abinit/tests/v3/Refs/t86.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 19h09 )
- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/v3_t86/t86.abi
- output file -> t86.abo
- root for input files -> t86i
- root for output files -> t86o
DATASET 1 : space group Fd -3 m (#227); 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 = 15 mpssoang = 3 mqgrid = 3001
natom = 2 nloc_mem = 1 nspden = 2 nspinor = 1
nsppol = 2 nsym = 48 n1xccc = 2501 ntypat = 1
occopt = 1 xclevel = 1
- mband = 6 mffmem = 1 mkmem = 2
mpw = 100 nfft = 3375 nkpt = 2
================================================================================
P This job should need less than 2.143 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.039 Mbytes ; DEN or POT disk file : 0.053 Mbytes.
================================================================================
DATASET 2 : space group Fd -3 m (#227); Bravais cF (face-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 2.
intxc = 0 ionmov = 0 iscf = -2 lmnmax = 2
lnmax = 2 mgfft = 15 mpssoang = 3 mqgrid = 3001
natom = 2 nloc_mem = 1 nspden = 2 nspinor = 1
nsppol = 2 nsym = 48 n1xccc = 2501 ntypat = 1
occopt = 1 xclevel = 1
- mband = 6 mffmem = 1 mkmem = 32
mpw = 100 nfft = 3375 nkpt = 32
================================================================================
P This job should need less than 1.957 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.588 Mbytes ; DEN or POT disk file : 0.053 Mbytes.
================================================================================
DATASET 3 : space group Fd -3 m (#227); 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 = 15 mpssoang = 3 mqgrid = 3001 natom = 2
nloc_mem = 1 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 2501 ntypat = 1 occopt = 1
xclevel = 1
- mband = 6 mffmem = 1 mkmem = 32
- mkqmem = 32 mk1mem = 32 mpw = 100
nfft = 3375 nkpt = 32
================================================================================
P This job should need less than 3.491 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.588 Mbytes ; DEN or POT disk file : 0.053 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 1.0208000000E+01 1.0208000000E+01 1.0208000000E+01 Bohr
amu 2.80855000E+01
asr 0
chneut 0
diemac 3.00000000E+00
ecut 4.00000000E+00 Hartree
- fftalg 512
getden1 0
getden2 1
getden3 1
getwfk1 0
getwfk2 1
getwfk3 1
getwfq1 0
getwfq2 0
getwfq3 2
iscf1 7
iscf2 -2
iscf3 7
ixc 7
jdtset 1 2 3
kpt1 -2.50000000E-01 5.00000000E-01 0.00000000E+00
-2.50000000E-01 0.00000000E+00 0.00000000E+00
kpt2 -2.50000000E-01 5.00000000E-01 0.00000000E+00
5.00000000E-01 -2.50000000E-01 0.00000000E+00
-2.50000000E-01 -2.50000000E-01 2.50000000E-01
-2.50000000E-01 0.00000000E+00 0.00000000E+00
5.00000000E-01 2.50000000E-01 0.00000000E+00
-2.50000000E-01 2.50000000E-01 2.50000000E-01
2.50000000E-01 5.00000000E-01 0.00000000E+00
5.00000000E-01 5.00000000E-01 2.50000000E-01
-2.50000000E-01 5.00000000E-01 5.00000000E-01
0.00000000E+00 -2.50000000E-01 0.00000000E+00
2.50000000E-01 -2.50000000E-01 2.50000000E-01
5.00000000E-01 -2.50000000E-01 5.00000000E-01
-2.50000000E-01 -2.50000000E-01 -2.50000000E-01
2.50000000E-01 0.00000000E+00 0.00000000E+00
5.00000000E-01 0.00000000E+00 2.50000000E-01
-2.50000000E-01 0.00000000E+00 5.00000000E-01
0.00000000E+00 2.50000000E-01 0.00000000E+00
2.50000000E-01 2.50000000E-01 2.50000000E-01
5.00000000E-01 2.50000000E-01 5.00000000E-01
-2.50000000E-01 2.50000000E-01 -2.50000000E-01
0.00000000E+00 5.00000000E-01 2.50000000E-01
2.50000000E-01 5.00000000E-01 5.00000000E-01
5.00000000E-01 5.00000000E-01 -2.50000000E-01
0.00000000E+00 -2.50000000E-01 5.00000000E-01
2.50000000E-01 -2.50000000E-01 -2.50000000E-01
0.00000000E+00 0.00000000E+00 2.50000000E-01
2.50000000E-01 0.00000000E+00 5.00000000E-01
5.00000000E-01 0.00000000E+00 -2.50000000E-01
0.00000000E+00 2.50000000E-01 5.00000000E-01
2.50000000E-01 2.50000000E-01 -2.50000000E-01
0.00000000E+00 5.00000000E-01 -2.50000000E-01
0.00000000E+00 0.00000000E+00 -2.50000000E-01
kpt3 -2.50000000E-01 5.00000000E-01 0.00000000E+00
5.00000000E-01 -2.50000000E-01 0.00000000E+00
-2.50000000E-01 -2.50000000E-01 2.50000000E-01
-2.50000000E-01 0.00000000E+00 0.00000000E+00
5.00000000E-01 2.50000000E-01 0.00000000E+00
-2.50000000E-01 2.50000000E-01 2.50000000E-01
2.50000000E-01 5.00000000E-01 0.00000000E+00
5.00000000E-01 5.00000000E-01 2.50000000E-01
-2.50000000E-01 5.00000000E-01 5.00000000E-01
0.00000000E+00 -2.50000000E-01 0.00000000E+00
2.50000000E-01 -2.50000000E-01 2.50000000E-01
5.00000000E-01 -2.50000000E-01 5.00000000E-01
-2.50000000E-01 -2.50000000E-01 -2.50000000E-01
2.50000000E-01 0.00000000E+00 0.00000000E+00
5.00000000E-01 0.00000000E+00 2.50000000E-01
-2.50000000E-01 0.00000000E+00 5.00000000E-01
0.00000000E+00 2.50000000E-01 0.00000000E+00
2.50000000E-01 2.50000000E-01 2.50000000E-01
5.00000000E-01 2.50000000E-01 5.00000000E-01
-2.50000000E-01 2.50000000E-01 -2.50000000E-01
0.00000000E+00 5.00000000E-01 2.50000000E-01
2.50000000E-01 5.00000000E-01 5.00000000E-01
5.00000000E-01 5.00000000E-01 -2.50000000E-01
0.00000000E+00 -2.50000000E-01 5.00000000E-01
2.50000000E-01 -2.50000000E-01 -2.50000000E-01
0.00000000E+00 0.00000000E+00 2.50000000E-01
2.50000000E-01 0.00000000E+00 5.00000000E-01
5.00000000E-01 0.00000000E+00 -2.50000000E-01
0.00000000E+00 2.50000000E-01 5.00000000E-01
2.50000000E-01 2.50000000E-01 -2.50000000E-01
0.00000000E+00 5.00000000E-01 -2.50000000E-01
0.00000000E+00 0.00000000E+00 -2.50000000E-01
kptopt1 1
kptopt2 3
kptopt3 3
kptrlatt 2 -2 2 -2 2 2 -2 -2 2
kptrlen 2.04160000E+01
P mkmem1 2
P mkmem2 32
P mkmem3 32
P mkqmem1 2
P mkqmem2 32
P mkqmem3 32
P mk1mem1 2
P mk1mem2 32
P mk1mem3 32
natom 2
nband1 6
nband2 6
nband3 6
nbdbuf 2
ndtset 3
ngfft 15 15 15
nkpt1 2
nkpt2 32
nkpt3 32
nqpt1 0
nqpt2 1
nqpt3 1
nspden 2
nsppol 2
nstep 12
nsym 48
ntypat 1
occ1 1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
occ3 1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
optdriver1 0
optdriver2 0
optdriver3 1
prtpot1 0
prtpot2 0
prtpot3 1
qpt1 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt2 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt3 5.00000000E-01 0.00000000E+00 0.00000000E+00
rfphon1 0
rfphon2 0
rfphon3 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
shiftk 5.00000000E-01 5.00000000E-01 5.00000000E-01
spgroup 227
spinat 0.0000000000E+00 0.0000000000E+00 2.0000000000E+00
0.0000000000E+00 0.0000000000E+00 2.0000000000E+00
spinmagntarget 0.00000000E+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
tnons 0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
tolvrs1 1.00000000E-20
tolvrs2 0.00000000E+00
tolvrs3 1.00000000E-12
tolwfr1 0.00000000E+00
tolwfr2 1.00000000E-20
tolwfr3 0.00000000E+00
typat 1 1
wtk1 0.75000 0.25000
wtk2 0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125
wtk3 0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125
xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
1.3504602363E+00 1.3504602363E+00 1.3504602363E+00
xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
2.5520000000E+00 2.5520000000E+00 2.5520000000E+00
xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
2.5000000000E-01 2.5000000000E-01 2.5000000000E-01
znucl 14.00000
================================================================================
chkinp: Checking input parameters for consistency, jdtset= 1.
This is a calculation with spin-up and spin-down wavefunctions, ... nsppol= 2
in which the target spin-polarization is zero. ... spinmagntarget= 0.00
Tip ... It might be possible that the ground state is either non-spin-polarized, or antiferromagnetic.
In the former case, it is advantageous to use nsppol=1 and nspden=1,
while in the latter case, it is advantageous to use nsppol=1 and nspden=2.
chkinp: Checking input parameters for consistency, jdtset= 2.
This is a calculation with spin-up and spin-down wavefunctions, ... nsppol= 2
in which the target spin-polarization is zero. ... spinmagntarget= 0.00
Tip ... It might be possible that the ground state is either non-spin-polarized, or antiferromagnetic.
In the former case, it is advantageous to use nsppol=1 and nspden=1,
while in the latter case, it is advantageous to use nsppol=1 and nspden=2.
chkinp: Checking input parameters for consistency, jdtset= 3.
This is a calculation with spin-up and spin-down wavefunctions, ... nsppol= 2
in which the target spin-polarization is zero. ... spinmagntarget= 0.00
Tip ... It might be possible that the ground state is either non-spin-polarized, or antiferromagnetic.
In the former case, it is advantageous to use nsppol=1 and nspden=1,
while in the latter case, it is advantageous to use nsppol=1 and nspden=2.
================================================================================
== DATASET 1 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 1, }
dimensions: {natom: 2, nkpt: 2, mband: 6, nsppol: 2, nspinor: 1, nspden: 2, mpw: 100, }
cutoff_energies: {ecut: 4.0, 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, }
...
Exchange-correlation functional for the present dataset will be:
LDA: Perdew-Wang 92 LSD fit to Ceperley-Alder data - ixc=7
Citation for XC functional:
J.P.Perdew and Y.Wang, PRB 45, 13244 (1992)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 5.1040000 5.1040000 G(1)= -0.0979624 0.0979624 0.0979624
R(2)= 5.1040000 0.0000000 5.1040000 G(2)= 0.0979624 -0.0979624 0.0979624
R(3)= 5.1040000 5.1040000 0.0000000 G(3)= 0.0979624 0.0979624 -0.0979624
Unit cell volume ucvol= 2.6592673E+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= 15 15 15
ecut(hartree)= 4.000 => boxcut(ratio)= 2.16527
--- 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/14si.pspnc
- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/PseudosTM_pwteter/14si.pspnc
- Troullier-Martins psp for element Si Thu Oct 27 17:31:21 EDT 1994
- 14.00000 4.00000 940714 znucl, zion, pspdat
1 1 2 2 2001 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
0 5.907 14.692 1 2.0872718 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
1 2.617 4.181 1 2.0872718 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
2 0.000 0.000 0 2.0872718 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
1.80626423934776 0.22824404341771 1.17378968127746 rchrg,fchrg,qchrg
pspatm : epsatm= 1.43386982
--- l ekb(1:nproj) -->
0 3.287949
1 1.849886
pspatm: atomic psp has been read and splines computed
2.29419171E+01 ecore*ucvol(ha*bohr**3)
--------------------------------------------------------------------------------
_setup2: Arith. and geom. avg. npw (full set) are 99.500 99.496
================================================================================
--- !BeginCycle
iteration_state: {dtset: 1, }
solver: {iscf: 7, nstep: 12, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-20, }
...
iter Etot(hartree) deltaE(h) residm vres2
ETOT 1 -8.8279279772878 -8.828E+00 2.747E-04 4.587E+00
ETOT 2 -8.8322748059663 -4.347E-03 6.037E-10 4.191E-02
ETOT 3 -8.8323031852459 -2.838E-05 2.897E-07 2.956E-03
ETOT 4 -8.8323058290757 -2.644E-06 9.938E-08 1.456E-04
ETOT 5 -8.8323060232735 -1.942E-07 5.743E-09 2.736E-06
ETOT 6 -8.8323060265886 -3.315E-09 1.455E-10 1.262E-09
ETOT 7 -8.8323060265894 -8.509E-13 2.638E-14 3.121E-12
ETOT 8 -8.8323060265894 3.375E-14 5.923E-17 2.994E-14
ETOT 9 -8.8323060265894 -2.665E-14 6.252E-19 1.139E-16
ETOT 10 -8.8323060265895 -2.842E-14 2.704E-21 2.259E-19
ETOT 11 -8.8323060265895 3.553E-15 4.246E-25 1.318E-21
At SCF step 11 vres2 = 1.32E-21 < tolvrs= 1.00E-20 =>converged.
Cartesian components of stress tensor (hartree/bohr^3)
sigma(1 1)= 1.97295601E-04 sigma(3 2)= 0.00000000E+00
sigma(2 2)= 1.97295601E-04 sigma(3 1)= 0.00000000E+00
sigma(3 3)= 1.97295601E-04 sigma(2 1)= 0.00000000E+00
--- !ResultsGS
iteration_state: {dtset: 1, }
comment : Summary of ground state results
lattice_vectors:
- [ 0.0000000, 5.1040000, 5.1040000, ]
- [ 5.1040000, 0.0000000, 5.1040000, ]
- [ 5.1040000, 5.1040000, 0.0000000, ]
lattice_lengths: [ 7.21815, 7.21815, 7.21815, ]
lattice_angles: [ 60.000, 60.000, 60.000, ] # degrees, (23, 13, 12)
lattice_volume: 2.6592673E+02
convergence: {deltae: 3.553E-15, res2: 1.318E-21, residm: 4.246E-25, diffor: null, }
etotal : -8.83230603E+00
entropy : 0.00000000E+00
fermie : 1.91786792E-01
cartesian_stress_tensor: # hartree/bohr^3
- [ 1.97295601E-04, 0.00000000E+00, 0.00000000E+00, ]
- [ 0.00000000E+00, 1.97295601E-04, 0.00000000E+00, ]
- [ 0.00000000E+00, 0.00000000E+00, 1.97295601E-04, ]
pressure_GPa: -5.8046E+00
xred :
- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Si]
- [ 2.5000E-01, 2.5000E-01, 2.5000E-01, Si]
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 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 0.886964 0.886964 1.773927 -0.000000
2 2.00000 0.861280 0.861280 1.722560 -0.000000
---------------------------------------------------------------------
Sum: 1.748244 1.748244 3.496487 -0.000000
Total magnetization (from the atomic spheres): -0.000000
Total magnetization (exact up - dn): 0.000000
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 13.163E-26; max= 42.459E-26
reduced coordinates (array xred) for 2 atoms
0.000000000000 0.000000000000 0.000000000000
0.250000000000 0.250000000000 0.250000000000
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 0.00000000000000 0.00000000000000 0.00000000000000
2 1.35046023632168 1.35046023632168 1.35046023632168
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= 10.208000000000 10.208000000000 10.208000000000 bohr
= 5.401840945287 5.401840945287 5.401840945287 angstroms
prteigrs : about to open file t86o_DS1_EIG
Fermi (or HOMO) energy (hartree) = 0.19179 Average Vxc (hartree)= -0.35504
Eigenvalues (hartree) for nkpt= 2 k points, SPIN UP:
kpt# 1, nband= 6, wtk= 0.75000, kpt= -0.2500 0.5000 0.0000 (reduced coord)
-0.11691 -0.01278 0.08675 0.13604 0.27709 0.38967
prteigrs : prtvol=0 or 1, do not print more k-points.
Eigenvalues (hartree) for nkpt= 2 k points, SPIN DOWN:
kpt# 1, nband= 6, wtk= 0.75000, kpt= -0.2500 0.5000 0.0000 (reduced coord)
-0.11691 -0.01278 0.08675 0.13604 0.27709 0.38967
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 : 2.97973880087700E+00
hartree : 5.34396395460556E-01
xc : -3.54452725797447E+00
Ewald energy : -8.44325712247936E+00
psp_core : 8.62715724957387E-02
local_psp : -2.47150781346426E+00
non_local_psp : 2.02657939849534E+00
total_energy : -8.83230602658946E+00
total_energy_eV : -2.40339269658517E+02
band_energy : 2.75366585776352E-01
...
Cartesian components of stress tensor (hartree/bohr^3)
sigma(1 1)= 1.97295601E-04 sigma(3 2)= 0.00000000E+00
sigma(2 2)= 1.97295601E-04 sigma(3 1)= 0.00000000E+00
sigma(3 3)= 1.97295601E-04 sigma(2 1)= 0.00000000E+00
-Cartesian components of stress tensor (GPa) [Pressure= -5.8046E+00 GPa]
- sigma(1 1)= 5.80463600E+00 sigma(3 2)= 0.00000000E+00
- sigma(2 2)= 5.80463600E+00 sigma(3 1)= 0.00000000E+00
- sigma(3 3)= 5.80463600E+00 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: 32, mband: 6, nsppol: 2, nspinor: 1, nspden: 2, mpw: 100, }
cutoff_energies: {ecut: 4.0, 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.
Exchange-correlation functional for the present dataset will be:
LDA: Perdew-Wang 92 LSD fit to Ceperley-Alder data - ixc=7
Citation for XC functional:
J.P.Perdew and Y.Wang, PRB 45, 13244 (1992)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 5.1040000 5.1040000 G(1)= -0.0979624 0.0979624 0.0979624
R(2)= 5.1040000 0.0000000 5.1040000 G(2)= 0.0979624 -0.0979624 0.0979624
R(3)= 5.1040000 5.1040000 0.0000000 G(3)= 0.0979624 0.0979624 -0.0979624
Unit cell volume ucvol= 2.6592673E+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= 15 15 15
ecut(hartree)= 4.000 => boxcut(ratio)= 2.16527
--------------------------------------------------------------------------------
-inwffil : will read wavefunctions from disk file t86o_DS1_WFK
================================================================================
prteigrs : about to open file t86o_DS2_EIG
SPIN UP channel
Non-SCF case, kpt 1 ( 0.25000 0.50000 0.00000), residuals and eigenvalues=
3.51E-21 2.55E-21 2.31E-21 2.86E-21 4.31E-21 5.58E-21
-1.1691E-01 -1.2785E-02 8.6753E-02 1.3604E-01 2.7709E-01 3.8967E-01
prteigrs : prtvol=0 or 1, do not print more k-points.
SPIN DOWN channel
Non-SCF case, kpt 1 ( 0.25000 0.50000 0.00000), residuals and eigenvalues=
3.51E-21 2.55E-21 2.31E-21 2.86E-21 4.31E-21 6.26E-21
-1.1691E-01 -1.2785E-02 8.6753E-02 1.3604E-01 2.7709E-01 3.8967E-01
prteigrs : prtvol=0 or 1, do not print more k-points.
--- !ResultsGS
iteration_state: {dtset: 2, }
comment : Summary of ground state results
lattice_vectors:
- [ 0.0000000, 5.1040000, 5.1040000, ]
- [ 5.1040000, 0.0000000, 5.1040000, ]
- [ 5.1040000, 5.1040000, 0.0000000, ]
lattice_lengths: [ 7.21815, 7.21815, 7.21815, ]
lattice_angles: [ 60.000, 60.000, 60.000, ] # degrees, (23, 13, 12)
lattice_volume: 2.6592673E+02
convergence: {deltae: 0.000E+00, res2: 0.000E+00, residm: 3.770E-21, diffor: 0.000E+00, }
etotal : -8.83230603E+00
entropy : 0.00000000E+00
fermie : 1.91786792E-01
cartesian_stress_tensor: null
pressure_GPa: null
xred :
- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Si]
- [ 2.5000E-01, 2.5000E-01, 2.5000E-01, Si]
cartesian_forces: null
force_length_stats: {min: null, max: null, mean: null, }
...
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 0.886964 0.886964 1.773927 -0.000000
2 2.00000 0.861280 0.861280 1.722560 -0.000000
---------------------------------------------------------------------
Sum: 1.748244 1.748244 3.496487 -0.000000
Total magnetization (from the atomic spheres): -0.000000
Total magnetization (exact up - dn): 0.000000
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 13.532E-22; max= 37.701E-22
reduced coordinates (array xred) for 2 atoms
0.000000000000 0.000000000000 0.000000000000
0.250000000000 0.250000000000 0.250000000000
cartesian coordinates (angstrom) at end:
1 0.00000000000000 0.00000000000000 0.00000000000000
2 1.35046023632168 1.35046023632168 1.35046023632168
length scales= 10.208000000000 10.208000000000 10.208000000000 bohr
= 5.401840945287 5.401840945287 5.401840945287 angstroms
prteigrs : about to open file t86o_DS2_EIG
Eigenvalues (hartree) for nkpt= 32 k points, SPIN UP:
kpt# 1, nband= 6, wtk= 0.03125, kpt= 0.2500 0.5000 0.0000 (reduced coord)
-0.11691 -0.01278 0.08675 0.13604 0.27709 0.38967
prteigrs : prtvol=0 or 1, do not print more k-points.
Eigenvalues (hartree) for nkpt= 32 k points, SPIN DOWN:
kpt# 1, nband= 6, wtk= 0.03125, kpt= 0.2500 0.5000 0.0000 (reduced coord)
-0.11691 -0.01278 0.08675 0.13604 0.27709 0.38967
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: 32, mband: 6, nsppol: 2, nspinor: 1, nspden: 2, mpw: 100, }
cutoff_energies: {ecut: 4.0, pawecutdg: -1.0, }
electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
mkfilename : getwfq/=0, take file _WFQ from output of DATASET 2.
mkfilename : getden/=0, take file _DEN from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
LDA: Perdew-Wang 92 LSD fit to Ceperley-Alder data - ixc=7
Citation for XC functional:
J.P.Perdew and Y.Wang, PRB 45, 13244 (1992)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 0.0000000 5.1040000 5.1040000 G(1)= -0.0979624 0.0979624 0.0979624
R(2)= 5.1040000 0.0000000 5.1040000 G(2)= 0.0979624 -0.0979624 0.0979624
R(3)= 5.1040000 5.1040000 0.0000000 G(3)= 0.0979624 0.0979624 -0.0979624
Unit cell volume ucvol= 2.6592673E+02 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= 15 15 15
ecut(hartree)= 4.000 => boxcut(ratio)= 2.00338
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 1 ipert= 1
2) idir= 2 ipert= 1
================================================================================
The perturbation idir= 3 ipert= 1 is
symmetric of a previously calculated perturbation.
So, its SCF calculation is not needed.
The perturbation idir= 1 ipert= 2 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.
--------------------------------------------------------------------------------
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 20 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 12, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 309.41101229731 2.341E+02 1.273E-01 3.887E+05
ETOT 2 333.12419273142 2.371E+01 2.277E-01 3.972E+05
ETOT 3 8.7156717001474 -3.244E+02 8.635E-02 9.351E+02
ETOT 4 7.8789828593392 -8.367E-01 2.675E-04 2.351E+01
ETOT 5 7.8639248451612 -1.506E-02 3.345E-06 3.276E-01
ETOT 6 7.8636245377513 -3.003E-04 7.791E-08 2.580E-03
ETOT 7 7.8636217044829 -2.833E-06 9.546E-10 8.061E-05
ETOT 8 7.8636215579224 -1.466E-07 5.484E-11 2.274E-06
ETOT 9 7.8636215560724 -1.850E-09 1.029E-12 6.916E-07
ETOT 10 7.8636215555268 -5.456E-10 2.078E-13 3.079E-08
ETOT 11 7.8636215554997 -2.709E-11 7.487E-15 1.736E-10
ETOT 12 7.8636215554995 -1.705E-13 7.313E-17 1.228E-11
scprqt: WARNING -
nstep= 12 was not enough SCF cycles to converge;
potential residual= 1.228E-11 exceeds tolvrs= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 32.035E-18; max= 73.128E-18
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 4.79157911E+01 eigvalue= -3.82754494E+00 local= -3.54807552E+01
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -8.13838805E+01 Hartree= 3.65378051E+01 xc= -5.68977429E+00
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 5.01632260E+00 enl0= 2.30188485E+01 enl1= -5.35975061E+01
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -6.74906937E+01
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 1.92943619E+00 fr.nonlo= 3.66341807E+01 Ewald= 3.75947576E+01
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -7.99460425E+00 frxc 2 = 7.19054499E+00
Resulting in :
2DEtotal= 0.7863621555E+01 Ha. Also 2DEtotal= 0.213980024676E+03 eV
(2DErelax= -6.7490693674E+01 Ha. 2DEnonrelax= 7.5354315229E+01 Ha)
( non-var. 2DEtotal : 7.8636219308E+00 Ha)
--------------------------------------------------------------------------------
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.
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 12, nline: 4, wfoptalg: 0, }
tolerances: {tolvrs: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 20.673853624686 -3.201E+01 3.945E-02 6.882E+03
ETOT 2 7.8951949563015 -1.278E+01 9.167E-03 5.520E+02
ETOT 3 6.7146915844441 -1.181E+00 4.448E-04 5.431E-01
ETOT 4 6.7137927910258 -8.988E-04 4.807E-07 5.975E-02
ETOT 5 6.7137487666687 -4.402E-05 3.119E-08 2.489E-02
ETOT 6 6.7137282277292 -2.054E-05 6.934E-09 2.421E-04
ETOT 7 6.7137280220207 -2.057E-07 6.756E-11 1.286E-06
ETOT 8 6.7137280209005 -1.120E-09 5.593E-13 1.170E-07
ETOT 9 6.7137280207996 -1.009E-10 4.392E-14 8.291E-10
ETOT 10 6.7137280207990 -5.329E-13 7.144E-16 2.886E-10
ETOT 11 6.7137280207988 -2.487E-13 1.384E-16 3.722E-11
ETOT 12 6.7137280207988 6.395E-14 1.106E-17 2.889E-13
At SCF step 12 vres2 = 2.89E-13 < tolvrs= 1.00E-12 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 24.526E-19; max= 11.055E-18
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 4.57534498E+01 eigvalue= -3.03988241E+00 local= -3.35433019E+01
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -3.70288127E+01 Hartree= 1.56805791E+01 xc= -5.38952042E+00
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 4.62614768E+00 enl0= 2.18876156E+01 enl1= -5.49213623E+01
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -4.59750875E+01
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 1.92943619E+00 fr.nonlo= 3.66341807E+01 Ewald= 1.49292575E+01
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = -7.99460383E+00 frxc 2 = 7.19054499E+00
Resulting in :
2DEtotal= 0.6713728021E+01 Ha. Also 2DEtotal= 0.182689830306E+03 eV
(2DErelax= -4.5975087512E+01 Ha. 2DEnonrelax= 5.2688815533E+01 Ha)
( non-var. 2DEtotal : 6.7137280400E+00 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 7.8636251013 -0.0000000251
1 1 2 1 3.3568655579 0.0000000000
1 1 3 1 3.3568655579 0.0000000000
1 1 1 2 -1.6364308156 0.0000000002
1 1 2 2 -3.0504606134 0.0000000002
1 1 3 2 -3.0504606134 0.0000000002
2 1 1 1 3.3568655579 0.0000000000
2 1 2 1 6.7137311159 0.0000000000
2 1 3 1 3.3568655579 0.0000000000
2 1 1 2 -3.0504606134 0.0000000002
2 1 2 2 -6.1009212268 0.0000000004
2 1 3 2 -3.0504606134 0.0000000002
3 1 1 1 3.3568655579 0.0000000000
3 1 2 1 3.3568655579 0.0000000000
3 1 3 1 6.7137311159 0.0000000000
3 1 1 2 -3.0504606134 0.0000000002
3 1 2 2 -3.0504606134 0.0000000002
3 1 3 2 -6.1009212268 0.0000000004
1 2 1 1 -1.6364308156 0.0000000002
1 2 2 1 -3.0504606134 0.0000000002
1 2 3 1 -3.0504606134 0.0000000002
1 2 1 2 7.8636251013 -0.0000000251
1 2 2 2 3.3568655579 0.0000000000
1 2 3 2 3.3568655579 0.0000000000
2 2 1 1 -3.0504606134 0.0000000002
2 2 2 1 -6.1009212268 0.0000000004
2 2 3 1 -3.0504606134 0.0000000002
2 2 1 2 3.3568655579 0.0000000000
2 2 2 2 6.7137311159 0.0000000000
2 2 3 2 3.3568655579 0.0000000000
3 2 1 1 -3.0504606134 0.0000000002
3 2 2 1 -3.0504606134 0.0000000002
3 2 3 1 -6.1009212268 0.0000000004
3 2 1 2 3.3568655579 0.0000000000
3 2 2 2 3.3568655579 0.0000000000
3 2 3 2 6.7137311159 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 0.1398934703 -0.0000000002
1 1 2 1 -0.0110351052 0.0000000002
1 1 3 1 -0.0110351052 0.0000000002
1 1 1 2 -0.0742524922 0.0000000000
1 1 2 2 -0.0428440554 0.0000000000
1 1 3 2 -0.0428440554 0.0000000000
2 1 1 1 -0.0110351052 0.0000000002
2 1 2 1 0.1398934703 -0.0000000002
2 1 3 1 0.0110351052 -0.0000000002
2 1 1 2 -0.0428440554 0.0000000000
2 1 2 2 -0.0742524922 0.0000000000
2 1 3 2 0.0428440554 -0.0000000000
3 1 1 1 -0.0110351052 0.0000000002
3 1 2 1 0.0110351052 -0.0000000002
3 1 3 1 0.1398934703 -0.0000000002
3 1 1 2 -0.0428440554 0.0000000000
3 1 2 2 0.0428440554 -0.0000000000
3 1 3 2 -0.0742524922 0.0000000000
1 2 1 1 -0.0742524922 0.0000000000
1 2 2 1 -0.0428440554 0.0000000000
1 2 3 1 -0.0428440554 0.0000000000
1 2 1 2 0.1398934703 -0.0000000002
1 2 2 2 -0.0110351052 0.0000000002
1 2 3 2 -0.0110351052 0.0000000002
2 2 1 1 -0.0428440554 0.0000000000
2 2 2 1 -0.0742524922 0.0000000000
2 2 3 1 0.0428440554 -0.0000000000
2 2 1 2 -0.0110351052 0.0000000002
2 2 2 2 0.1398934703 -0.0000000002
2 2 3 2 0.0110351052 -0.0000000002
3 2 1 1 -0.0428440554 0.0000000000
3 2 2 1 0.0428440554 -0.0000000000
3 2 3 1 -0.0742524922 0.0000000000
3 2 1 2 -0.0110351052 0.0000000002
3 2 2 2 0.0110351052 -0.0000000002
3 2 3 2 0.1398934703 -0.0000000002
Phonon wavevector (reduced coordinates) : 0.50000 0.00000 0.00000
Phonon energies in Hartree :
4.793096E-04 4.793096E-04 1.714698E-03 1.840359E-03 2.191829E-03
2.191829E-03
Phonon frequencies in cm-1 :
- 1.051963E+02 1.051963E+02 3.763327E+02 4.039121E+02 4.810508E+02
- 4.810508E+02
== END DATASET(S) ==============================================================
================================================================================
-outvars: echo values of variables after computation --------
acell 1.0208000000E+01 1.0208000000E+01 1.0208000000E+01 Bohr
amu 2.80855000E+01
asr 0
chneut 0
diemac 3.00000000E+00
ecut 4.00000000E+00 Hartree
etotal1 -8.8323060266E+00
etotal3 6.7137280208E+00
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
getden1 0
getden2 1
getden3 1
getwfk1 0
getwfk2 1
getwfk3 1
getwfq1 0
getwfq2 0
getwfq3 2
iscf1 7
iscf2 -2
iscf3 7
ixc 7
jdtset 1 2 3
kpt1 -2.50000000E-01 5.00000000E-01 0.00000000E+00
-2.50000000E-01 0.00000000E+00 0.00000000E+00
kpt2 -2.50000000E-01 5.00000000E-01 0.00000000E+00
5.00000000E-01 -2.50000000E-01 0.00000000E+00
-2.50000000E-01 -2.50000000E-01 2.50000000E-01
-2.50000000E-01 0.00000000E+00 0.00000000E+00
5.00000000E-01 2.50000000E-01 0.00000000E+00
-2.50000000E-01 2.50000000E-01 2.50000000E-01
2.50000000E-01 5.00000000E-01 0.00000000E+00
5.00000000E-01 5.00000000E-01 2.50000000E-01
-2.50000000E-01 5.00000000E-01 5.00000000E-01
0.00000000E+00 -2.50000000E-01 0.00000000E+00
2.50000000E-01 -2.50000000E-01 2.50000000E-01
5.00000000E-01 -2.50000000E-01 5.00000000E-01
-2.50000000E-01 -2.50000000E-01 -2.50000000E-01
2.50000000E-01 0.00000000E+00 0.00000000E+00
5.00000000E-01 0.00000000E+00 2.50000000E-01
-2.50000000E-01 0.00000000E+00 5.00000000E-01
0.00000000E+00 2.50000000E-01 0.00000000E+00
2.50000000E-01 2.50000000E-01 2.50000000E-01
5.00000000E-01 2.50000000E-01 5.00000000E-01
-2.50000000E-01 2.50000000E-01 -2.50000000E-01
0.00000000E+00 5.00000000E-01 2.50000000E-01
2.50000000E-01 5.00000000E-01 5.00000000E-01
5.00000000E-01 5.00000000E-01 -2.50000000E-01
0.00000000E+00 -2.50000000E-01 5.00000000E-01
2.50000000E-01 -2.50000000E-01 -2.50000000E-01
0.00000000E+00 0.00000000E+00 2.50000000E-01
2.50000000E-01 0.00000000E+00 5.00000000E-01
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0.00000000E+00 2.50000000E-01 5.00000000E-01
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0.00000000E+00 5.00000000E-01 -2.50000000E-01
0.00000000E+00 0.00000000E+00 -2.50000000E-01
kpt3 -2.50000000E-01 5.00000000E-01 0.00000000E+00
5.00000000E-01 -2.50000000E-01 0.00000000E+00
-2.50000000E-01 -2.50000000E-01 2.50000000E-01
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5.00000000E-01 2.50000000E-01 0.00000000E+00
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5.00000000E-01 -2.50000000E-01 5.00000000E-01
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5.00000000E-01 0.00000000E+00 2.50000000E-01
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0.00000000E+00 -2.50000000E-01 5.00000000E-01
2.50000000E-01 -2.50000000E-01 -2.50000000E-01
0.00000000E+00 0.00000000E+00 2.50000000E-01
2.50000000E-01 0.00000000E+00 5.00000000E-01
5.00000000E-01 0.00000000E+00 -2.50000000E-01
0.00000000E+00 2.50000000E-01 5.00000000E-01
2.50000000E-01 2.50000000E-01 -2.50000000E-01
0.00000000E+00 5.00000000E-01 -2.50000000E-01
0.00000000E+00 0.00000000E+00 -2.50000000E-01
kptopt1 1
kptopt2 3
kptopt3 3
kptrlatt 2 -2 2 -2 2 2 -2 -2 2
kptrlen 2.04160000E+01
P mkmem1 2
P mkmem2 32
P mkmem3 32
P mkqmem1 2
P mkqmem2 32
P mkqmem3 32
P mk1mem1 2
P mk1mem2 32
P mk1mem3 32
natom 2
nband1 6
nband2 6
nband3 6
nbdbuf 2
ndtset 3
ngfft 15 15 15
nkpt1 2
nkpt2 32
nkpt3 32
nqpt1 0
nqpt2 1
nqpt3 1
nspden 2
nsppol 2
nstep 12
nsym 48
ntypat 1
occ1 1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
occ3 1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 0.000000 0.000000
optdriver1 0
optdriver2 0
optdriver3 1
prtpot1 0
prtpot2 0
prtpot3 1
qpt1 0.00000000E+00 0.00000000E+00 0.00000000E+00
qpt2 5.00000000E-01 0.00000000E+00 0.00000000E+00
qpt3 5.00000000E-01 0.00000000E+00 0.00000000E+00
rfphon1 0
rfphon2 0
rfphon3 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
shiftk 5.00000000E-01 5.00000000E-01 5.00000000E-01
spgroup 227
spinat 0.0000000000E+00 0.0000000000E+00 2.0000000000E+00
0.0000000000E+00 0.0000000000E+00 2.0000000000E+00
spinmagntarget 0.00000000E+00
strten1 1.9729560058E-04 1.9729560058E-04 1.9729560058E-04
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 -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
tnons 0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
0.0000000 0.0000000 0.0000000 0.2500000 0.2500000 0.2500000
tolvrs1 1.00000000E-20
tolvrs2 0.00000000E+00
tolvrs3 1.00000000E-12
tolwfr1 0.00000000E+00
tolwfr2 1.00000000E-20
tolwfr3 0.00000000E+00
typat 1 1
wtk1 0.75000 0.25000
wtk2 0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125
wtk3 0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125 0.03125 0.03125 0.03125 0.03125
0.03125 0.03125
xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
1.3504602363E+00 1.3504602363E+00 1.3504602363E+00
xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
2.5520000000E+00 2.5520000000E+00 2.5520000000E+00
xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
2.5000000000E-01 2.5000000000E-01 2.5000000000E-01
znucl 14.00000
================================================================================
- 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= 2.9 wall= 3.0
================================================================================
Calculation completed.
.Delivered 5 WARNINGs and 9 COMMENTs to log file.
+Overall time at end (sec) : cpu= 2.9 wall= 3.0