mirror of https://github.com/abinit/abinit.git
851 lines
39 KiB
Plaintext
851 lines
39 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 19h08 )
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- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/v3_t06/t06.abi
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- output file -> t06.abo
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- root for input files -> t06i
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- root for output files -> t06o
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DATASET 1 : space group P1 (# 1); Bravais aP (primitive triclinic)
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================================================================================
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Values of the parameters that define the memory need for DATASET 1.
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intxc = 0 ionmov = 0 iscf = 7 lmnmax = 1
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lnmax = 1 mgfft = 16 mpssoang = 1 mqgrid = 3001
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natom = 2 nloc_mem = 1 nspden = 1 nspinor = 1
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nsppol = 1 nsym = 1 n1xccc = 0 ntypat = 1
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occopt = 1 xclevel = 0
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- mband = 4 mffmem = 1 mkmem = 4
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mpw = 82 nfft = 4096 nkpt = 4
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================================================================================
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P This job should need less than 1.556 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 0.022 Mbytes ; DEN or POT disk file : 0.033 Mbytes.
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================================================================================
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DATASET 2 : space group P1 (# 1); Bravais aP (primitive triclinic)
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================================================================================
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Values of the parameters that define the memory need for DATASET 2 (RF).
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intxc = 0 iscf = 7 lmnmax = 1 lnmax = 1
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mgfft = 16 mpssoang = 1 mqgrid = 3001 natom = 2
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nloc_mem = 1 nspden = 1 nspinor = 1 nsppol = 1
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nsym = 1 n1xccc = 0 ntypat = 1 occopt = 1
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xclevel = 0
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- mband = 4 mffmem = 1 mkmem = 4
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- mkqmem = 4 mk1mem = 4 mpw = 82
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nfft = 4096 nkpt = 4
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================================================================================
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P This job should need less than 1.283 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 0.022 Mbytes ; DEN or POT disk file : 0.033 Mbytes.
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================================================================================
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DATASET 3 : space group P1 (# 1); Bravais aP (primitive triclinic)
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================================================================================
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Values of the parameters that define the memory need for DATASET 3 (RF).
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intxc = 0 iscf = 7 lmnmax = 1 lnmax = 1
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mgfft = 16 mpssoang = 1 mqgrid = 3001 natom = 2
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nloc_mem = 1 nspden = 1 nspinor = 1 nsppol = 1
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nsym = 1 n1xccc = 0 ntypat = 1 occopt = 1
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xclevel = 0
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- mband = 4 mffmem = 1 mkmem = 4
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- mkqmem = 4 mk1mem = 4 mpw = 82
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nfft = 4096 nkpt = 4
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================================================================================
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P This job should need less than 1.283 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 0.022 Mbytes ; DEN or POT disk file : 0.033 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 = 0
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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 1.0000000000E+01 1.0000000000E+01 1.0000000000E+01 Bohr
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amu 1.00000000E+00
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asr 0
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chneut 0
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diemac1 1.00000000E+06
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diemac2 1.00000000E+00
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diemac3 1.00000000E+00
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diemix1 1.00000000E+00
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diemix2 3.50000000E-01
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diemix3 3.50000000E-01
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dilatmx 1.10000000E+00
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ecut 1.20000000E+00 Hartree
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- fftalg 512
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getwfk1 0
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getwfk2 1
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getwfk3 1
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get1wf1 0
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get1wf2 0
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get1wf3 2
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ixc 0
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jdtset 1 2 3
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kpt 0.00000000E+00 0.00000000E+00 -3.75000000E-01
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0.00000000E+00 0.00000000E+00 -1.25000000E-01
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0.00000000E+00 0.00000000E+00 1.25000000E-01
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0.00000000E+00 0.00000000E+00 3.75000000E-01
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kptopt 0
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P mkmem 4
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P mkqmem 4
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P mk1mem 4
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natom 2
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nband 4
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ndtset 3
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ngfft 16 16 16
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nkpt 4
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nqpt1 0
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nqpt2 1
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nqpt3 1
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nstep1 30
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nstep2 12
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nstep3 30
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nsym 1
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ntypat 1
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occ 2.000000 2.000000 2.000000 2.000000
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optdriver1 0
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optdriver2 1
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optdriver3 1
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prtpot1 0
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prtpot2 1
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prtpot3 1
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rfatpol 2 2
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rfdir 0 0 1
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rfphon1 0
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rfphon2 1
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rfphon3 1
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spgroup 1
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tolwfr 1.00000000E-15
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typat 1 1
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wtk 0.25000 0.25000 0.25000 0.25000
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xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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0.0000000000E+00 0.0000000000E+00 1.5875316258E+00
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xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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0.0000000000E+00 0.0000000000E+00 3.0000000000E+00
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xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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0.0000000000E+00 0.0000000000E+00 3.0000000000E-01
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znucl 32.00000
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================================================================================
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chkinp: Checking input parameters for consistency, jdtset= 1.
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chkinp: Checking input parameters for consistency, jdtset= 2.
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chkinp: Checking input parameters for consistency, jdtset= 3.
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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: 2, nkpt: 4, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 82, }
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cutoff_energies: {ecut: 1.2, pawecutdg: -1.0, }
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electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
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meta: {optdriver: 0, ionmov: 0, optcell: 0, iscf: 7, paral_kgb: 0, }
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...
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Exchange-correlation functional for the present dataset will be:
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No xc applied (usually for testing) - ixc=0
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Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
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R(1)= 10.0000000 0.0000000 0.0000000 G(1)= 0.1000000 0.0000000 0.0000000
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R(2)= 0.0000000 10.0000000 0.0000000 G(2)= 0.0000000 0.1000000 0.0000000
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R(3)= 0.0000000 0.0000000 10.0000000 G(3)= 0.0000000 0.0000000 0.1000000
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Unit cell volume ucvol= 1.0000000E+03 bohr^3
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Angles (23,13,12)= 9.00000000E+01 9.00000000E+01 9.00000000E+01 degrees
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getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
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ecut(hartree)= 1.452 => boxcut(ratio)= 2.94966
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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= 3.158273 Hartrees makes boxcut=2
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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/32ge.SJ_mod
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- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/32ge.SJ_mod
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- Starkloff-Joannopoulos local psp ( !!! OLD : only for tests)
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- 32.00000 4.00000 900101 znucl, zion, pspdat
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5 3 0 0 700 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
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1.000000E-06 2.603367E-02 r1 and al (Hamman grid)
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0 0.000 0.000 0 1.0500000 l,e99.0,e99.9,nproj,rcpsp
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0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
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0.00000000000000 0.00000000000000 0.00000000000000 rchrg,fchrg,qchrg
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Note: local psp for atom with Z= 32.0
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pspatm : epsatm= 27.96404307
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--- l ekb(1:nproj) -->
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pspatm: atomic psp has been read and splines computed
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4.47424689E+02 ecore*ucvol(ha*bohr**3)
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--------------------------------------------------------------------------------
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_setup2: Arith. and geom. avg. npw (full set) are 81.500 81.498
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================================================================================
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--- !BeginCycle
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iteration_state: {dtset: 1, }
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solver: {iscf: 7, nstep: 30, nline: 4, wfoptalg: 0, }
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tolerances: {tolwfr: 1.00E-15, }
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...
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iter Etot(hartree) deltaE(h) residm vres2
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ETOT 1 -4.4806623370892 -4.481E+00 3.867E-04 1.008E+02
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ETOT 2 -4.7780975497327 -2.974E-01 8.599E-07 8.118E-01
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ETOT 3 -4.7793314156778 -1.234E-03 1.216E-06 1.373E-01
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ETOT 4 -4.7794392055794 -1.078E-04 6.502E-08 2.678E-02
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ETOT 5 -4.7794591124761 -1.991E-05 3.254E-08 8.190E-04
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ETOT 6 -4.7794606723846 -1.560E-06 1.343E-08 9.201E-05
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ETOT 7 -4.7794608644840 -1.921E-07 1.089E-09 6.553E-06
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ETOT 8 -4.7794608736285 -9.145E-09 8.224E-11 3.572E-07
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ETOT 9 -4.7794608747648 -1.136E-09 1.545E-11 5.724E-08
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ETOT 10 -4.7794608748330 -6.822E-11 2.113E-12 1.682E-08
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ETOT 11 -4.7794608748878 -5.472E-11 4.766E-13 2.175E-09
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ETOT 12 -4.7794608748821 5.697E-12 4.039E-13 2.512E-09
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ETOT 13 -4.7794608748984 -1.638E-11 1.692E-13 8.384E-11
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ETOT 14 -4.7794608748992 -7.123E-13 6.202E-15 6.643E-12
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ETOT 15 -4.7794608748991 2.132E-14 5.602E-15 1.968E-11
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ETOT 16 -4.7794608748991 2.132E-14 9.182E-16 1.176E-11
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At SCF step 16 max residual= 9.18E-16 < tolwfr= 1.00E-15 =>converged.
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Cartesian components of stress tensor (hartree/bohr^3)
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sigma(1 1)= 1.51864385E-04 sigma(3 2)= 8.12372125E-12
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sigma(2 2)= 1.51864376E-04 sigma(3 1)= -1.93076883E-10
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sigma(3 3)= -2.42283999E-03 sigma(2 1)= -5.34839437E-12
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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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- [ 10.0000000, 0.0000000, 0.0000000, ]
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- [ 0.0000000, 10.0000000, 0.0000000, ]
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- [ 0.0000000, 0.0000000, 10.0000000, ]
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lattice_lengths: [ 10.00000, 10.00000, 10.00000, ]
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lattice_angles: [ 90.000, 90.000, 90.000, ] # degrees, (23, 13, 12)
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lattice_volume: 1.0000000E+03
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convergence: {deltae: 2.132E-14, res2: 1.176E-11, residm: 9.182E-16, diffor: null, }
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etotal : -4.77946087E+00
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entropy : 0.00000000E+00
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fermie : 1.11308993E-01
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cartesian_stress_tensor: # hartree/bohr^3
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- [ 1.51864385E-04, -5.34839437E-12, -1.93076883E-10, ]
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- [ -5.34839437E-12, 1.51864376E-04, 8.12372125E-12, ]
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- [ -1.93076883E-10, 8.12372125E-12, -2.42283999E-03, ]
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pressure_GPa: 2.0782E+01
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xred :
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- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Ge]
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- [ 0.0000E+00, 0.0000E+00, 3.0000E-01, Ge]
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cartesian_forces: # hartree/bohr
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- [ 2.71109764E-08, 4.08138145E-09, -8.55922195E-01, ]
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- [ -2.71109764E-08, -4.08138145E-09, 8.55922195E-01, ]
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force_length_stats: {min: 8.55922195E-01, max: 8.55922195E-01, mean: 8.55922195E-01, }
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...
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Integrated electronic density in atomic spheres:
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------------------------------------------------
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Atom Sphere_radius Integrated_density
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1 2.00000 1.46256149
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2 2.00000 1.42238603
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================================================================================
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----iterations are completed or convergence reached----
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Mean square residual over all n,k,spin= 50.709E-17; max= 91.818E-17
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reduced coordinates (array xred) for 2 atoms
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0.000000000000 0.000000000000 0.000000000000
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0.000000000000 0.000000000000 0.300000000000
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rms dE/dt= 4.9417E+00; max dE/dt= 8.5592E+00; dE/dt below (all hartree)
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1 -0.000000234606 -0.000000107817 8.559221913855
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2 0.000000307614 -0.000000026189 -8.559221983163
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cartesian coordinates (angstrom) at end:
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1 0.00000000000000 0.00000000000000 0.00000000000000
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2 0.00000000000000 0.00000000000000 1.58753162577000
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cartesian forces (hartree/bohr) at end:
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1 0.00000002711098 0.00000000408138 -0.85592219485090
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2 -0.00000002711098 -0.00000000408138 0.85592219485090
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frms,max,avg= 4.9416691E-01 8.5592219E-01 -3.650E-09 6.700E-09 3.465E-09 h/b
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cartesian forces (eV/Angstrom) at end:
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1 0.00000139410234 0.00000020987305 -44.01328519125066
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2 -0.00000139410234 -0.00000020987305 44.01328519125066
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frms,max,avg= 2.5411082E+01 4.4013285E+01 -1.877E-07 3.445E-07 1.782E-07 e/A
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length scales= 10.000000000000 10.000000000000 10.000000000000 bohr
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= 5.291772085900 5.291772085900 5.291772085900 angstroms
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prteigrs : about to open file t06o_DS1_EIG
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Fermi (or HOMO) energy (hartree) = 0.11131 Average Vxc (hartree)= 0.00000
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Eigenvalues (hartree) for nkpt= 4 k points:
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kpt# 1, nband= 4, wtk= 0.25000, kpt= 0.0000 0.0000 -0.3750 (reduced coord)
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-0.17950 -0.00480 0.11131 0.11131
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prteigrs : prtvol=0 or 1, do not print more k-points.
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--- !EnergyTerms
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iteration_state : {dtset: 1, }
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comment : Components of total free energy in Hartree
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kinetic : 2.16285337327726E+00
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hartree : 1.92335229626557E+00
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xc : 0.00000000000000E+00
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Ewald energy : -3.40312010772530E+00
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psp_core : 4.47424689112462E-01
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local_psp : -5.90997112582911E+00
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non_local_psp : 0.00000000000000E+00
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total_energy : -4.77946087489912E+00
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total_energy_eV : -1.30055744510731E+02
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band_energy : 9.95868221187726E-02
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...
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Cartesian components of stress tensor (hartree/bohr^3)
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sigma(1 1)= 1.51864385E-04 sigma(3 2)= 8.12372125E-12
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sigma(2 2)= 1.51864376E-04 sigma(3 1)= -1.93076883E-10
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sigma(3 3)= -2.42283999E-03 sigma(2 1)= -5.34839437E-12
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-Cartesian components of stress tensor (GPa) [Pressure= 2.0782E+01 GPa]
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- sigma(1 1)= 4.46800373E+00 sigma(3 2)= 2.39008091E-07
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- sigma(2 2)= 4.46800345E+00 sigma(3 1)= -5.68051708E-06
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- sigma(3 3)= -7.12824015E+01 sigma(2 1)= -1.57355169E-07
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================================================================================
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== DATASET 2 ==================================================================
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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: 2, }
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dimensions: {natom: 2, nkpt: 4, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 82, }
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cutoff_energies: {ecut: 1.2, pawecutdg: -1.0, }
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electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
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meta: {optdriver: 1, rfphon: 1, }
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...
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mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
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Exchange-correlation functional for the present dataset will be:
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No xc applied (usually for testing) - ixc=0
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Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
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R(1)= 10.0000000 0.0000000 0.0000000 G(1)= 0.1000000 0.0000000 0.0000000
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R(2)= 0.0000000 10.0000000 0.0000000 G(2)= 0.0000000 0.1000000 0.0000000
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R(3)= 0.0000000 0.0000000 10.0000000 G(3)= 0.0000000 0.0000000 0.1000000
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Unit cell volume ucvol= 1.0000000E+03 bohr^3
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Angles (23,13,12)= 9.00000000E+01 9.00000000E+01 9.00000000E+01 degrees
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setup1 : take into account q-point for computing boxcut.
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getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
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ecut(hartree)= 1.452 => boxcut(ratio)= 2.94966
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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= 3.158273 Hartrees makes boxcut=2
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|
--------------------------------------------------------------------------------
|
|
|
|
|
|
==> initialize data related to q vector <==
|
|
|
|
The list of irreducible perturbations for this q vector is:
|
|
1) idir= 3 ipert= 2
|
|
|
|
================================================================================
|
|
|
|
--------------------------------------------------------------------------------
|
|
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
|
|
Perturbation : displacement of atom 2 along direction 3
|
|
The set of symmetries contains only one element for this perturbation.
|
|
symkpt : the number of k-points, thanks to the symmetries,
|
|
is reduced to 2 .
|
|
|
|
--------------------------------------------------------------------------------
|
|
|
|
--------------------------------------------------------------------------------
|
|
|
|
Initialisation of the first-order wave-functions :
|
|
ireadwf= 0
|
|
|
|
--- !BeginCycle
|
|
iteration_state: {dtset: 2, }
|
|
solver: {iscf: 7, nstep: 12, nline: 4, wfoptalg: 0, }
|
|
tolerances: {tolwfr: 1.00E-15, }
|
|
...
|
|
|
|
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
|
|
-ETOT 1 263.30335780052 9.921E+01 4.049E-02 2.149E+04
|
|
ETOT 2 132.79562679230 -1.305E+02 1.292E-02 2.153E+03
|
|
ETOT 3 118.43127830952 -1.436E+01 1.316E-03 6.631E+01
|
|
ETOT 4 118.03618880869 -3.951E-01 4.425E-05 1.282E+00
|
|
ETOT 5 118.03010126177 -6.088E-03 2.453E-06 5.967E-02
|
|
ETOT 6 118.02988561634 -2.156E-04 1.368E-07 3.906E-03
|
|
ETOT 7 118.02986268548 -2.293E-05 4.937E-09 5.092E-04
|
|
ETOT 8 118.02986138131 -1.304E-06 7.822E-10 7.966E-06
|
|
ETOT 9 118.02986134343 -3.788E-08 8.589E-12 4.245E-07
|
|
ETOT 10 118.02986134090 -2.538E-09 3.054E-13 1.227E-08
|
|
ETOT 11 118.02986134089 -5.215E-12 8.099E-15 3.304E-09
|
|
ETOT 12 118.02986134087 -1.739E-11 6.344E-15 2.047E-11
|
|
|
|
scprqt: WARNING -
|
|
nstep= 12 was not enough SCF cycles to converge;
|
|
maximum residual= 6.344E-15 exceeds tolwfr= 1.000E-15
|
|
|
|
================================================================================
|
|
|
|
----iterations are completed or convergence reached----
|
|
|
|
Mean square residual over all n,k,spin= 14.905E-16; max= 63.438E-16
|
|
|
|
Thirteen components of 2nd-order total energy (hartree) are
|
|
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
|
|
kin0= 3.45881758E+01 eigvalue= -4.07914911E+00 local= -9.04130077E+00
|
|
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
|
|
loc psp = -9.21176393E+01 Hartree= 2.45910941E+01 xc= 0.00000000E+00
|
|
note that "loc psp" includes a xc core correction that could be resolved
|
|
7,8,9: eventually, occupation + non-local contributions
|
|
edocc= 0.00000000E+00 enl0= 0.00000000E+00 enl1= 0.00000000E+00
|
|
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
|
|
erelax= -4.60588193E+01
|
|
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
|
|
fr.local= 3.30479060E+01 fr.nonlo= 0.00000000E+00 Ewald= 1.31040775E+02
|
|
13,14 Frozen wf xc core corrections (1) and (2)
|
|
frxc 1 = 0.00000000E+00 frxc 2 = 0.00000000E+00
|
|
Resulting in :
|
|
2DEtotal= 0.1180298613E+03 Ha. Also 2DEtotal= 0.321175586389E+04 eV
|
|
(2DErelax= -4.6058819343E+01 Ha. 2DEnonrelax= 1.6408868068E+02 Ha)
|
|
( non-var. 2DEtotal : 1.1802986102E+02 Ha)
|
|
|
|
================================================================================
|
|
|
|
---- first-order wavefunction calculations are completed ----
|
|
|
|
|
|
==> Compute Derivative Database <==
|
|
|
|
2nd-order matrix (non-cartesian coordinates, masses not included,
|
|
asr not included )
|
|
j1 j2 matrix element
|
|
dir pert dir pert real part imaginary part
|
|
|
|
1 1 3 2 -0.0000116616 0.0000000000
|
|
|
|
2 1 3 2 -0.0000015634 0.0000000000
|
|
|
|
3 1 3 2 -118.0298614703 -0.0000000000
|
|
|
|
1 2 3 2 0.0000122266 0.0000000000
|
|
|
|
2 2 3 2 0.0000024445 0.0000000000
|
|
|
|
3 2 1 1 -0.0000116616 -0.0000000000
|
|
3 2 2 1 -0.0000015634 -0.0000000000
|
|
3 2 3 1 -118.0298614703 0.0000000000
|
|
3 2 1 2 0.0000122266 0.0000000000
|
|
3 2 2 2 0.0000024445 0.0000000000
|
|
3 2 3 2 118.0298610190 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 3 2 -0.0000001166 0.0000000000
|
|
|
|
2 1 3 2 -0.0000000156 0.0000000000
|
|
|
|
3 1 3 2 -1.1802986147 -0.0000000000
|
|
|
|
1 2 3 2 0.0000001223 0.0000000000
|
|
|
|
2 2 3 2 0.0000000244 0.0000000000
|
|
|
|
3 2 1 1 -0.0000001166 -0.0000000000
|
|
3 2 2 1 -0.0000000156 -0.0000000000
|
|
3 2 3 1 -1.1802986147 0.0000000000
|
|
3 2 1 2 0.0000001223 0.0000000000
|
|
3 2 2 2 0.0000000244 0.0000000000
|
|
3 2 3 2 1.1802986102 0.0000000000
|
|
|
|
Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.00000
|
|
Phonon energies in Hartree :
|
|
0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00
|
|
2.544579E-02
|
|
Phonon frequencies in cm-1 :
|
|
- 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00
|
|
- 5.584705E+03
|
|
chkph3 : WARNING -
|
|
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
|
|
|
|
================================================================================
|
|
== DATASET 3 ==================================================================
|
|
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
|
|
|
|
|
|
--- !DatasetInfo
|
|
iteration_state: {dtset: 3, }
|
|
dimensions: {natom: 2, nkpt: 4, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 82, }
|
|
cutoff_energies: {ecut: 1.2, 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 : get1wf/=0, take file _1WF from output of DATASET 2.
|
|
|
|
Exchange-correlation functional for the present dataset will be:
|
|
No xc applied (usually for testing) - ixc=0
|
|
|
|
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
|
|
R(1)= 10.0000000 0.0000000 0.0000000 G(1)= 0.1000000 0.0000000 0.0000000
|
|
R(2)= 0.0000000 10.0000000 0.0000000 G(2)= 0.0000000 0.1000000 0.0000000
|
|
R(3)= 0.0000000 0.0000000 10.0000000 G(3)= 0.0000000 0.0000000 0.1000000
|
|
Unit cell volume ucvol= 1.0000000E+03 bohr^3
|
|
Angles (23,13,12)= 9.00000000E+01 9.00000000E+01 9.00000000E+01 degrees
|
|
setup1 : take into account q-point for computing boxcut.
|
|
|
|
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
|
|
ecut(hartree)= 1.452 => boxcut(ratio)= 2.94966
|
|
|
|
getcut : COMMENT -
|
|
Note that boxcut > 2.2 ; recall that boxcut=Gcut(box)/Gcut(sphere) = 2
|
|
is sufficient for exact treatment of convolution.
|
|
Such a large boxcut is a waste : you could raise ecut
|
|
e.g. ecut= 3.158273 Hartrees makes boxcut=2
|
|
|
|
--------------------------------------------------------------------------------
|
|
|
|
|
|
==> initialize data related to q vector <==
|
|
|
|
The list of irreducible perturbations for this q vector is:
|
|
1) idir= 3 ipert= 2
|
|
|
|
================================================================================
|
|
|
|
--------------------------------------------------------------------------------
|
|
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
|
|
Perturbation : displacement of atom 2 along direction 3
|
|
The set of symmetries contains only one element for this perturbation.
|
|
symkpt : the number of k-points, thanks to the symmetries,
|
|
is reduced to 2 .
|
|
|
|
--------------------------------------------------------------------------------
|
|
|
|
--------------------------------------------------------------------------------
|
|
|
|
Initialisation of the first-order wave-functions :
|
|
ireadwf= 1
|
|
|
|
--- !BeginCycle
|
|
iteration_state: {dtset: 3, }
|
|
solver: {iscf: 7, nstep: 30, nline: 4, wfoptalg: 0, }
|
|
tolerances: {tolwfr: 1.00E-15, }
|
|
...
|
|
|
|
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
|
|
-ETOT 1 118.02986134087 -4.606E+01 9.160E-16 7.622E-12
|
|
|
|
At SCF step 1 max residual= 9.16E-16 < tolwfr= 1.00E-15 =>converged.
|
|
================================================================================
|
|
|
|
----iterations are completed or convergence reached----
|
|
|
|
Mean square residual over all n,k,spin= 63.517E-17; max= 91.603E-17
|
|
|
|
Thirteen components of 2nd-order total energy (hartree) are
|
|
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
|
|
kin0= 3.45881757E+01 eigvalue= -4.07914894E+00 local= -9.04130113E+00
|
|
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
|
|
loc psp = -9.21176384E+01 Hartree= 2.45910934E+01 xc= 0.00000000E+00
|
|
note that "loc psp" includes a xc core correction that could be resolved
|
|
7,8,9: eventually, occupation + non-local contributions
|
|
edocc= 0.00000000E+00 enl0= 0.00000000E+00 enl1= 0.00000000E+00
|
|
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
|
|
erelax= -4.60588193E+01
|
|
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
|
|
fr.local= 3.30479060E+01 fr.nonlo= 0.00000000E+00 Ewald= 1.31040775E+02
|
|
13,14 Frozen wf xc core corrections (1) and (2)
|
|
frxc 1 = 0.00000000E+00 frxc 2 = 0.00000000E+00
|
|
Resulting in :
|
|
2DEtotal= 0.1180298613E+03 Ha. Also 2DEtotal= 0.321175586389E+04 eV
|
|
(2DErelax= -4.6058819343E+01 Ha. 2DEnonrelax= 1.6408868068E+02 Ha)
|
|
( non-var. 2DEtotal : 1.1802986150E+02 Ha)
|
|
|
|
================================================================================
|
|
|
|
---- first-order wavefunction calculations are completed ----
|
|
|
|
|
|
==> Compute Derivative Database <==
|
|
|
|
2nd-order matrix (non-cartesian coordinates, masses not included,
|
|
asr not included )
|
|
j1 j2 matrix element
|
|
dir pert dir pert real part imaginary part
|
|
|
|
1 1 3 2 -0.0000116607 0.0000000000
|
|
|
|
2 1 3 2 -0.0000015621 0.0000000000
|
|
|
|
3 1 3 2 -118.0298600694 -0.0000000000
|
|
|
|
1 2 3 2 0.0000122174 0.0000000000
|
|
|
|
2 2 3 2 0.0000024437 0.0000000000
|
|
|
|
3 2 1 1 -0.0000116607 -0.0000000000
|
|
3 2 2 1 -0.0000015621 -0.0000000000
|
|
3 2 3 1 -118.0298600694 0.0000000000
|
|
3 2 1 2 0.0000122174 0.0000000000
|
|
3 2 2 2 0.0000024437 0.0000000000
|
|
3 2 3 2 118.0298615021 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 3 2 -0.0000001166 0.0000000000
|
|
|
|
2 1 3 2 -0.0000000156 0.0000000000
|
|
|
|
3 1 3 2 -1.1802986007 -0.0000000000
|
|
|
|
1 2 3 2 0.0000001222 0.0000000000
|
|
|
|
2 2 3 2 0.0000000244 0.0000000000
|
|
|
|
3 2 1 1 -0.0000001166 -0.0000000000
|
|
3 2 2 1 -0.0000000156 -0.0000000000
|
|
3 2 3 1 -1.1802986007 0.0000000000
|
|
3 2 1 2 0.0000001222 0.0000000000
|
|
3 2 2 2 0.0000000244 0.0000000000
|
|
3 2 3 2 1.1802986150 0.0000000000
|
|
|
|
Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.00000
|
|
Phonon energies in Hartree :
|
|
0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00
|
|
2.544579E-02
|
|
Phonon frequencies in cm-1 :
|
|
- 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00
|
|
- 5.584705E+03
|
|
chkph3 : WARNING -
|
|
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
|
|
|
|
== END DATASET(S) ==============================================================
|
|
================================================================================
|
|
|
|
-outvars: echo values of variables after computation --------
|
|
acell 1.0000000000E+01 1.0000000000E+01 1.0000000000E+01 Bohr
|
|
amu 1.00000000E+00
|
|
asr 0
|
|
chneut 0
|
|
diemac1 1.00000000E+06
|
|
diemac2 1.00000000E+00
|
|
diemac3 1.00000000E+00
|
|
diemix1 1.00000000E+00
|
|
diemix2 3.50000000E-01
|
|
diemix3 3.50000000E-01
|
|
dilatmx 1.10000000E+00
|
|
ecut 1.20000000E+00 Hartree
|
|
etotal1 -4.7794608749E+00
|
|
etotal2 1.1802986134E+02
|
|
etotal3 1.1802986134E+02
|
|
fcart1 2.7110976447E-08 4.0813814526E-09 -8.5592219485E-01
|
|
-2.7110976447E-08 -4.0813814526E-09 8.5592219485E-01
|
|
fcart2 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
|
|
getwfk1 0
|
|
getwfk2 1
|
|
getwfk3 1
|
|
get1wf1 0
|
|
get1wf2 0
|
|
get1wf3 2
|
|
ixc 0
|
|
jdtset 1 2 3
|
|
kpt 0.00000000E+00 0.00000000E+00 -3.75000000E-01
|
|
0.00000000E+00 0.00000000E+00 -1.25000000E-01
|
|
0.00000000E+00 0.00000000E+00 1.25000000E-01
|
|
0.00000000E+00 0.00000000E+00 3.75000000E-01
|
|
kptopt 0
|
|
P mkmem 4
|
|
P mkqmem 4
|
|
P mk1mem 4
|
|
natom 2
|
|
nband 4
|
|
ndtset 3
|
|
ngfft 16 16 16
|
|
nkpt 4
|
|
nqpt1 0
|
|
nqpt2 1
|
|
nqpt3 1
|
|
nstep1 30
|
|
nstep2 12
|
|
nstep3 30
|
|
nsym 1
|
|
ntypat 1
|
|
occ 2.000000 2.000000 2.000000 2.000000
|
|
optdriver1 0
|
|
optdriver2 1
|
|
optdriver3 1
|
|
prtpot1 0
|
|
prtpot2 1
|
|
prtpot3 1
|
|
rfatpol 2 2
|
|
rfdir 0 0 1
|
|
rfphon1 0
|
|
rfphon2 1
|
|
rfphon3 1
|
|
spgroup 1
|
|
strten1 1.5186438546E-04 1.5186437598E-04 -2.4228399906E-03
|
|
8.1237212454E-12 -1.9307688349E-10 -5.3483943725E-12
|
|
strten2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
strten3 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
tolwfr 1.00000000E-15
|
|
typat 1 1
|
|
wtk 0.25000 0.25000 0.25000 0.25000
|
|
xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 1.5875316258E+00
|
|
xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 3.0000000000E+00
|
|
xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 3.0000000000E-01
|
|
znucl 32.00000
|
|
|
|
================================================================================
|
|
|
|
The spacegroup number, the magnetic point group, and/or the number of symmetries
|
|
have changed between the initial recognition based on the input file
|
|
and a postprocessing based on the final acell, rprim, and xred.
|
|
More details in the log file.
|
|
|
|
|
|
- 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).
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- Comment: Non-vanishing rfphon and/or rfelfd, in the norm-conserving case.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze1997
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-
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- [3] Dynamical matrices, Born effective charges, dielectric permittivity tensors, and ,
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- interatomic force constants from density-functional perturbation theory,
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- X. Gonze and C. Lee, Phys. Rev. B55, 10355 (1997).
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- 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).
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|
- A. Romero, D.C. Allan, B. Amadon, G. Antonius, T. Applencourt, L.Baguet,
|
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- J.Bieder, F.Bottin, J.Bouchet, E.Bousquet, F.Bruneval,
|
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- G.Brunin, D.Caliste, M.Cote,
|
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- 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
|
|
-
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- Proc. 0 individual time (sec): cpu= 0.4 wall= 0.5
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================================================================================
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Calculation completed.
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.Delivered 67 WARNINGs and 29 COMMENTs to log file.
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+Overall time at end (sec) : cpu= 0.4 wall= 0.5
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