mirror of https://github.com/abinit/abinit.git
832 lines
51 KiB
Plaintext
832 lines
51 KiB
Plaintext
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.Version 10.1.4.5 of ABINIT, released Sep 2024.
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.(MPI version, prepared for a x86_64_linux_gnu13.2 computer)
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.Copyright (C) 1998-2025 ABINIT group .
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ABINIT comes with ABSOLUTELY NO WARRANTY.
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It is free software, and you are welcome to redistribute it
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under certain conditions (GNU General Public License,
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see ~abinit/COPYING or http://www.gnu.org/copyleft/gpl.txt).
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ABINIT is a project of the Universite Catholique de Louvain,
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Corning Inc. and other collaborators, see ~abinit/doc/developers/contributors.txt .
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Please read https://docs.abinit.org/theory/acknowledgments for suggested
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acknowledgments of the ABINIT effort.
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For more information, see https://www.abinit.org .
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.Starting date : Fri 13 Sep 2024.
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- ( at 19h10 )
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- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/v5_t18/t18.abi
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- output file -> t18.abo
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- root for input files -> t18i
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- root for output files -> t18o
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Magnetic group, Shubnikov type IV
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Fedorov space group R-3 m (#166)
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Magnetic Bravais lattice hR_I (rhombohedral, centered magnetic, #31)
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================================================================================
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Values of the parameters that define the memory need of the present run
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intxc = 0 ionmov = 0 iscf = 17 lmnmax = 18
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lnmax = 6 mgfft = 24 mpssoang = 3 mqgrid = 3001
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natom = 4 nloc_mem = 2 nspden = 2 nspinor = 1
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nsppol = 1 nsym = 24 n1xccc = 1 ntypat = 2
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occopt = 1 xclevel = 2
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- mband = 30 mffmem = 1 mkmem = 20
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mpw = 103 nfft = 3456 nkpt = 20
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PAW method is used; the additional fine FFT grid is defined by:
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mgfftf= 32 nfftf = 8192
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================================================================================
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P This job should need less than 8.529 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 0.945 Mbytes ; DEN or POT disk file : 0.065 Mbytes.
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================================================================================
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--------------------------------------------------------------------------------
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------------- Echo of variables that govern the present computation ------------
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--------------------------------------------------------------------------------
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-
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- outvars: echo of selected default values
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- iomode0 = 0 , fftalg0 =512 , wfoptalg0 = 10
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-
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- outvars: echo of global parameters not present in the input file
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- max_nthreads = 0
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-
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-outvars: echo values of preprocessed input variables --------
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acell 7.9200000000E+00 7.9200000000E+00 7.9200000000E+00 Bohr
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amu 5.86900000E+01 1.59994000E+01
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chksymbreak 0
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ecut 4.00000000E+00 Hartree
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- fftalg 512
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ixc 11
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kpt 1.25000000E-01 1.25000000E-01 1.25000000E-01
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3.75000000E-01 1.25000000E-01 1.25000000E-01
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-3.75000000E-01 1.25000000E-01 1.25000000E-01
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-1.25000000E-01 1.25000000E-01 1.25000000E-01
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3.75000000E-01 3.75000000E-01 1.25000000E-01
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-3.75000000E-01 3.75000000E-01 1.25000000E-01
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-1.25000000E-01 3.75000000E-01 1.25000000E-01
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-3.75000000E-01 -3.75000000E-01 1.25000000E-01
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-1.25000000E-01 -3.75000000E-01 1.25000000E-01
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-1.25000000E-01 -1.25000000E-01 1.25000000E-01
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1.25000000E-01 1.25000000E-01 3.75000000E-01
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3.75000000E-01 1.25000000E-01 3.75000000E-01
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-3.75000000E-01 1.25000000E-01 3.75000000E-01
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-1.25000000E-01 1.25000000E-01 3.75000000E-01
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3.75000000E-01 3.75000000E-01 3.75000000E-01
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-3.75000000E-01 3.75000000E-01 3.75000000E-01
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-1.25000000E-01 3.75000000E-01 3.75000000E-01
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-3.75000000E-01 -3.75000000E-01 3.75000000E-01
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-1.25000000E-01 -3.75000000E-01 3.75000000E-01
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-1.25000000E-01 -1.25000000E-01 3.75000000E-01
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kptrlatt 4 0 0 0 4 0 0 0 4
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kptrlen 2.24011428E+01
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lexexch 2 -1
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P mkmem 20
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natom 4
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nband 30
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ngfft 12 12 24
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ngfftdg 16 16 32
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nkpt 20
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nspden 2
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nstep 70
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nsym 24
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ntypat 2
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occ 2.000000 2.000000 2.000000 2.000000 2.000000 2.000000
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2.000000 2.000000 2.000000 2.000000 2.000000 2.000000
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2.000000 2.000000 2.000000 2.000000 0.000000 0.000000
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0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
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0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
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pawecutdg 1.00000000E+01 Hartree
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rprim 0.0000000000E+00 5.0000000000E-01 5.0000000000E-01
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5.0000000000E-01 0.0000000000E+00 5.0000000000E-01
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1.0000000000E+00 1.0000000000E+00 0.0000000000E+00
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shiftk 5.00000000E-01 5.00000000E-01 5.00000000E-01
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spgroup 166
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spinat 0.0000000000E+00 0.0000000000E+00 1.0000000000E+00
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0.0000000000E+00 0.0000000000E+00 -1.0000000000E+00
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0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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symafm 1 -1 1 -1 1 -1 1 -1 1 -1
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1 -1 1 -1 1 -1 1 -1 1 -1
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1 -1 1 -1
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symrel 1 0 0 0 1 0 0 0 1 1 0 0 0 1 0 0 0 1
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-1 0 0 0 -1 0 0 0 -1 -1 0 0 0 -1 0 0 0 -1
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0 1 0 1 0 0 0 0 1 0 1 0 1 0 0 0 0 1
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0 -1 0 -1 0 0 0 0 -1 0 -1 0 -1 0 0 0 0 -1
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0 -1 0 1 -1 0 0 -2 1 0 -1 0 1 -1 0 0 -2 1
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0 1 0 -1 1 0 0 2 -1 0 1 0 -1 1 0 0 2 -1
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1 -1 0 0 -1 0 0 -2 1 1 -1 0 0 -1 0 0 -2 1
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-1 1 0 0 1 0 0 2 -1 -1 1 0 0 1 0 0 2 -1
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-1 1 0 -1 0 0 -2 0 1 -1 1 0 -1 0 0 -2 0 1
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1 -1 0 1 0 0 2 0 -1 1 -1 0 1 0 0 2 0 -1
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-1 0 0 -1 1 0 -2 0 1 -1 0 0 -1 1 0 -2 0 1
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1 0 0 1 -1 0 2 0 -1 1 0 0 1 -1 0 2 0 -1
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tnons 0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
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toldfe 1.00000000E-08 Hartree
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typat 1 1 2 2
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useexexch 1
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useylm 1
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wtk 0.03125 0.06250 0.06250 0.06250 0.03125 0.06250
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0.06250 0.03125 0.06250 0.03125 0.03125 0.06250
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0.06250 0.06250 0.03125 0.06250 0.06250 0.03125
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0.06250 0.03125
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xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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2.0955417460E+00 2.0955417460E+00 -2.0880793867E-33
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2.0955417460E+00 2.0955417460E+00 2.0955417460E+00
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4.1910834920E+00 4.1910834920E+00 2.0955417460E+00
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xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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3.9600000000E+00 3.9600000000E+00 -3.9458981845E-33
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3.9600000000E+00 3.9600000000E+00 3.9600000000E+00
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7.9200000000E+00 7.9200000000E+00 3.9600000000E+00
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xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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-2.7710718120E-17 2.7710718120E-17 5.0000000000E-01
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5.0000000000E-01 5.0000000000E-01 2.5000000000E-01
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5.0000000000E-01 5.0000000000E-01 7.5000000000E-01
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znucl 28.00000 8.00000
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================================================================================
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chkinp: Checking input parameters for consistency.
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================================================================================
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== DATASET 1 ==================================================================
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- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
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--- !DatasetInfo
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iteration_state: {dtset: 1, }
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dimensions: {natom: 4, nkpt: 20, mband: 30, nsppol: 1, nspinor: 1, nspden: 2, mpw: 103, }
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cutoff_energies: {ecut: 4.0, pawecutdg: 10.0, }
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electrons: {nelect: 3.20000000E+01, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
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meta: {optdriver: 0, ionmov: 0, optcell: 0, iscf: 17, paral_kgb: 0, }
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...
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Exchange-correlation functional for the present dataset will be:
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GGA: Perdew-Burke-Ernzerhof functional - ixc=11
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Citation for XC functional:
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J.P.Perdew, K.Burke, M.Ernzerhof, PRL 77, 3865 (1996)
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Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
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R(1)= 0.0000000 3.9600000 3.9600000 G(1)= -0.1262626 0.1262626 0.1262626
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R(2)= 3.9600000 0.0000000 3.9600000 G(2)= 0.1262626 -0.1262626 0.1262626
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R(3)= 7.9200000 7.9200000 0.0000000 G(3)= 0.0631313 0.0631313 -0.0631313
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Unit cell volume ucvol= 2.4839654E+02 bohr^3
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Angles (23,13,12)= 6.00000000E+01 6.00000000E+01 6.00000000E+01 degrees
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Coarse grid specifications (used for wave-functions):
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getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 12 12 24
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ecut(hartree)= 4.000 => boxcut(ratio)= 2.37999
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getcut : COMMENT -
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Note that boxcut > 2.2 ; recall that boxcut=Gcut(box)/Gcut(sphere) = 2
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is sufficient for exact treatment of convolution.
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Such a large boxcut is a waste : you could raise ecut
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e.g. ecut= 5.664374 Hartrees makes boxcut=2
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Fine grid specifications (used for densities):
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getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 32
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ecut(hartree)= 10.000 => boxcut(ratio)= 2.00699
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--- Pseudopotential description ------------------------------------------------
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- pspini: atom type 1 psp file is /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/28ni-gga.paw
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- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/28ni-gga.paw
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- Paw atomic data for element Ni - Generated by AtomPAW (N. Holzwarth) + AtomPAW2Abinit v3.1.1
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- 28.00000 10.00000 20070601 znucl, zion, pspdat
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7 11 2 0 1080 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
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Pseudopotential format is: paw3
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basis_size (lnmax)= 6 (lmn_size= 18), orbitals= 0 0 1 1 2 2
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Spheres core radius: rc_sph= 2.31080032
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4 radial meshes are used:
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- mesh 1: r(i)=AA*[exp(BB*(i-1))-1], size=1080 , AA= 0.29784E-03 BB= 0.83395E-02
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- mesh 2: r(i)=AA*[exp(BB*(i-1))-1], size=1075 , AA= 0.29784E-03 BB= 0.83395E-02
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- mesh 3: r(i)=AA*[exp(BB*(i-1))-1], size=1165 , AA= 0.29784E-03 BB= 0.83395E-02
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- mesh 4: r(i)=AA*[exp(BB*(i-1))-1], size=1250 , AA= 0.29784E-03 BB= 0.83395E-02
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Shapefunction is BESSEL type: shapef(r,l)=aa(1,l)*jl(q(1,l)*r)+aa(2,l)*jl(q(2,l)*r)
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Radius for shape functions = 2.00531667
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Radial grid used for partial waves is grid 1
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Radial grid used for projectors is grid 2
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Radial grid used for (t)core density is grid 3
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Radial grid used for Vloc is grid 4
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Compensation charge density is taken into account in XC energy/potential
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pspatm: atomic psp has been read and splines computed
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- pspini: atom type 2 psp file is /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/08o-gga.paw
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- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/08o-gga.paw
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- oxygen - PAW data extracted from US-psp (D.Vanderbilt) - generated by USpp2Abinit v2.2.1
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- 8.00000 6.00000 20070614 znucl, zion, pspdat
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7 11 1 0 489 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
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Pseudopotential format is: paw3
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basis_size (lnmax)= 4 (lmn_size= 8), orbitals= 0 0 1 1
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Spheres core radius: rc_sph= 1.11262345
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4 radial meshes are used:
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- mesh 1: r(i)=AA*[exp(BB*(i-1))-1], size= 489 , AA= 0.30984E-03 BB= 0.16949E-01
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- mesh 2: r(i)=AA*[exp(BB*(i-1))-1], size= 548 , AA= 0.30984E-03 BB= 0.16949E-01
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- mesh 3: r(i)=AA*[exp(BB*(i-1))-1], size= 506 , AA= 0.30984E-03 BB= 0.16949E-01
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- mesh 4: r(i)=AA*[exp(BB*(i-1))-1], size= 613 , AA= 0.30984E-03 BB= 0.16949E-01
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Shapefunction is BESSEL type: shapef(r,l)=aa(1,l)*jl(q(1,l)*r)+aa(2,l)*jl(q(2,l)*r)
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Radius for shape functions = sphere core radius
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Radial grid used for partial waves is grid 1
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Radial grid used for projectors is grid 2
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Radial grid used for (t)core density is grid 3
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Radial grid used for Vloc is grid 4
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Compensation charge density is taken into account in XC energy/potential
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pspatm: atomic psp has been read and splines computed
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9.20677178E+02 ecore*ucvol(ha*bohr**3)
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--------------------------------------------------------------------------------
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_setup2: Arith. and geom. avg. npw (full set) are 95.125 95.078
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******************************************
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PAW Local Exact exchange: PBE0
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******************************************
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================================================================================
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--- !BeginCycle
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iteration_state: {dtset: 1, }
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solver: {iscf: 17, nstep: 70, nline: 4, wfoptalg: 10, }
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tolerances: {toldfe: 1.00E-08, }
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...
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iter Etot(hartree) deltaE(h) residm nres2
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ETOT 1 -104.68701969414 -1.047E+02 6.274E-01 6.682E+01
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ETOT 2 -96.517789782979 8.169E+00 8.277E-03 3.291E+01
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ETOT 3 -96.226186927373 2.916E-01 1.807E-02 8.773E+00
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ETOT 4 -96.184191871957 4.200E-02 2.715E-03 8.893E-02
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ETOT 5 -96.191699999997 -7.508E-03 6.359E-03 5.531E-02
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ETOT 6 -96.176595813502 1.510E-02 2.592E-03 1.335E-02
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ETOT 7 -96.177423333236 -8.275E-04 1.484E-04 5.592E-03
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ETOT 8 -96.178474287314 -1.051E-03 9.426E-05 3.554E-03
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ETOT 9 -96.178181119429 2.932E-04 7.970E-05 1.284E-03
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ETOT 10 -96.178065204973 1.159E-04 1.034E-05 5.374E-05
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ETOT 11 -96.178059731627 5.473E-06 2.814E-06 1.826E-05
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ETOT 12 -96.178054088019 5.644E-06 1.810E-06 6.797E-06
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ETOT 13 -96.178042717382 1.137E-05 3.537E-07 1.082E-06
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ETOT 14 -96.178045015498 -2.298E-06 9.058E-08 6.342E-08
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ETOT 15 -96.178045699270 -6.838E-07 6.873E-08 2.884E-08
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ETOT 16 -96.178046500680 -8.014E-07 2.268E-08 2.030E-09
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ETOT 17 -96.178046709304 -2.086E-07 1.572E-08 8.104E-10
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ETOT 18 -96.178046796837 -8.753E-08 8.869E-09 8.768E-11
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ETOT 19 -96.178046838294 -4.146E-08 6.625E-09 2.089E-11
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ETOT 20 -96.178046829067 9.227E-09 3.737E-09 1.974E-12
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ETOT 21 -96.178046825016 4.051E-09 2.808E-09 9.139E-14
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At SCF step 21, etot is converged :
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for the second time, diff in etot= 4.051E-09 < toldfe= 1.000E-08
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Cartesian components of stress tensor (hartree/bohr^3)
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sigma(1 1)= 1.71785800E-01 sigma(3 2)= 8.70084642E-04
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sigma(2 2)= 1.71785800E-01 sigma(3 1)= 8.70084642E-04
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sigma(3 3)= 1.71785800E-01 sigma(2 1)= -8.70084642E-04
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--- !ResultsGS
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iteration_state: {dtset: 1, }
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comment : Summary of ground state results
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lattice_vectors:
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- [ 0.0000000, 3.9600000, 3.9600000, ]
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- [ 3.9600000, 0.0000000, 3.9600000, ]
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- [ 7.9200000, 7.9200000, 0.0000000, ]
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lattice_lengths: [ 5.60029, 5.60029, 11.20057, ]
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lattice_angles: [ 60.000, 60.000, 60.000, ] # degrees, (23, 13, 12)
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lattice_volume: 2.4839654E+02
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convergence: {deltae: 4.051E-09, res2: 9.139E-14, residm: 2.808E-09, diffor: null, }
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etotal : -9.61780468E+01
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entropy : 0.00000000E+00
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fermie : 6.98033863E-01
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cartesian_stress_tensor: # hartree/bohr^3
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- [ 1.71785800E-01, -8.70084642E-04, 8.70084642E-04, ]
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- [ -8.70084642E-04, 1.71785800E-01, 8.70084642E-04, ]
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- [ 8.70084642E-04, 8.70084642E-04, 1.71785800E-01, ]
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pressure_GPa: -5.0541E+03
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xred :
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- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Ni]
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- [ -2.7711E-17, 2.7711E-17, 5.0000E-01, Ni]
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- [ 5.0000E-01, 5.0000E-01, 2.5000E-01, O]
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- [ 5.0000E-01, 5.0000E-01, 7.5000E-01, O]
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cartesian_forces: # hartree/bohr
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- [ -0.00000000E+00, -0.00000000E+00, -0.00000000E+00, ]
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- [ -0.00000000E+00, -0.00000000E+00, -0.00000000E+00, ]
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- [ -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 2.31080 4.340398 4.340398 8.680796 0.000000
|
|
2 2.31080 4.340398 4.340398 8.680796 -0.000000
|
|
3 1.11262 1.097086 1.097086 2.194172 -0.000000
|
|
4 1.11262 1.097086 1.097086 2.194172 0.000000
|
|
---------------------------------------------------------------------
|
|
Sum: 10.874968 10.874968 21.749936 0.000000
|
|
Total magnetization (from the atomic spheres): 0.000000
|
|
Total magnetization (exact up - dn): -0.000000
|
|
|
|
PAW TEST:
|
|
==== Compensation charge inside spheres ============
|
|
The following values must be close to each other ...
|
|
Compensation charge over spherical meshes = 7.471541724939993
|
|
Compensation charge over fine fft grid = 7.471589908459454
|
|
|
|
==== Results concerning PAW augmentation regions ====
|
|
|
|
Total pseudopotential strength Dij (hartree):
|
|
Atom # 1 - Spin component 1
|
|
0.38845 0.03893 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00022 -0.00022 0.00000 -0.00022 ...
|
|
0.03893 9.26906 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00049 -0.00049 0.00000 -0.00049 ...
|
|
0.00000 0.00000 0.03012 0.00001 -0.00001 -0.13243 0.00020 -0.00020 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 0.00001 0.03012 0.00001 0.00020 -0.13243 0.00020 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.00001 0.00001 0.03012 -0.00020 0.00020 -0.13243 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.13243 0.00020 -0.00020 21.65964 0.00779 -0.00779 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 0.00020 -0.13243 0.00020 0.00779 21.65964 0.00779 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.00020 0.00020 -0.13243 -0.00779 0.00779 21.65964 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00022 0.00049 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 -0.70809 0.00021 0.00067 0.00021 ...
|
|
-0.00022 -0.00049 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00021 -0.70809 0.00034 -0.00021 ...
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00067 0.00034 -0.72112 0.00034 ...
|
|
-0.00022 -0.00049 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00021 -0.00021 0.00034 -0.70809 ...
|
|
... only 12 components have been written...
|
|
Atom # 1 - Spin component 2
|
|
0.38845 0.03893 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00022 -0.00022 0.00000 -0.00022 ...
|
|
0.03893 9.26906 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00049 -0.00049 0.00000 -0.00049 ...
|
|
0.00000 0.00000 0.03012 0.00001 -0.00001 -0.13243 0.00020 -0.00020 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 0.00001 0.03012 0.00001 0.00020 -0.13243 0.00020 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.00001 0.00001 0.03012 -0.00020 0.00020 -0.13243 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.13243 0.00020 -0.00020 21.65964 0.00779 -0.00779 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 0.00020 -0.13243 0.00020 0.00779 21.65964 0.00779 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.00020 0.00020 -0.13243 -0.00779 0.00779 21.65964 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00022 0.00049 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 -0.70809 0.00021 0.00067 0.00021 ...
|
|
-0.00022 -0.00049 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00021 -0.70809 0.00034 -0.00021 ...
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00067 0.00034 -0.72112 0.00034 ...
|
|
-0.00022 -0.00049 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00021 -0.00021 0.00034 -0.70809 ...
|
|
... only 12 components have been written...
|
|
Atom # 4 - Spin component 1
|
|
1.13865 1.81932 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
1.81932 2.90637 0.00000 0.00000 0.00000 -0.00000 0.00000 -0.00000
|
|
0.00000 0.00000 -0.49055 -0.00004 0.00004 -0.56202 -0.00006 0.00006
|
|
0.00000 0.00000 -0.00004 -0.49055 -0.00004 -0.00006 -0.56202 -0.00006
|
|
0.00000 0.00000 0.00004 -0.00004 -0.49055 0.00006 -0.00006 -0.56202
|
|
0.00000 -0.00000 -0.56202 -0.00006 0.00006 -0.60589 -0.00008 0.00008
|
|
0.00000 0.00000 -0.00006 -0.56202 -0.00006 -0.00008 -0.60589 -0.00008
|
|
0.00000 -0.00000 0.00006 -0.00006 -0.56202 0.00008 -0.00008 -0.60589
|
|
Atom # 4 - Spin component 2
|
|
1.13865 1.81932 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
1.81932 2.90637 0.00000 0.00000 0.00000 0.00000 -0.00000 0.00000
|
|
0.00000 0.00000 -0.49055 -0.00004 0.00004 -0.56202 -0.00006 0.00006
|
|
0.00000 0.00000 -0.00004 -0.49055 -0.00004 -0.00006 -0.56202 -0.00006
|
|
0.00000 0.00000 0.00004 -0.00004 -0.49055 0.00006 -0.00006 -0.56202
|
|
0.00000 0.00000 -0.56202 -0.00006 0.00006 -0.60589 -0.00008 0.00008
|
|
0.00000 -0.00000 -0.00006 -0.56202 -0.00006 -0.00008 -0.60589 -0.00008
|
|
0.00000 0.00000 0.00006 -0.00006 -0.56202 0.00008 -0.00008 -0.60589
|
|
|
|
|
|
Augmentation waves occupancies Rhoij:
|
|
Atom # 1 - Spin component 1
|
|
2.51692 -0.11082 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.01625 -0.01625 0.00000 -0.01625 ...
|
|
-0.11082 0.00575 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 -0.00081 0.00081 0.00000 0.00081 ...
|
|
0.00000 0.00000 2.90878 -0.00606 0.00606 -0.01544 0.00004 -0.00004 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.00606 2.90878 -0.00606 0.00004 -0.01544 0.00004 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 0.00606 -0.00606 2.90878 -0.00004 0.00004 -0.01544 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.01544 0.00004 -0.00004 0.00020 0.00000 -0.00000 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 0.00004 -0.01544 0.00004 0.00000 0.00020 0.00000 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.00004 0.00004 -0.01544 -0.00000 0.00000 0.00020 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.01625 -0.00081 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 1.02741 0.00437 0.00617 0.00437 ...
|
|
-0.01625 0.00081 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00437 1.02741 0.00309 -0.00437 ...
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00617 0.00309 1.03169 0.00309 ...
|
|
-0.01625 0.00081 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00437 -0.00437 0.00309 1.02741 ...
|
|
... only 12 components have been written...
|
|
Atom # 1 - Spin component 2
|
|
2.51692 -0.11082 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.01625 -0.01625 0.00000 -0.01625 ...
|
|
-0.11082 0.00575 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 -0.00081 0.00081 0.00000 0.00081 ...
|
|
0.00000 0.00000 2.90878 -0.00606 0.00606 -0.01544 0.00004 -0.00004 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.00606 2.90878 -0.00606 0.00004 -0.01544 0.00004 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 0.00606 -0.00606 2.90878 -0.00004 0.00004 -0.01544 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.01544 0.00004 -0.00004 0.00020 0.00000 -0.00000 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 0.00004 -0.01544 0.00004 0.00000 0.00020 0.00000 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.00000 0.00000 -0.00004 0.00004 -0.01544 -0.00000 0.00000 0.00020 0.00000 0.00000 0.00000 0.00000 ...
|
|
0.01625 -0.00081 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 1.02741 0.00437 0.00617 0.00437 ...
|
|
-0.01625 0.00081 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00437 1.02741 0.00309 -0.00437 ...
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00617 0.00309 1.03169 0.00309 ...
|
|
-0.01625 0.00081 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00437 -0.00437 0.00309 1.02741 ...
|
|
... only 12 components have been written...
|
|
Atom # 4 - Spin component 1
|
|
2.59756 -0.75121 -0.00000 0.00000 -0.00000 0.00000 -0.00000 0.00000
|
|
-0.75121 0.27822 0.00000 -0.00000 0.00000 -0.00000 0.00000 -0.00000
|
|
-0.00000 0.00000 2.42828 -0.01130 0.01130 -1.41718 0.00689 -0.00689
|
|
0.00000 -0.00000 -0.01130 2.42828 -0.01130 0.00689 -1.41718 0.00689
|
|
-0.00000 0.00000 0.01130 -0.01130 2.42828 -0.00689 0.00689 -1.41718
|
|
0.00000 -0.00000 -1.41718 0.00689 -0.00689 0.83057 -0.00422 0.00422
|
|
-0.00000 0.00000 0.00689 -1.41718 0.00689 -0.00422 0.83057 -0.00422
|
|
0.00000 -0.00000 -0.00689 0.00689 -1.41718 0.00422 -0.00422 0.83057
|
|
Atom # 4 - Spin component 2
|
|
2.59756 -0.75121 0.00000 -0.00000 0.00000 -0.00000 0.00000 -0.00000
|
|
-0.75121 0.27822 -0.00000 0.00000 -0.00000 0.00000 -0.00000 0.00000
|
|
0.00000 -0.00000 2.42828 -0.01130 0.01130 -1.41718 0.00689 -0.00689
|
|
-0.00000 0.00000 -0.01130 2.42828 -0.01130 0.00689 -1.41718 0.00689
|
|
0.00000 -0.00000 0.01130 -0.01130 2.42828 -0.00689 0.00689 -1.41718
|
|
-0.00000 0.00000 -1.41718 0.00689 -0.00689 0.83057 -0.00422 0.00422
|
|
0.00000 -0.00000 0.00689 -1.41718 0.00689 -0.00422 0.83057 -0.00422
|
|
-0.00000 0.00000 -0.00689 0.00689 -1.41718 0.00422 -0.00422 0.83057
|
|
|
|
"Local exact-exchange" part of augmentation waves occupancies Rhoij:
|
|
Atom # 1 - L=2 ONLY - Spin component 1
|
|
1.02741 0.00437 0.00617 0.00437 0.00000 0.05795 -0.00054 -0.00073 -0.00054 0.00000
|
|
0.00437 1.02741 0.00309 -0.00437 -0.00535 -0.00054 0.05795 -0.00036 0.00054 0.00063
|
|
0.00617 0.00309 1.03169 0.00309 0.00000 -0.00035 -0.00018 0.05508 -0.00018 0.00000
|
|
0.00437 -0.00437 0.00309 1.02741 0.00535 -0.00054 0.00054 -0.00036 0.05795 -0.00063
|
|
0.00000 -0.00535 0.00000 0.00535 1.03169 0.00000 0.00030 0.00000 -0.00030 0.05508
|
|
0.05795 -0.00054 -0.00035 -0.00054 0.00000 0.00439 -0.00008 -0.00012 -0.00008 0.00000
|
|
-0.00054 0.05795 -0.00018 0.00054 0.00030 -0.00008 0.00439 -0.00006 0.00008 0.00010
|
|
-0.00073 -0.00036 0.05508 -0.00036 0.00000 -0.00012 -0.00006 0.00648 -0.00006 0.00000
|
|
-0.00054 0.00054 -0.00018 0.05795 -0.00030 -0.00008 0.00008 -0.00006 0.00439 -0.00010
|
|
0.00000 0.00063 0.00000 -0.00063 0.05508 0.00000 0.00010 0.00000 -0.00010 0.00648
|
|
Atom # 1 - L=2 ONLY - Spin component 2
|
|
1.02741 0.00437 0.00617 0.00437 0.00000 0.05795 -0.00054 -0.00073 -0.00054 0.00000
|
|
0.00437 1.02741 0.00309 -0.00437 -0.00535 -0.00054 0.05795 -0.00036 0.00054 0.00063
|
|
0.00617 0.00309 1.03169 0.00309 0.00000 -0.00035 -0.00018 0.05508 -0.00018 0.00000
|
|
0.00437 -0.00437 0.00309 1.02741 0.00535 -0.00054 0.00054 -0.00036 0.05795 -0.00063
|
|
0.00000 -0.00535 0.00000 0.00535 1.03169 0.00000 0.00030 0.00000 -0.00030 0.05508
|
|
0.05795 -0.00054 -0.00035 -0.00054 0.00000 0.00439 -0.00008 -0.00012 -0.00008 0.00000
|
|
-0.00054 0.05795 -0.00018 0.00054 0.00030 -0.00008 0.00439 -0.00006 0.00008 0.00010
|
|
-0.00073 -0.00036 0.05508 -0.00036 0.00000 -0.00012 -0.00006 0.00648 -0.00006 0.00000
|
|
-0.00054 0.00054 -0.00018 0.05795 -0.00030 -0.00008 0.00008 -0.00006 0.00439 -0.00010
|
|
0.00000 0.00063 0.00000 -0.00063 0.05508 0.00000 0.00010 0.00000 -0.00010 0.00648
|
|
Atom # 2 - L=2 ONLY - Spin component 1
|
|
1.02741 0.00437 0.00617 0.00437 0.00000 0.05795 -0.00054 -0.00073 -0.00054 0.00000
|
|
0.00437 1.02741 0.00309 -0.00437 -0.00535 -0.00054 0.05795 -0.00036 0.00054 0.00063
|
|
0.00617 0.00309 1.03169 0.00309 0.00000 -0.00035 -0.00018 0.05508 -0.00018 0.00000
|
|
0.00437 -0.00437 0.00309 1.02741 0.00535 -0.00054 0.00054 -0.00036 0.05795 -0.00063
|
|
0.00000 -0.00535 0.00000 0.00535 1.03169 0.00000 0.00030 0.00000 -0.00030 0.05508
|
|
0.05795 -0.00054 -0.00035 -0.00054 0.00000 0.00439 -0.00008 -0.00012 -0.00008 0.00000
|
|
-0.00054 0.05795 -0.00018 0.00054 0.00030 -0.00008 0.00439 -0.00006 0.00008 0.00010
|
|
-0.00073 -0.00036 0.05508 -0.00036 0.00000 -0.00012 -0.00006 0.00648 -0.00006 0.00000
|
|
-0.00054 0.00054 -0.00018 0.05795 -0.00030 -0.00008 0.00008 -0.00006 0.00439 -0.00010
|
|
0.00000 0.00063 0.00000 -0.00063 0.05508 0.00000 0.00010 0.00000 -0.00010 0.00648
|
|
Atom # 2 - L=2 ONLY - Spin component 2
|
|
1.02741 0.00437 0.00617 0.00437 0.00000 0.05795 -0.00054 -0.00073 -0.00054 0.00000
|
|
0.00437 1.02741 0.00309 -0.00437 -0.00535 -0.00054 0.05795 -0.00036 0.00054 0.00063
|
|
0.00617 0.00309 1.03169 0.00309 0.00000 -0.00035 -0.00018 0.05508 -0.00018 0.00000
|
|
0.00437 -0.00437 0.00309 1.02741 0.00535 -0.00054 0.00054 -0.00036 0.05795 -0.00063
|
|
0.00000 -0.00535 0.00000 0.00535 1.03169 0.00000 0.00030 0.00000 -0.00030 0.05508
|
|
0.05795 -0.00054 -0.00035 -0.00054 0.00000 0.00439 -0.00008 -0.00012 -0.00008 0.00000
|
|
-0.00054 0.05795 -0.00018 0.00054 0.00030 -0.00008 0.00439 -0.00006 0.00008 0.00010
|
|
-0.00073 -0.00036 0.05508 -0.00036 0.00000 -0.00012 -0.00006 0.00648 -0.00006 0.00000
|
|
-0.00054 0.00054 -0.00018 0.05795 -0.00030 -0.00008 0.00008 -0.00006 0.00439 -0.00010
|
|
0.00000 0.00063 0.00000 -0.00063 0.05508 0.00000 0.00010 0.00000 -0.00010 0.00648
|
|
|
|
---------- Exact Exchange ---------------------------------------------------
|
|
|
|
====== For Atom 1, occupations for correlated orbitals. l = 2
|
|
|
|
Occupation matrix for spin 1
|
|
0.62505 0.00638 0.00736 0.00638 0.00000
|
|
0.00638 0.62505 0.00368 -0.00638 -0.00637
|
|
0.00736 0.00368 0.69056 0.00368 0.00000
|
|
0.00638 -0.00638 0.00368 0.62505 0.00637
|
|
0.00000 -0.00637 0.00000 0.00637 0.69056
|
|
|
|
Occupation matrix for spin 2
|
|
0.62505 0.00638 0.00736 0.00638 0.00000
|
|
0.00638 0.62505 0.00368 -0.00638 -0.00637
|
|
0.00736 0.00368 0.69056 0.00368 0.00000
|
|
0.00638 -0.00638 0.00368 0.62505 0.00637
|
|
0.00000 -0.00637 0.00000 0.00637 0.69056
|
|
|
|
====== For Atom 2, occupations for correlated orbitals. l = 2
|
|
|
|
Occupation matrix for spin 1
|
|
0.62505 0.00638 0.00736 0.00638 0.00000
|
|
0.00638 0.62505 0.00368 -0.00638 -0.00637
|
|
0.00736 0.00368 0.69056 0.00368 0.00000
|
|
0.00638 -0.00638 0.00368 0.62505 0.00637
|
|
0.00000 -0.00637 0.00000 0.00637 0.69056
|
|
|
|
Occupation matrix for spin 2
|
|
0.62505 0.00638 0.00736 0.00638 0.00000
|
|
0.00638 0.62505 0.00368 -0.00638 -0.00637
|
|
0.00736 0.00368 0.69056 0.00368 0.00000
|
|
0.00638 -0.00638 0.00368 0.62505 0.00637
|
|
0.00000 -0.00637 0.00000 0.00637 0.69056
|
|
|
|
|
|
================================================================================
|
|
|
|
----iterations are completed or convergence reached----
|
|
|
|
Mean square residual over all n,k,spin= 76.220E-13; max= 28.076E-10
|
|
reduced coordinates (array xred) for 4 atoms
|
|
0.000000000000 0.000000000000 0.000000000000
|
|
-0.000000000000 0.000000000000 0.500000000000
|
|
0.500000000000 0.500000000000 0.250000000000
|
|
0.500000000000 0.500000000000 0.750000000000
|
|
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
|
|
3 0.000000000000 0.000000000000 0.000000000000
|
|
4 0.000000000000 0.000000000000 0.000000000000
|
|
|
|
cartesian coordinates (angstrom) at end:
|
|
1 0.00000000000000 0.00000000000000 0.00000000000000
|
|
2 2.09554174601640 2.09554174601640 -0.00000000000000
|
|
3 2.09554174601640 2.09554174601640 2.09554174601640
|
|
4 4.19108349203280 4.19108349203280 2.09554174601640
|
|
|
|
cartesian forces (hartree/bohr) at end:
|
|
1 -0.00000000000000 -0.00000000000000 -0.00000000000000
|
|
2 -0.00000000000000 -0.00000000000000 -0.00000000000000
|
|
3 -0.00000000000000 -0.00000000000000 -0.00000000000000
|
|
4 -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
|
|
3 -0.00000000000000 -0.00000000000000 -0.00000000000000
|
|
4 -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= 7.920000000000 7.920000000000 7.920000000000 bohr
|
|
= 4.191083492033 4.191083492033 4.191083492033 angstroms
|
|
prteigrs : about to open file t18o_EIG
|
|
Fermi (or HOMO) energy (hartree) = 0.69803 Average Vxc (hartree)= -0.50587
|
|
Eigenvalues (hartree) for nkpt= 20 k points:
|
|
kpt# 1, nband= 30, wtk= 0.03125, kpt= 0.1250 0.1250 0.1250 (reduced coord)
|
|
-0.62856 -0.57708 -0.08540 -0.06134 -0.04421 0.05816 0.06368 0.10469
|
|
0.12878 0.13930 0.21131 0.29645 0.32281 0.37442 0.39962 0.40030
|
|
0.49622 0.58424 0.69276 0.76020 0.87631 0.89456 0.90427 0.92570
|
|
0.92580 0.95067 1.02634 1.04487 1.05053 1.10364
|
|
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 : 3.30864489872339E+01
|
|
hartree : 9.76685710129448E+00
|
|
xc : -1.65899625884123E+01
|
|
Ewald energy : -9.52410591238850E+01
|
|
psp_core : 3.70648142959666E+00
|
|
local_psp : -5.39544389375535E+01
|
|
spherical_terms : 2.30476261691416E+01
|
|
total_energy : -9.61780469625842E+01
|
|
total_energy_eV : -2.61713775480399E+03
|
|
...
|
|
|
|
|
|
--- !EnergyTermsDC
|
|
iteration_state : {dtset: 1, }
|
|
comment : '"Double-counting" decomposition of free energy'
|
|
band_energy : 5.16479152698433E+00
|
|
Ewald energy : -9.52410591238850E+01
|
|
psp_core : 3.70648142959666E+00
|
|
xc_dc : -5.07508860027944E+00
|
|
spherical_terms : -4.73317205743244E+00
|
|
total_energy_dc : -9.61780468250159E+01
|
|
total_energy_dc_eV : -2.61713775106056E+03
|
|
...
|
|
|
|
|
|
Cartesian components of stress tensor (hartree/bohr^3)
|
|
sigma(1 1)= 1.71785800E-01 sigma(3 2)= 8.70084642E-04
|
|
sigma(2 2)= 1.71785800E-01 sigma(3 1)= 8.70084642E-04
|
|
sigma(3 3)= 1.71785800E-01 sigma(2 1)= -8.70084642E-04
|
|
|
|
-Cartesian components of stress tensor (GPa) [Pressure= -5.0541E+03 GPa]
|
|
- sigma(1 1)= 5.05411188E+03 sigma(3 2)= 2.55987697E+01
|
|
- sigma(2 2)= 5.05411188E+03 sigma(3 1)= 2.55987697E+01
|
|
- sigma(3 3)= 5.05411188E+03 sigma(2 1)= -2.55987697E+01
|
|
|
|
== END DATASET(S) ==============================================================
|
|
================================================================================
|
|
|
|
-outvars: echo values of variables after computation --------
|
|
acell 7.9200000000E+00 7.9200000000E+00 7.9200000000E+00 Bohr
|
|
amu 5.86900000E+01 1.59994000E+01
|
|
chksymbreak 0
|
|
ecut 4.00000000E+00 Hartree
|
|
etotal -9.6178046825E+01
|
|
fcart -0.0000000000E+00 -0.0000000000E+00 -0.0000000000E+00
|
|
-0.0000000000E+00 -0.0000000000E+00 -0.0000000000E+00
|
|
-0.0000000000E+00 -0.0000000000E+00 -0.0000000000E+00
|
|
-0.0000000000E+00 -0.0000000000E+00 -0.0000000000E+00
|
|
- fftalg 512
|
|
ixc 11
|
|
kpt 1.25000000E-01 1.25000000E-01 1.25000000E-01
|
|
3.75000000E-01 1.25000000E-01 1.25000000E-01
|
|
-3.75000000E-01 1.25000000E-01 1.25000000E-01
|
|
-1.25000000E-01 1.25000000E-01 1.25000000E-01
|
|
3.75000000E-01 3.75000000E-01 1.25000000E-01
|
|
-3.75000000E-01 3.75000000E-01 1.25000000E-01
|
|
-1.25000000E-01 3.75000000E-01 1.25000000E-01
|
|
-3.75000000E-01 -3.75000000E-01 1.25000000E-01
|
|
-1.25000000E-01 -3.75000000E-01 1.25000000E-01
|
|
-1.25000000E-01 -1.25000000E-01 1.25000000E-01
|
|
1.25000000E-01 1.25000000E-01 3.75000000E-01
|
|
3.75000000E-01 1.25000000E-01 3.75000000E-01
|
|
-3.75000000E-01 1.25000000E-01 3.75000000E-01
|
|
-1.25000000E-01 1.25000000E-01 3.75000000E-01
|
|
3.75000000E-01 3.75000000E-01 3.75000000E-01
|
|
-3.75000000E-01 3.75000000E-01 3.75000000E-01
|
|
-1.25000000E-01 3.75000000E-01 3.75000000E-01
|
|
-3.75000000E-01 -3.75000000E-01 3.75000000E-01
|
|
-1.25000000E-01 -3.75000000E-01 3.75000000E-01
|
|
-1.25000000E-01 -1.25000000E-01 3.75000000E-01
|
|
kptrlatt 4 0 0 0 4 0 0 0 4
|
|
kptrlen 2.24011428E+01
|
|
lexexch 2 -1
|
|
P mkmem 20
|
|
natom 4
|
|
nband 30
|
|
ngfft 12 12 24
|
|
ngfftdg 16 16 32
|
|
nkpt 20
|
|
nspden 2
|
|
nstep 70
|
|
nsym 24
|
|
ntypat 2
|
|
occ 2.000000 2.000000 2.000000 2.000000 2.000000 2.000000
|
|
2.000000 2.000000 2.000000 2.000000 2.000000 2.000000
|
|
2.000000 2.000000 2.000000 2.000000 0.000000 0.000000
|
|
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
|
|
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
|
|
pawecutdg 1.00000000E+01 Hartree
|
|
rprim 0.0000000000E+00 5.0000000000E-01 5.0000000000E-01
|
|
5.0000000000E-01 0.0000000000E+00 5.0000000000E-01
|
|
1.0000000000E+00 1.0000000000E+00 0.0000000000E+00
|
|
shiftk 5.00000000E-01 5.00000000E-01 5.00000000E-01
|
|
spgroup 166
|
|
spinat 0.0000000000E+00 0.0000000000E+00 1.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 -1.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
strten 1.7178580016E-01 1.7178580016E-01 1.7178580016E-01
|
|
8.7008464237E-04 8.7008464237E-04 -8.7008464237E-04
|
|
symafm 1 -1 1 -1 1 -1 1 -1 1 -1
|
|
1 -1 1 -1 1 -1 1 -1 1 -1
|
|
1 -1 1 -1
|
|
symrel 1 0 0 0 1 0 0 0 1 1 0 0 0 1 0 0 0 1
|
|
-1 0 0 0 -1 0 0 0 -1 -1 0 0 0 -1 0 0 0 -1
|
|
0 1 0 1 0 0 0 0 1 0 1 0 1 0 0 0 0 1
|
|
0 -1 0 -1 0 0 0 0 -1 0 -1 0 -1 0 0 0 0 -1
|
|
0 -1 0 1 -1 0 0 -2 1 0 -1 0 1 -1 0 0 -2 1
|
|
0 1 0 -1 1 0 0 2 -1 0 1 0 -1 1 0 0 2 -1
|
|
1 -1 0 0 -1 0 0 -2 1 1 -1 0 0 -1 0 0 -2 1
|
|
-1 1 0 0 1 0 0 2 -1 -1 1 0 0 1 0 0 2 -1
|
|
-1 1 0 -1 0 0 -2 0 1 -1 1 0 -1 0 0 -2 0 1
|
|
1 -1 0 1 0 0 2 0 -1 1 -1 0 1 0 0 2 0 -1
|
|
-1 0 0 -1 1 0 -2 0 1 -1 0 0 -1 1 0 -2 0 1
|
|
1 0 0 1 -1 0 2 0 -1 1 0 0 1 -1 0 2 0 -1
|
|
tnons 0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
0.0000000 0.0000000 0.0000000 -0.0000000 0.0000000 0.5000000
|
|
toldfe 1.00000000E-08 Hartree
|
|
typat 1 1 2 2
|
|
useexexch 1
|
|
useylm 1
|
|
wtk 0.03125 0.06250 0.06250 0.06250 0.03125 0.06250
|
|
0.06250 0.03125 0.06250 0.03125 0.03125 0.06250
|
|
0.06250 0.06250 0.03125 0.06250 0.06250 0.03125
|
|
0.06250 0.03125
|
|
xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
2.0955417460E+00 2.0955417460E+00 -2.0880793867E-33
|
|
2.0955417460E+00 2.0955417460E+00 2.0955417460E+00
|
|
4.1910834920E+00 4.1910834920E+00 2.0955417460E+00
|
|
xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
3.9600000000E+00 3.9600000000E+00 -3.9458981845E-33
|
|
3.9600000000E+00 3.9600000000E+00 3.9600000000E+00
|
|
7.9200000000E+00 7.9200000000E+00 3.9600000000E+00
|
|
xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
-2.7710718120E-17 2.7710718120E-17 5.0000000000E-01
|
|
5.0000000000E-01 5.0000000000E-01 2.5000000000E-01
|
|
5.0000000000E-01 5.0000000000E-01 7.5000000000E-01
|
|
znucl 28.00000 8.00000
|
|
|
|
================================================================================
|
|
|
|
|
|
- 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] Implementation of the Projector Augmented-Wave Method in the ABINIT code.
|
|
- M. Torrent, F. Jollet, F. Bottin, G. Zerah, and X. Gonze Comput. Mat. Science 42, 337, (2008).
|
|
- Comment: PAW calculations. Strong suggestion to cite this paper.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#torrent2008
|
|
-
|
|
- [2] 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
|
|
-
|
|
- [3] 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
|
|
-
|
|
- [4] 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
|
|
-
|
|
- And optionally:
|
|
-
|
|
- [5] ABINIT: First-principles approach of materials and nanosystem properties.
|
|
- Computer Phys. Comm. 180, 2582-2615 (2009).
|
|
- X. Gonze, B. Amadon, P.-M. Anglade, J.-M. Beuken, F. Bottin, P. Boulanger, F. Bruneval,
|
|
- D. Caliste, R. Caracas, M. Cote, T. Deutsch, L. Genovese, Ph. Ghosez, M. Giantomassi
|
|
- S. Goedecker, D.R. Hamann, P. Hermet, F. Jollet, G. Jomard, S. Leroux, M. Mancini, S. Mazevet,
|
|
- M.J.T. Oliveira, G. Onida, Y. Pouillon, T. Rangel, G.-M. Rignanese, D. Sangalli, R. Shaltaf,
|
|
- M. Torrent, M.J. Verstraete, G. Zerah, J.W. Zwanziger
|
|
- Comment: the third 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/ABINIT_CPC_v10.pdf .
|
|
- The licence allows the authors to put it on the Web.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze2009
|
|
-
|
|
- Proc. 0 individual time (sec): cpu= 6.3 wall= 6.3
|
|
|
|
================================================================================
|
|
|
|
Calculation completed.
|
|
.Delivered 0 WARNINGs and 3 COMMENTs to log file.
|
|
+Overall time at end (sec) : cpu= 6.3 wall= 6.3
|