-08 2.929E-10 4.349E-07
ETOT 7 0.90634017306717 -9.423E-10 2.671E-12 9.383E-09
ETOT 8 0.90634017303950 -2.766E-11 7.055E-14 8.758E-11
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 8.758E-11 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 14.887E-15; max= 70.553E-15
Seventeen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 1.00924101E+01 eigvalue= -1.77063817E-01 local= -1.79877062E+00
4,5,6,7: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -6.42729656E+00 Hartree= 2.99771670E+00 xc= -4.71092363E-01
kin1= -1.41452110E+01
8,9,10: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 3.56674056E-01 enl1= 2.19018535E-01
1-10 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -9.35361499E+00
11,12,13 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.hart= 8.56429419E-02 fr.kin= 7.60094711E+00 fr.loc= -7.60461472E-01
14,15,16 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.nonl= 2.20409429E-01 fr.xc= -1.75328756E-02 Ewald= 3.13095003E+00
17 Non-relaxation contributions : pseudopotential core energy
pspcore= 0.00000000E+00
Resulting in :
2DEtotal= 0.9063401730E+00 Ha. Also 2DEtotal= 0.246627703563E+02 eV
(2DErelax= -9.3536149863E+00 Ha. 2DEnonrelax= 1.0259955159E+01 Ha)
( non-var. 2DEtotal : 9.0634061506E-01 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Found 4 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 126 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 1.5366098384550 -8.723E+00 3.303E-01 2.069E+02
ETOT 2 0.91849706647513 -6.181E-01 6.411E-04 4.875E+00
ETOT 3 0.90684922759721 -1.165E-02 2.499E-05 2.460E-01
ETOT 4 0.90635118595258 -4.980E-04 5.705E-07 6.167E-03
ETOT 5 0.90634026326434 -1.092E-05 2.079E-08 4.846E-05
ETOT 6 0.90634017208071 -9.118E-08 2.929E-10 4.348E-07
ETOT 7 0.90634017113869 -9.420E-10 2.671E-12 9.385E-09
ETOT 8 0.90634017111108 -2.761E-11 6.662E-14 8.761E-11
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 8.761E-11 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 14.996E-15; max= 66.624E-15
Seventeen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 1.00924101E+01 eigvalue= -1.77063817E-01 local= -1.79877062E+00
4,5,6,7: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -6.42729656E+00 Hartree= 2.99771671E+00 xc= -4.71092363E-01
kin1= -1.41452110E+01
8,9,10: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 3.56674057E-01 enl1= 2.19018535E-01
1-10 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -9.35361499E+00
11,12,13 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.hart= 8.56429419E-02 fr.kin= 7.60094711E+00 fr.loc= -7.60461472E-01
14,15,16 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.nonl= 2.20409429E-01 fr.xc= -1.75328756E-02 Ewald= 3.13095003E+00
17 Non-relaxation contributions : pseudopotential core energy
pspcore= 0.00000000E+00
Resulting in :
2DEtotal= 0.9063401711E+00 Ha. Also 2DEtotal= 0.246627703038E+02 eV
(2DErelax= -9.3536149910E+00 Ha. 2DEnonrelax= 1.0259955162E+01 Ha)
( non-var. 2DEtotal : 9.0634061235E-01 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Found 4 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 126 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 8, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 1.5364475458195 -8.724E+00 3.303E-01 2.069E+02
ETOT 2 0.91848910569518 -6.180E-01 6.411E-04 4.874E+00
ETOT 3 0.90684844725666 -1.164E-02 2.547E-05 2.457E-01
ETOT 4 0.90635117116457 -4.973E-04 5.697E-07 6.158E-03
ETOT 5 0.90634026067298 -1.091E-05 2.079E-08 4.843E-05
ETOT 6 0.90634016953923 -9.113E-08 2.924E-10 4.349E-07
ETOT 7 0.90634016859757 -9.417E-10 2.674E-12 9.399E-09
ETOT 8 0.90634016856987 -2.770E-11 6.455E-14 8.770E-11
-open ddk wf file :tpolarization_2o_DS2_1WF7
-open ddk wf file :tpolarization_2o_DS2_1WF8
-open ddk wf file :tpolarization_2o_DS2_1WF9
scprqt: WARNING -
nstep= 8 was not enough SCF cycles to converge;
potential residual= 8.770E-11 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 14.896E-15; max= 64.549E-15
Seventeen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 1.00924101E+01 eigvalue= -1.77063817E-01 local= -1.79877062E+00
4,5,6,7: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -6.42729656E+00 Hartree= 2.99771670E+00 xc= -4.71092363E-01
kin1= -1.41452110E+01
8,9,10: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= 3.56674056E-01 enl1= 2.19018535E-01
1-10 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -9.35361500E+00
11,12,13 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.hart= 8.56429419E-02 fr.kin= 7.60094711E+00 fr.loc= -7.60461472E-01
14,15,16 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.nonl= 2.20409429E-01 fr.xc= -1.75328756E-02 Ewald= 3.13095003E+00
17 Non-relaxation contributions : pseudopotential core energy
pspcore= 0.00000000E+00
Resulting in :
2DEtotal= 0.9063401686E+00 Ha. Also 2DEtotal= 0.246627702347E+02 eV
(2DErelax= -9.3536149964E+00 Ha. 2DEnonrelax= 1.0259955165E+01 Ha)
( non-var. 2DEtotal : 9.0634061099E-01 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
The violation of the charge neutrality conditions
by the effective charges is as follows :
atom electric field
displacement direction
1 1 0.000065 0.000000
1 2 -0.000000 0.000000
1 3 0.000000 0.000000
2 1 -0.000000 0.000000
2 2 0.000065 0.000000
2 3 -0.000000 0.000000
3 1 0.000000 0.000000
3 2 0.000000 0.000000
3 3 0.000065 0.000000
Effective charge tensors after
imposition of the charge neutrality (if requested by user),
and eventual restriction to some part :
atom displacement
1 1 -2.254026E+00 -2.925658E-16 9.263883E-17
1 2 -2.925658E-16 -2.254026E+00 -9.941145E-17
1 3 2.925658E-16 2.925658E-16 -2.254026E+00
2 1 2.254026E+00 2.925658E-16 -9.263883E-17
2 2 2.925658E-16 2.254026E+00 9.941145E-17
2 3 -2.925658E-16 -2.925658E-16 2.254026E+00
Now, the imaginary part of the dynamical matrix is zeroed
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
cartesian coordinates for strain terms (1/ucvol factor
for elastic tensor components not included)
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 5.6035118961 0.0000000000
1 1 2 1 2.8017559481 0.0000000000
1 1 3 1 2.8017559481 0.0000000000
1 1 1 2 -5.6043281845 -0.0000000000
1 1 2 2 -2.8021640922 0.0000000000
1 1 3 2 -2.8021640922 0.0000000000
1 1 1 4 -45.5781849719 0.0000000000
1 1 2 4 -0.0000000000 0.0000000000
1 1 3 4 -0.0000000000 0.0000000000
1 1 1 5 -0.0000000000 0.0000000000
1 1 2 5 -0.0000000000 0.0000000000
1 1 3 5 -0.0000000000 0.0000000000
1 1 1 6 0.0000000000 0.0000000000
1 1 2 6 0.8892825795 0.0000000000
1 1 3 6 0.8892825762 0.0000000000
2 1 1 1 2.8017559481 0.0000000000
2 1 2 1 5.6035118961 0.0000000000
2 1 3 1 2.8017559481 0.0000000000
2 1 1 2 -2.8021640922 0.0000000000
2 1 2 2 -5.6043281845 -0.0000000000
2 1 3 2 -2.8021640922 -0.0000000000
2 1 1 4 0.0000000000 0.0000000000
2 1 2 4 -45.5781849719 0.0000000000
2 1 3 4 -0.0000000000 0.0000000000
2 1 1 5 0.0000000000 0.0000000000
2 1 2 5 0.0000000000 0.0000000000
2 1 3 5 -0.0000000000 0.0000000000
2 1 1 6 0.8892825779 0.0000000000
2 1 2 6 -0.0000000000 0.0000000000
2 1 3 6 0.8892825762 0.0000000000
3 1 1 1 2.8017559481 0.0000000000
3 1 2 1 2.8017559481 0.0000000000
3 1 3 1 5.6035118961 0.0000000000
3 1 1 2 -2.8021640922 0.0000000000
3 1 2 2 -2.8021640922 -0.0000000000
3 1 3 2 -5.6043281845 -0.0000000000
3 1 1 4 0.0000000000 0.0000000000
3 1 2 4 -0.0000000000 0.0000000000
3 1 3 4 -45.5781849719 0.0000000000
3 1 1 5 0.0000000000 0.0000000000
3 1 2 5 0.0000000000 0.0000000000
3 1 3 5 0.0000000000 0.0000000000
3 1 1 6 0.8892825779 0.0000000000
3 1 2 6 0.8892825795 0.0000000000
3 1 3 6 -0.0000000000 0.0000000000
1 2 1 1 -5.6043258334 0.0000000000
1 2 2 1 -2.8021629167 -0.0000000000
1 2 3 1 -2.8021629167 -0.0000000000
1 2 1 2 5.6042189585 0.0000000000
1 2 2 2 2.8021094793 0.0000000000
1 2 3 2 2.8021094793 0.0000000000
1 2 1 4 -4.6868870947 0.0000000000
1 2 2 4 0.0000000000 0.0000000000
1 2 3 4 0.0000000000 0.0000000000
1 2 1 5 0.0000000000 0.0000000000
1 2 2 5 0.0000000000 0.0000000000
1 2 3 5 0.0000000000 0.0000000000
1 2 1 6 -0.0000000000 0.0000000000
1 2 2 6 -0.8892553578 0.0000000000
1 2 3 6 -0.8892553594 0.0000000000
2 2 1 1 -2.8021629167 -0.0000000000
2 2 2 1 -5.6043258334 0.0000000000
2 2 3 1 -2.8021629167 0.0000000000
2 2 1 2 2.8021094793 0.0000000000
2 2 2 2 5.6042189585 0.0000000000
2 2 3 2 2.8021094793 0.0000000000
2 2 1 4 0.0000000000 0.0000000000
2 2 2 4 -4.6868870947 0.0000000000
2 2 3 4 0.0000000000 0.0000000000
2 2 1 5 -0.0000000000 0.0000000000
2 2 2 5 0.0000000000 0.0000000000
2 2 3 5 0.0000000000 0.0000000000
2 2 1 6 -0.8892553590 0.0000000000
2 2 2 6 -0.0000000000 0.0000000000
2 2 3 6 -0.8892553594 0.0000000000
3 2 1 1 -2.8021629167 -0.0000000000
3 2 2 1 -2.8021629167 0.0000000000
3 2 3 1 -5.6043258334 0.0000000000
3 2 1 2 2.8021094793 0.0000000000
3 2 2 2 2.8021094793 0.0000000000
3 2 3 2 5.6042189585 0.0000000000
3 2 1 4 0.0000000000 0.0000000000
3 2 2 4 -0.0000000000 0.0000000000
3 2 3 4 -4.6868870947 0.0000000000
3 2 1 5 -0.0000000000 0.0000000000
3 2 2 5 -0.0000000000 0.0000000000
3 2 3 5 -0.0000000000 0.0000000000
3 2 1 6 -0.8892553590 0.0000000000
3 2 2 6 -0.8892553578 0.0000000000
3 2 3 6 0.0000000000 0.0000000000
1 4 1 1 -45.5781993385 0.0000000000
1 4 2 1 0.0000000000 0.0000000000
1 4 3 1 0.0000000000 0.0000000000
1 4 1 2 -4.6868902326 0.0000000000
1 4 2 2 0.0000000000 0.0000000000
1 4 3 2 0.0000000000 0.0000000000
1 4 1 4 -132.3808243684 0.0000000000
1 4 2 4 44.1269414561 0.0000000000
1 4 3 4 44.1269414561 0.0000000000
1 4 1 5 0.0000000000 0.0000000000
1 4 2 5 0.0000000000 0.0000000000
1 4 3 5 0.0000000000 0.0000000000
1 4 1 6 1.8664623329 0.0000000000
1 4 2 6 -1.8664623337 0.0000000000
1 4 3 6 -1.8664623342 0.0000000000
2 4 1 1 0.0000000000 0.0000000000
2 4 2 1 -45.5781993385 0.0000000000
2 4 3 1 -0.0000000000 0.0000000000
2 4 1 2 0.0000000000 0.0000000000
2 4 2 2 -4.6868902326 0.0000000000
2 4 3 2 -0.0000000000 0.0000000000
2 4 1 4 44.1269414561 0.0000000000
2 4 2 4 -132.3808243684 0.0000000000
2 4 3 4 44.1269414561 0.0000000000
2 4 1 5 -0.0000000000 0.0000000000
2 4 2 5 0.0000000000 0.0000000000
2 4 3 5 0.0000000000 0.0000000000
2 4 1 6 -1.8664623329 0.0000000000
2 4 2 6 1.8664623337 0.0000000000
2 4 3 6 -1.8664623342 0.0000000000
3 4 1 1 0.0000000000 0.0000000000
3 4 2 1 0.0000000000 0.0000000000
3 4 3 1 -45.5781993385 0.0000000000
3 4 1 2 0.0000000000 0.0000000000
3 4 2 2 0.0000000000 0.0000000000
3 4 3 2 -4.6868902326 0.0000000000
3 4 1 4 44.1269414561 0.0000000000
3 4 2 4 44.1269414561 0.0000000000
3 4 3 4 -132.3808243684 0.0000000000
3 4 1 5 -0.0000000000 0.0000000000
3 4 2 5 0.0000000000 0.0000000000
3 4 3 5 0.0000000000 0.0000000000
3 4 1 6 -1.8664623329 0.0000000000
3 4 2 6 -1.8664623337 0.0000000000
3 4 3 6 1.8664623342 0.0000000000
1 5 1 5 1.3236107163 0.0000000000
1 5 2 5 0.6778600193 0.0000000000
1 5 3 5 0.6778600149 0.0000000000
1 5 1 6 0.0000000174 0.0000000000
1 5 2 6 0.0000000180 0.0000000000
1 5 3 6 -0.0000000300 0.0000000000
2 5 1 5 0.6778600160 0.0000000000
2 5 2 5 1.3236107332 0.0000000000
2 5 3 5 0.6778600121 0.0000000000
2 5 1 6 0.0000000225 0.0000000000
2 5 2 6 0.0000000174 0.0000000000
2 5 3 6 -0.0000000300 0.0000000000
3 5 1 5 0.6778600132 0.0000000000
3 5 2 5 0.6778600137 0.0000000000
3 5 3 5 1.3236107457 0.0000000000
3 5 1 6 0.0000000225 0.0000000000
3 5 2 6 0.0000000180 0.0000000000
3 5 3 6 -0.0000000248 0.0000000000
1 6 1 5 -0.0000000030 0.0000000000
1 6 2 5 -0.0000000085 0.0000000000
1 6 3 5 -0.0000000085 0.0000000000
1 6 1 6 0.9063406151 0.0000000000
1 6 2 6 0.0000000030 0.0000000000
1 6 3 6 -0.0000000000 0.0000000000
2 6 1 5 0.0000000000 0.0000000000
2 6 2 5 -0.0000000000 0.0000000000
2 6 3 5 0.0000000000 0.0000000000
2 6 1 6 0.0000000030 0.0000000000
2 6 2 6 0.9063406123 0.0000000000
2 6 3 6 -0.0000000030 0.0000000000
3 6 1 5 0.0000000085 0.0000000000
3 6 2 5 0.0000000085 0.0000000000
3 6 3 5 0.0000000030 0.0000000000
3 6 1 6 -0.0000000000 0.0000000000
3 6 2 6 -0.0000000030 0.0000000000
3 6 3 6 0.9063406110 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 0.1059530620 0.0000000000
1 1 2 1 -0.0000000000 0.0000000000
1 1 3 1 0.0000000000 0.0000000000
1 1 1 2 -0.1059530620 0.0000000000
1 1 2 2 0.0000000000 0.0000000000
1 1 3 2 -0.0000000000 0.0000000000
2 1 1 1 -0.0000000000 0.0000000000
2 1 2 1 0.1059530620 0.0000000000
2 1 3 1 0.0000000000 0.0000000000
2 1 1 2 0.0000000000 0.0000000000
2 1 2 2 -0.1059530620 0.0000000000
2 1 3 2 -0.0000000000 0.0000000000
3 1 1 1 0.0000000000 0.0000000000
3 1 2 1 0.0000000000 0.0000000000
3 1 3 1 0.1059530620 0.0000000000
3 1 1 2 -0.0000000000 0.0000000000
3 1 2 2 -0.0000000000 0.0000000000
3 1 3 2 -0.1059530620 0.0000000000
1 2 1 1 -0.1059530175 0.0000000000
1 2 2 1 0.0000000000 0.0000000000
1 2 3 1 -0.0000000000 0.0000000000
1 2 1 2 0.1059530175 0.0000000000
1 2 2 2 -0.0000000000 0.0000000000
1 2 3 2 0.0000000000 0.0000000000
2 2 1 1 0.0000000000 0.0000000000
2 2 2 1 -0.1059530175 0.0000000000
2 2 3 1 -0.0000000000 0.0000000000
2 2 1 2 -0.0000000000 0.0000000000
2 2 2 2 0.1059530175 0.0000000000
2 2 3 2 0.0000000000 0.0000000000
3 2 1 1 -0.0000000000 0.0000000000
3 2 2 1 -0.0000000000 0.0000000000
3 2 3 1 -0.1059530175 0.0000000000
3 2 1 2 0.0000000000 0.0000000000
3 2 2 2 0.0000000000 0.0000000000
3 2 3 2 0.1059530175 0.0000000000
Dielectric tensor, in cartesian coordinates,
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 4 1 4 6.4625311139 -0.0000000000
1 4 2 4 0.0000000000 -0.0000000000
1 4 3 4 0.0000000000 -0.0000000000
2 4 1 4 0.0000000000 -0.0000000000
2 4 2 4 6.4625311139 -0.0000000000
2 4 3 4 0.0000000000 -0.0000000000
3 4 1 4 0.0000000000 -0.0000000000
3 4 2 4 0.0000000000 -0.0000000000
3 4 3 4 6.4625311139 -0.0000000000
Effective charges, in cartesian coordinates,
(from electric field response)
if specified in the inputs, charge neutrality has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 4 -2.2540260933 0.0000000000
2 1 1 4 -0.0000000000 0.0000000000
3 1 1 4 0.0000000000 0.0000000000
1 2 1 4 2.2540260933 0.0000000000
2 2 1 4 0.0000000000 0.0000000000
3 2 1 4 -0.0000000000 0.0000000000
1 1 2 4 -0.0000000000 0.0000000000
2 1 2 4 -2.2540260933 0.0000000000
3 1 2 4 0.0000000000 0.0000000000
1 2 2 4 0.0000000000 0.0000000000
2 2 2 4 2.2540260933 0.0000000000
3 2 2 4 -0.0000000000 0.0000000000
1 1 3 4 0.0000000000 0.0000000000
2 1 3 4 -0.0000000000 0.0000000000
3 1 3 4 -2.2540260933 0.0000000000
1 2 3 4 -0.0000000000 0.0000000000
2 2 3 4 0.0000000000 0.0000000000
3 2 3 4 2.2540260933 0.0000000000
Effective charges, in cartesian coordinates,
(from phonon response)
if specified in the inputs, charge neutrality has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 4 1 1 -2.2540269869 0.0000000000
2 4 1 1 0.0000000000 0.0000000000
3 4 1 1 0.0000000000 0.0000000000
1 4 2 1 0.0000000000 0.0000000000
2 4 2 1 -2.2540269869 0.0000000000
3 4 2 1 -0.0000000000 0.0000000000
1 4 3 1 -0.0000000000 0.0000000000
2 4 3 1 -0.0000000000 0.0000000000
3 4 3 1 -2.2540269869 0.0000000000
1 4 1 2 2.2540269869 0.0000000000
2 4 1 2 -0.0000000000 0.0000000000
3 4 1 2 -0.0000000000 0.0000000000
1 4 2 2 -0.0000000000 0.0000000000
2 4 2 2 2.2540269869 0.0000000000
3 4 2 2 0.0000000000 0.0000000000
1 4 3 2 0.0000000000 0.0000000000
2 4 3 2 0.0000000000 0.0000000000
3 4 3 2 2.2540269869 0.0000000000
Rigid-atom elastic tensor , in cartesian coordinates,
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 5 1 5 0.0048658666 0.0000000000
1 5 2 5 0.0024919536 0.0000000000
1 5 3 5 0.0024919536 0.0000000000
1 5 1 6 0.0000000001 0.0000000000
1 5 2 6 0.0000000001 0.0000000000
1 5 3 6 -0.0000000001 0.0000000000
2 5 1 5 0.0024919536 0.0000000000
2 5 2 5 0.0048658667 0.0000000000
2 5 3 5 0.0024919535 0.0000000000
2 5 1 6 0.0000000001 0.0000000000
2 5 2 6 0.0000000001 0.0000000000
2 5 3 6 -0.0000000001 0.0000000000
3 5 1 5 0.0024919535 0.0000000000
3 5 2 5 0.0024919536 0.0000000000
3 5 3 5 0.0048658667 0.0000000000
3 5 1 6 0.0000000001 0.0000000000
3 5 2 6 0.0000000001 0.0000000000
3 5 3 6 -0.0000000001 0.0000000000
1 6 1 5 -0.0000000000 0.0000000000
1 6 2 5 -0.0000000000 0.0000000000
1 6 3 5 -0.0000000000 0.0000000000
1 6 1 6 0.0033318955 0.0000000000
1 6 2 6 0.0000000000 0.0000000000
1 6 3 6 -0.0000000000 0.0000000000
2 6 1 5 0.0000000000 0.0000000000
2 6 2 5 -0.0000000000 0.0000000000
2 6 3 5 0.0000000000 0.0000000000
2 6 1 6 0.0000000000 0.0000000000
2 6 2 6 0.0033318955 0.0000000000
2 6 3 6 -0.0000000000 0.0000000000
3 6 1 5 0.0000000000 0.0000000000
3 6 2 5 0.0000000000 0.0000000000
3 6 3 5 0.0000000000 0.0000000000
3 6 1 6 -0.0000000000 0.0000000000
3 6 2 6 -0.0000000000 0.0000000000
3 6 3 6 0.0033318955 0.0000000000
Internal strain coupling parameters, in cartesian coordinates,
zero average net force deriv. has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 5 -0.0000000000 0.0000000000
1 1 2 5 -0.0000000000 0.0000000000
1 1 3 5 -0.0000000000 0.0000000000
1 1 1 6 -0.1729191579 0.0000000000
1 1 2 6 -0.0000000000 0.0000000000
1 1 3 6 0.0000000000 0.0000000000
2 1 1 5 -0.0000000000 0.0000000000
2 1 2 5 0.0000000000 0.0000000000
2 1 3 5 0.0000000000 0.0000000000
2 1 1 6 -0.0000000000 0.0000000000
2 1 2 6 -0.1729191579 0.0000000000
2 1 3 6 0.0000000000 0.0000000000
3 1 1 5 0.0000000000 0.0000000000
3 1 2 5 0.0000000000 0.0000000000
3 1 3 5 0.0000000000 0.0000000000
3 1 1 6 0.0000000000 0.0000000000
3 1 2 6 0.0000000000 0.0000000000
3 1 3 6 -0.1729191578 0.0000000000
1 2 1 5 0.0000000000 0.0000000000
1 2 2 5 0.0000000000 0.0000000000
1 2 3 5 0.0000000000 0.0000000000
1 2 1 6 0.1729191579 0.0000000000
1 2 2 6 0.0000000000 0.0000000000
1 2 3 6 -0.0000000000 0.0000000000
2 2 1 5 0.0000000000 0.0000000000
2 2 2 5 -0.0000000000 0.0000000000
2 2 3 5 -0.0000000000 0.0000000000
2 2 1 6 0.0000000000 0.0000000000
2 2 2 6 0.1729191579 0.0000000000
2 2 3 6 -0.0000000000 0.0000000000
3 2 1 5 -0.0000000000 0.0000000000
3 2 2 5 -0.0000000000 0.0000000000
3 2 3 5 -0.0000000000 0.0000000000
3 2 1 6 -0.0000000000 0.0000000000
3 2 2 6 -0.0000000000 0.0000000000
3 2 3 6 0.1729191578 0.0000000000
Rigid-atom proper piezoelectric tensor, in cartesian coordinates,
(from strain response)
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 4 1 5 -0.0000000000 0.0000000000
1 4 2 5 0.0000000000 0.0000000000
1 4 3 5 0.0000000000 0.0000000000
1 4 1 6 -0.0112320573 0.0000000000
1 4 2 6 0.0000000000 0.0000000000
1 4 3 6 -0.0000000000 0.0000000000
2 4 1 5 0.0000000000 0.0000000000
2 4 2 5 0.0000000000 0.0000000000
2 4 3 5 0.0000000000 0.0000000000
2 4 1 6 0.0000000000 0.0000000000
2 4 2 6 -0.0112320573 0.0000000000
2 4 3 6 0.0000000000 0.0000000000
3 4 1 5 -0.0000000000 0.0000000000
3 4 2 5 0.0000000000 0.0000000000
3 4 3 5 0.0000000000 0.0000000000
3 4 1 6 0.0000000000 0.0000000000
3 4 2 6 0.0000000000 0.0000000000
3 4 3 6 -0.0112320573 0.0000000000
Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00 2.007673E-03 2.007673E-03
2.007673E-03
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00 4.406332E+02 4.406332E+02
- 4.406332E+02
Phonon at Gamma, with non-analyticity in the
direction (cartesian coordinates) 1.00000 0.00000 0.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00 2.007673E-03 2.007673E-03
2.326456E-03
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00 4.406332E+02 4.406332E+02
- 5.105981E+02
Phonon at Gamma, with non-analyticity in the
direction (cartesian coordinates) 0.00000 1.00000 0.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00 2.007673E-03 2.007673E-03
2.326456E-03
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00 4.406332E+02 4.406332E+02
- 5.105981E+02
Phonon at Gamma, with non-analyticity in the
direction (cartesian coordinates) 0.00000 0.00000 1.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00 2.007673E-03 2.007673E-03
2.326456E-03
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00 4.406332E+02 4.406332E+02
- 5.105981E+02
== END DATASET(S) ==============================================================
================================================================================
-outvars: echo values of variables after computation --------
acell 7.2728565836E+00 7.2728565836E+00 7.2728565836E+00 Bohr
amu 3.09737620E+01 2.69815390E+01
berryopt1 0
berryopt2 -2
berryopt3 0
dilatmx 1.05000000E+00
ecut 5.00000000E+00 Hartree
ecutsm 5.00000000E-01 Hartree
etotal1 -9.2844385682E+00
etotal3 9.0634016857E-01
fcart1 -0.0000000000E+00 -0.0000000000E+00 -0.0000000000E+00
-0.0000000000E+00 -0.0000000000E+00 -0.0000000000E+00
fcart3 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
- fftalg 512
getddk1 0
getddk2 0
getddk3 2
getden1 0
getden2 1
getden3 0
getwfk1 0
getwfk2 1
getwfk3 2
iscf1 7
iscf2 -2
iscf3 7
ixc -1012
jdtset 1 2 3
kpt1 -8.33333333E-02 -1.66666667E-01 0.00000000E+00
-8.33333333E-02 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -2.50000000E-01 0.00000000E+00
-8.33333333E-02 -2.50000000E-01 8.33333333E-02
-8.33333333E-02 5.00000000E-01 0.00000000E+00
-1.66666667E-01 -4.16666667E-01 0.00000000E+00
-8.33333333E-02 -4.16666667E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -3.33333333E-01 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 1.66666667E-01
-8.33333333E-02 3.33333333E-01 0.00000000E+00
-1.66666667E-01 4.16666667E-01 0.00000000E+00
-2.50000000E-01 5.00000000E-01 0.00000000E+00
-1.66666667E-01 5.00000000E-01 8.33333333E-02
-3.33333333E-01 -4.16666667E-01 0.00000000E+00
-2.50000000E-01 -4.16666667E-01 8.33333333E-02
-1.66666667E-01 -4.16666667E-01 1.66666667E-01
-8.33333333E-02 -4.16666667E-01 2.50000000E-01
-8.33333333E-02 1.66666667E-01 0.00000000E+00
-1.66666667E-01 2.50000000E-01 0.00000000E+00
-2.50000000E-01 3.33333333E-01 0.00000000E+00
-3.33333333E-01 4.16666667E-01 0.00000000E+00
-4.16666667E-01 5.00000000E-01 0.00000000E+00
-3.33333333E-01 5.00000000E-01 8.33333333E-02
-2.50000000E-01 5.00000000E-01 1.66666667E-01
-8.33333333E-02 0.00000000E+00 0.00000000E+00
-2.50000000E-01 0.00000000E+00 0.00000000E+00
-4.16666667E-01 0.00000000E+00 0.00000000E+00
kpt2 -8.33333333E-02 -1.66666667E-01 0.00000000E+00
-1.66666667E-01 -8.33333333E-02 0.00000000E+00
-8.33333333E-02 -8.33333333E-02 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -2.50000000E-01 0.00000000E+00
-8.33333333E-02 -2.50000000E-01 8.33333333E-02
-2.50000000E-01 -1.66666667E-01 0.00000000E+00
-1.66666667E-01 -1.66666667E-01 8.33333333E-02
-8.33333333E-02 -1.66666667E-01 1.66666667E-01
-3.33333333E-01 -8.33333333E-02 0.00000000E+00
-2.50000000E-01 -8.33333333E-02 8.33333333E-02
-1.66666667E-01 -8.33333333E-02 1.66666667E-01
-8.33333333E-02 -8.33333333E-02 2.50000000E-01
-8.33333333E-02 5.00000000E-01 0.00000000E+00
-1.66666667E-01 -4.16666667E-01 0.00000000E+00
-8.33333333E-02 -4.16666667E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -3.33333333E-01 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 1.66666667E-01
-3.33333333E-01 -2.50000000E-01 0.00000000E+00
-2.50000000E-01 -2.50000000E-01 8.33333333E-02
-1.66666667E-01 -2.50000000E-01 1.66666667E-01
-8.33333333E-02 -2.50000000E-01 2.50000000E-01
-4.16666667E-01 -1.66666667E-01 0.00000000E+00
-3.33333333E-01 -1.66666667E-01 8.33333333E-02
-2.50000000E-01 -1.66666667E-01 1.66666667E-01
-1.66666667E-01 -1.66666667E-01 2.50000000E-01
-8.33333333E-02 -1.66666667E-01 3.33333333E-01
5.00000000E-01 -8.33333333E-02 0.00000000E+00
-4.16666667E-01 -8.33333333E-02 8.33333333E-02
-3.33333333E-01 -8.33333333E-02 1.66666667E-01
-2.50000000E-01 -8.33333333E-02 2.50000000E-01
-1.66666667E-01 -8.33333333E-02 3.33333333E-01
-8.33333333E-02 -8.33333333E-02 4.16666667E-01
-8.33333333E-02 3.33333333E-01 0.00000000E+00
-1.66666667E-01 4.16666667E-01 0.00000000E+00
-8.33333333E-02 4.16666667E-01 8.33333333E-02
-2.50000000E-01 5.00000000E-01 0.00000000E+00
-1.66666667E-01 5.00000000E-01 8.33333333E-02
-8.33333333E-02 5.00000000E-01 1.66666667E-01
-3.33333333E-01 -4.16666667E-01 0.00000000E+00
-2.50000000E-01 -4.16666667E-01 8.33333333E-02
-1.66666667E-01 -4.16666667E-01 1.66666667E-01
-8.33333333E-02 -4.16666667E-01 2.50000000E-01
-4.16666667E-01 -3.33333333E-01 0.00000000E+00
-3.33333333E-01 -3.33333333E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 1.66666667E-01
-1.66666667E-01 -3.33333333E-01 2.50000000E-01
-8.33333333E-02 -3.33333333E-01 3.33333333E-01
5.00000000E-01 -2.50000000E-01 0.00000000E+00
kpt3 -8.33333333E-02 -1.66666667E-01 0.00000000E+00
-1.66666667E-01 -8.33333333E-02 0.00000000E+00
-8.33333333E-02 -8.33333333E-02 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -2.50000000E-01 0.00000000E+00
-8.33333333E-02 -2.50000000E-01 8.33333333E-02
-2.50000000E-01 -1.66666667E-01 0.00000000E+00
-1.66666667E-01 -1.66666667E-01 8.33333333E-02
-8.33333333E-02 -1.66666667E-01 1.66666667E-01
-3.33333333E-01 -8.33333333E-02 0.00000000E+00
-2.50000000E-01 -8.33333333E-02 8.33333333E-02
-1.66666667E-01 -8.33333333E-02 1.66666667E-01
-8.33333333E-02 -8.33333333E-02 2.50000000E-01
-8.33333333E-02 5.00000000E-01 0.00000000E+00
-1.66666667E-01 -4.16666667E-01 0.00000000E+00
-8.33333333E-02 -4.16666667E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 0.00000000E+00
-1.66666667E-01 -3.33333333E-01 8.33333333E-02
-8.33333333E-02 -3.33333333E-01 1.66666667E-01
-3.33333333E-01 -2.50000000E-01 0.00000000E+00
-2.50000000E-01 -2.50000000E-01 8.33333333E-02
-1.66666667E-01 -2.50000000E-01 1.66666667E-01
-8.33333333E-02 -2.50000000E-01 2.50000000E-01
-4.16666667E-01 -1.66666667E-01 0.00000000E+00
-3.33333333E-01 -1.66666667E-01 8.33333333E-02
-2.50000000E-01 -1.66666667E-01 1.66666667E-01
-1.66666667E-01 -1.66666667E-01 2.50000000E-01
-8.33333333E-02 -1.66666667E-01 3.33333333E-01
5.00000000E-01 -8.33333333E-02 0.00000000E+00
-4.16666667E-01 -8.33333333E-02 8.33333333E-02
-3.33333333E-01 -8.33333333E-02 1.66666667E-01
-2.50000000E-01 -8.33333333E-02 2.50000000E-01
-1.66666667E-01 -8.33333333E-02 3.33333333E-01
-8.33333333E-02 -8.33333333E-02 4.16666667E-01
-8.33333333E-02 3.33333333E-01 0.00000000E+00
-1.66666667E-01 4.16666667E-01 0.00000000E+00
-8.33333333E-02 4.16666667E-01 8.33333333E-02
-2.50000000E-01 5.00000000E-01 0.00000000E+00
-1.66666667E-01 5.00000000E-01 8.33333333E-02
-8.33333333E-02 5.00000000E-01 1.66666667E-01
-3.33333333E-01 -4.16666667E-01 0.00000000E+00
-2.50000000E-01 -4.16666667E-01 8.33333333E-02
-1.66666667E-01 -4.16666667E-01 1.66666667E-01
-8.33333333E-02 -4.16666667E-01 2.50000000E-01
-4.16666667E-01 -3.33333333E-01 0.00000000E+00
-3.33333333E-01 -3.33333333E-01 8.33333333E-02
-2.50000000E-01 -3.33333333E-01 1.66666667E-01
-1.66666667E-01 -3.33333333E-01 2.50000000E-01
-8.33333333E-02 -3.33333333E-01 3.33333333E-01
5.00000000E-01 -2.50000000E-01 0.00000000E+00
outvar_i_n : Printing only first 50 k-points.
kptopt1 1
kptopt2 2
kptopt3 2
kptrlatt 6 -6 6 -6 6 6 -6 -6 6
kptrlen 6.17122345E+01
P mkmem1 28
P mkmem2 432
P mkmem3 432
P mkqmem1 28
P mkqmem2 432
P mkqmem3 432
P mk1mem1 28
P mk1mem2 432
P mk1mem3 432
natom 2
nband1 4
nband2 4
nband3 4
nbdbuf1 0
nbdbuf2 2
nbdbuf3 0
ndtset 3
ngfft 16 16 16
nkpt1 28
nkpt2 432
nkpt3 432
nstep1 8
nstep2 30
nstep3 8
nsym 24
ntypat 2
occ1 2.000000 2.000000 2.000000 2.000000
occ3 2.000000 2.000000 2.000000 2.000000
optdriver1 0
optdriver2 0
optdriver3 1
prtden1 1
prtden2 0
prtden3 0
prteig 0
prtpot1 0
prtpot2 0
prtpot3 1
prtwf1 1
prtwf2 1
prtwf3 0
rfelfd1 0
rfelfd2 0
rfelfd3 3
rfphon1 0
rfphon2 0
rfphon3 1
rfstrs1 0
rfstrs2 0
rfstrs3 3
rprim 0.0000000000E+00 7.0710678119E-01 7.0710678119E-01
7.0710678119E-01 0.0000000000E+00 7.0710678119E-01
7.0710678119E-01 7.0710678119E-01 0.0000000000E+00
shiftk 5.00000000E-01 5.00000000E-01 5.00000000E-01
spgroup 216
strten1 2.0949188185E-10 2.0949188196E-10 2.0949188196E-10
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
symrel 1 0 0 0 1 0 0 0 1 0 -1 1 0 -1 0 1 -1 0
-1 0 0 -1 0 1 -1 1 0 0 1 -1 1 0 -1 0 0 -1
-1 0 0 -1 1 0 -1 0 1 0 -1 1 1 -1 0 0 -1 0
1 0 0 0 0 1 0 1 0 0 1 -1 0 0 -1 1 0 -1
-1 0 1 -1 1 0 -1 0 0 0 -1 0 1 -1 0 0 -1 1
1 0 -1 0 0 -1 0 1 -1 0 1 0 0 0 1 1 0 0
1 0 -1 0 1 -1 0 0 -1 0 -1 0 0 -1 1 1 -1 0
-1 0 1 -1 0 0 -1 1 0 0 1 0 1 0 0 0 0 1
0 0 -1 0 1 -1 1 0 -1 1 -1 0 0 -1 1 0 -1 0
0 0 1 1 0 0 0 1 0 -1 1 0 -1 0 0 -1 0 1
0 0 1 0 1 0 1 0 0 1 -1 0 0 -1 0 0 -1 1
0 0 -1 1 0 -1 0 1 -1 -1 1 0 -1 0 1 -1 0 0
tolvrs1 1.00000000E-18
tolvrs2 0.00000000E+00
tolvrs3 1.00000000E-12
tolwfr1 0.00000000E+00
tolwfr2 1.00000000E-22
tolwfr3 0.00000000E+00
typat 1 2
wtk1 0.02778 0.02778 0.02778 0.05556 0.02778 0.02778
0.05556 0.02778 0.05556 0.05556 0.02778 0.02778
0.02778 0.05556 0.02778 0.05556 0.05556 0.05556
0.02778 0.02778 0.02778 0.02778 0.02778 0.05556
0.05556 0.00926 0.00926 0.00926
wtk2 0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231
wtk3 0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231 0.00231 0.00231 0.00231 0.00231
0.00231 0.00231
outvars : Printing only first 50 k-points.
xangst 1.3606961663E+00 1.3606961663E+00 1.3606961663E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
xcart 2.5713431044E+00 2.5713431044E+00 2.5713431044E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
xred 2.5000000000E-01 2.5000000000E-01 2.5000000000E-01
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
znucl 15.00000 13.00000
================================================================================
- 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] Metric tensor formulation of strain in density-functional perturbation theory,
- D. R. Hamann, X. Wu, K. M. Rabe, and D. Vanderbilt, Phys. Rev. B71, 035117 (2005).
- Comment: Non-vanishing rfstrs. Strong suggestion to cite this paper in your publications.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#hamann2005
-
- [2] Libxc: A library of exchange and correlation functionals for density functional theory.
- M.A.L. Marques, M.J.T. Oliveira, T. Burnus, Computer Physics Communications 183, 2227 (2012).
- Comment: to be cited when LibXC is used (negative value of ixc)
- Strong suggestion to cite this paper.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#marques2012
-
- [3] 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
-
- [4] 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
-
- [5] 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
-
- [6] Optimized norm-conserving Vanderbilt pseudopotentials.
- D.R. Hamann, Phys. Rev. B 88, 085117 (2013).
- Comment: Some pseudopotential generated using the ONCVPSP code were used.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#hamann2013
-
- [7] 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
-
- [8] 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= 31.9 wall= 32.8
================================================================================
Calculation completed.
.Delivered 21 WARNINGs and 8 COMMENTs to log file.
+Overall time at end (sec) : cpu= 31.9 wall= 32.8
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