mirror of https://github.com/abinit/abinit.git
716 lines
38 KiB
Plaintext
716 lines
38 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 19h09 )
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- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/v3_t54/t54.abi
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- output file -> t54.abo
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- root for input files -> t54i
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- root for output files -> t54o
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DATASET 1 : space group P4 m m (# 99); Bravais tP (primitive tetrag.)
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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 = 36 mpssoang = 1 mqgrid = 3001
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natom = 2 nloc_mem = 1 nspden = 1 nspinor = 1
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nsppol = 1 nsym = 8 n1xccc = 0 ntypat = 2
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occopt = 1 xclevel = 3
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- mband = 1 mffmem = 1 mkmem = 1
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mpw = 777 nfft = 32400 nkpt = 1
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================================================================================
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P This job should need less than 10.294 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 0.014 Mbytes ; DEN or POT disk file : 0.249 Mbytes.
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================================================================================
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DATASET 2 : space group P4 m m (# 99); Bravais tP (primitive tetrag.)
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================================================================================
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Values of the parameters that define the memory need for DATASET 2.
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intxc = 0 ionmov = 0 iscf = -1 lmnmax = 1
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lnmax = 1 mgfft = 36 mpssoang = 1 mqgrid = 3242
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natom = 2 nloc_mem = 1 nspden = 1 nspinor = 1
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nsppol = 1 nsym = 8 n1xccc = 0 ntypat = 2
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occopt = 1 xclevel = 3
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- mband = 20 mffmem = 1 mkmem = 1
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mpw = 777 nfft = 32400 nkpt = 1
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For the susceptibility and dielectric matrices, or tddft :
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mgfft = 36 nbnd_in_blk= 6 nfft = 32400 npw = 12449
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================================================================================
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P This job should need less than 10.344 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 0.239 Mbytes ; DEN or POT disk file : 0.249 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 1.2000000000E+01 1.0000000000E+01 1.0000000000E+01 Bohr
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amu 4.00260200E+00 1.00794000E+00
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boxcenter 0.00000000E+00 0.00000000E+00 0.00000000E+00
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cellcharge 1.00000000E+00
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diecut1 2.20000000E+00 Hartree
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diecut2 3.60000000E+01 Hartree
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diemac 1.00000000E+00
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diemix 5.00000000E-01
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ecut 9.00000000E+00 Hartree
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- fftalg 512
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getden1 0
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getden2 1
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getwfk1 0
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getwfk2 1
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iscf1 7
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iscf2 -1
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istwfk 2
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ixc 20
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jdtset 1 2
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kptnrm 4.00000000E+00
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kptopt 0
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P mkmem 1
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natom 2
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nband1 1
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nband2 20
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ndtset 2
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ngfft 36 30 30
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nkpt 1
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nstep 25
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nsym 8
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ntypat 2
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occ1 2.000000
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occ2 2.000000 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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0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
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0.000000 0.000000
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spgroup 99
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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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1 0 0 0 0 1 0 1 0 1 0 0 0 0 1 0 -1 0
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1 0 0 0 0 -1 0 -1 0 1 0 0 0 0 -1 0 1 0
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tolwfr1 1.00000000E-22
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tolwfr2 1.00000000E-09
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typat 1 2
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xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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1.0583544172E+00 0.0000000000E+00 0.0000000000E+00
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xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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2.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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1.6666666667E-01 0.0000000000E+00 0.0000000000E+00
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znucl 2.00000 1.00000
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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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================================================================================
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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: 1, mband: 1, nsppol: 1, nspinor: 1, nspden: 1, mpw: 777, }
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cutoff_energies: {ecut: 9.0, pawecutdg: -1.0, }
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electrons: {nelect: 2.00000000E+00, charge: 1.00000000E+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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Fermi-Amaldi correction - ixc=20
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Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
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R(1)= 12.0000000 0.0000000 0.0000000 G(1)= 0.0833333 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= 1.2000000E+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= 36 30 30
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ecut(hartree)= 9.000 => boxcut(ratio)= 2.22144
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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= 11.103305 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/PseudosHGH_pwteter/2he.2.hgh
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- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/PseudosHGH_pwteter/2he.2.hgh
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- Hartwigsen-Goedecker-Hutter psp for He, from PRB58, 3641 (1998)
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- 2.00000 2.00000 10605 znucl, zion, pspdat
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3 1 0 0 2001 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
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rloc= 0.2000000
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cc1 = -9.1120230; cc2 = 1.6983680; cc3 = 0.0000000; cc4 = 0.0000000
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rrs = 0.0000000; h11s= 0.0000000; h22s= 0.0000000; h33s= 0.0000000
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- Local part computed in reciprocal space.
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pspatm : COMMENT -
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the projectors are not normalized,
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so that the KB energies are not consistent with
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definition in PRB44, 8503 (1991).
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However, this does not influence the results obtained hereafter.
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pspatm : epsatm= -0.00346443
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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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- pspini: atom type 2 psp file is /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/PseudosHGH_pwteter/1h.1.hgh
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- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/PseudosHGH_pwteter/1h.1.hgh
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- Hartwigsen-Goedecker-Hutter psp for H, from PRB58, 3641 (1998)
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- 1.00000 1.00000 10605 znucl, zion, pspdat
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3 1 0 0 2001 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
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rloc= 0.2000000
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cc1 = -4.1802370; cc2 = 0.7250750; cc3 = 0.0000000; cc4 = 0.0000000
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rrs = 0.0000000; h11s= 0.0000000; h22s= 0.0000000; h33s= 0.0000000
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- Local part computed in reciprocal space.
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pspatm : COMMENT -
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the projectors are not normalized,
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so that the KB energies are not consistent with
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definition in PRB44, 8503 (1991).
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However, this does not influence the results obtained hereafter.
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pspatm : epsatm= -0.00129784
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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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-1.42868343E-02 ecore*ucvol(ha*bohr**3)
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--------------------------------------------------------------------------------
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_setup2: Arith. and geom. avg. npw (full set) are 1553.000 1553.000
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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: 25, nline: 4, wfoptalg: 0, }
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tolerances: {tolwfr: 1.00E-22, }
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...
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iter Etot(hartree) deltaE(h) residm vres2
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ETOT 1 -2.4642005769193 -2.464E+00 8.322E-05 5.340E+01
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ETOT 2 -2.4680861694896 -3.886E-03 8.117E-10 1.244E+01
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ETOT 3 -2.4688555102607 -7.693E-04 7.808E-06 9.101E-03
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ETOT 4 -2.4688640764615 -8.566E-06 2.871E-08 2.839E-04
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ETOT 5 -2.4688642017814 -1.253E-07 2.082E-10 2.122E-05
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ETOT 6 -2.4688642218789 -2.010E-08 1.094E-10 6.505E-07
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ETOT 7 -2.4688642225229 -6.440E-10 2.864E-12 4.091E-09
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ETOT 8 -2.4688642225262 -3.303E-12 2.043E-14 2.209E-10
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ETOT 9 -2.4688642225262 -8.615E-14 4.170E-16 9.201E-13
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ETOT 10 -2.4688642225263 -9.681E-14 5.117E-18 5.847E-15
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ETOT 11 -2.4688642225262 1.261E-13 4.150E-20 7.458E-17
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ETOT 12 -2.4688642225262 -1.643E-14 7.833E-23 1.032E-18
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At SCF step 12 max residual= 7.83E-23 < tolwfr= 1.00E-22 =>converged.
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Cartesian components of stress tensor (hartree/bohr^3)
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sigma(1 1)= 5.35632977E-04 sigma(3 2)= 0.00000000E+00
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sigma(2 2)= 4.89876475E-04 sigma(3 1)= 0.00000000E+00
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sigma(3 3)= 4.89876475E-04 sigma(2 1)= 0.00000000E+00
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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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- [ 12.0000000, 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: [ 12.00000, 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: 1.2000000E+03
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convergence: {deltae: -1.643E-14, res2: 1.032E-18, residm: 7.833E-23, diffor: null, }
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etotal : -2.46886422E+00
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entropy : 0.00000000E+00
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fermie : -8.41187493E-01
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cartesian_stress_tensor: # hartree/bohr^3
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- [ 5.35632977E-04, 0.00000000E+00, 0.00000000E+00, ]
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- [ 0.00000000E+00, 4.89876475E-04, 0.00000000E+00, ]
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- [ 0.00000000E+00, 0.00000000E+00, 4.89876475E-04, ]
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pressure_GPa: -1.4861E+01
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xred :
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- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, He]
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- [ 1.6667E-01, 0.0000E+00, 0.0000E+00, H]
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cartesian_forces: # hartree/bohr
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- [ 3.78307541E-02, -0.00000000E+00, -0.00000000E+00, ]
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- [ -3.78307541E-02, -0.00000000E+00, -0.00000000E+00, ]
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force_length_stats: {min: 3.78307541E-02, max: 3.78307541E-02, mean: 3.78307541E-02, }
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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 1.80406349
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2 2.00000 0.93296351
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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= 78.334E-24; max= 78.334E-24
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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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0.166666666667 0.000000000000 0.000000000000
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rms dE/dt= 2.6210E-01; max dE/dt= 4.5397E-01; dE/dt below (all hartree)
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1 -0.453969049605 0.000000000000 0.000000000000
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2 0.453969049615 0.000000000000 0.000000000000
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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 1.05835441718000 0.00000000000000 0.00000000000000
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cartesian forces (hartree/bohr) at end:
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1 0.03783075413416 -0.00000000000000 -0.00000000000000
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2 -0.03783075413416 -0.00000000000000 -0.00000000000000
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frms,max,avg= 2.1841596E-02 3.7830754E-02 -4.079E-13 0.000E+00 0.000E+00 h/b
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cartesian forces (eV/Angstrom) at end:
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1 1.94533542969632 -0.00000000000000 -0.00000000000000
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2 -1.94533542969632 -0.00000000000000 -0.00000000000000
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frms,max,avg= 1.1231399E+00 1.9453354E+00 -2.098E-11 0.000E+00 0.000E+00 e/A
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length scales= 12.000000000000 10.000000000000 10.000000000000 bohr
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= 6.350126503080 5.291772085900 5.291772085900 angstroms
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prteigrs : about to open file t54o_DS1_EIG
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Fermi (or HOMO) energy (hartree) = -0.84119 Average Vxc (hartree)= -0.00000
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Eigenvalues (hartree) for nkpt= 1 k points:
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kpt# 1, nband= 1, wtk= 1.00000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
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-0.84119
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Calculation was performed for a charged system with PBC
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You may consider including the monopole correction to the total energy
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The correction is to be divided by the dielectric constant
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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 : 1.91090613077938E+00
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hartree : 1.21197445645396E+00
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xc : -6.05987228226978E-01
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Ewald energy : -1.80490102117720E-01
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psp_core : -1.19056952472076E-05
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local_psp : -4.80525557371963E+00
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non_local_psp : 0.00000000000000E+00
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total_energy : -2.46886422252623E+00
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total_energy_eV : -6.71812120573818E+01
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band_energy : -1.68237498650529E+00
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monopole_correction : 1.31961991697000E-01
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monopole_correction_eV: 3.59086841099720E+00
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...
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Cartesian components of stress tensor (hartree/bohr^3)
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sigma(1 1)= 5.35632977E-04 sigma(3 2)= 0.00000000E+00
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sigma(2 2)= 4.89876475E-04 sigma(3 1)= 0.00000000E+00
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sigma(3 3)= 4.89876475E-04 sigma(2 1)= 0.00000000E+00
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-Cartesian components of stress tensor (GPa) [Pressure= -1.4861E+01 GPa]
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- sigma(1 1)= 1.57588636E+01 sigma(3 2)= 0.00000000E+00
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- sigma(2 2)= 1.44126611E+01 sigma(3 1)= 0.00000000E+00
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- sigma(3 3)= 1.44126611E+01 sigma(2 1)= 0.00000000E+00
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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: 1, mband: 20, nsppol: 1, nspinor: 1, nspden: 1, mpw: 777, }
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cutoff_energies: {ecut: 9.0, pawecutdg: -1.0, }
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electrons: {nelect: 2.00000000E+00, charge: 1.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
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meta: {optdriver: 0, ionmov: 0, optcell: 0, iscf: -1, paral_kgb: 0, }
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...
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mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
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mkfilename : getden/=0, take file _DEN from output of DATASET 1.
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Exchange-correlation functional for the present dataset will be:
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Fermi-Amaldi correction - ixc=20
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Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
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R(1)= 12.0000000 0.0000000 0.0000000 G(1)= 0.0833333 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= 1.2000000E+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= 36 30 30
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ecut(hartree)= 9.000 => boxcut(ratio)= 2.22144
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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= 11.103305 Hartrees makes boxcut=2
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--------------------------------------------------------------------------------
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|
|
-inwffil : will read wavefunctions from disk file t54o_DS1_WFK
|
|
|
|
================================================================================
|
|
prteigrs : about to open file t54o_DS2_EIG
|
|
Non-SCF case, kpt 1 ( 0.00000 0.00000 0.00000), residuals and eigenvalues=
|
|
4.07E-22 8.20E-10 6.54E-11 4.70E-11 1.48E-10 1.46E-10 1.19E-10 3.33E-10
|
|
7.89E-10 3.75E-10 5.86E-10 1.32E-10 7.11E-10 7.31E-10 4.15E-10 9.43E-10
|
|
7.63E-10 4.82E-10 3.75E-10 7.84E-10
|
|
-8.4119E-01 -2.3131E-01 4.0895E-02 7.5172E-02 7.5172E-02 1.7601E-01
|
|
1.9930E-01 2.0860E-01 2.7392E-01 3.0779E-01 3.0779E-01 3.3066E-01
|
|
3.3066E-01 3.6508E-01 3.7052E-01 3.8866E-01 3.9109E-01 4.0162E-01
|
|
4.0162E-01 4.1022E-01
|
|
|
|
|
|
*** TDDFT : computation of excited states ***
|
|
Splitting of 20 states in 1 occupied states, and 19 unoccupied states,
|
|
giving 19 excitations.
|
|
|
|
Ground state total energy (Ha) : -2.46886422E+00
|
|
|
|
Kohn-Sham energy differences,
|
|
corresponding total energies and oscillator strengths (X,Y,Z and average)-
|
|
(oscillator strengths smaller than 1.e-6 are set to zero)
|
|
Transition (Ha) and (eV) Tot. Ene. (Ha) Aver XX YY ZZ
|
|
1-> 2 6.09874E-01 1.65955E+01 -1.85899E+00 4.2006E-01 1.26E+00 0.00E+00 0.00E+00
|
|
1-> 3 8.82083E-01 2.40027E+01 -1.58678E+00 3.0189E-02 9.06E-02 0.00E+00 0.00E+00
|
|
1-> 4 9.16359E-01 2.49354E+01 -1.55250E+00 3.4751E-01 0.00E+00 1.02E+00 2.32E-02
|
|
1-> 5 9.16359E-01 2.49354E+01 -1.55250E+00 3.4751E-01 0.00E+00 2.32E-02 1.02E+00
|
|
1-> 6 1.01720E+00 2.76794E+01 -1.45167E+00 6.3586E-03 1.91E-02 0.00E+00 0.00E+00
|
|
1-> 7 1.04049E+00 2.83130E+01 -1.42838E+00 0.0000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
1-> 8 1.04979E+00 2.85661E+01 -1.41908E+00 0.0000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
1-> 9 1.11511E+00 3.03437E+01 -1.35376E+00 3.3871E-02 1.02E-01 0.00E+00 0.00E+00
|
|
1-> 10 1.14897E+00 3.12652E+01 -1.31989E+00 2.0458E-02 0.00E+00 3.87E-02 2.27E-02
|
|
1-> 11 1.14897E+00 3.12652E+01 -1.31989E+00 2.0458E-02 0.00E+00 2.27E-02 3.86E-02
|
|
1-> 12 1.17184E+00 3.18875E+01 -1.29702E+00 4.8175E-02 0.00E+00 7.45E-02 7.00E-02
|
|
1-> 13 1.17184E+00 3.18875E+01 -1.29702E+00 4.8174E-02 0.00E+00 7.00E-02 7.45E-02
|
|
1-> 14 1.20627E+00 3.28243E+01 -1.26259E+00 0.0000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
1-> 15 1.21171E+00 3.29724E+01 -1.25715E+00 0.0000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
1-> 16 1.22984E+00 3.34658E+01 -1.23902E+00 0.0000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
1-> 17 1.23228E+00 3.35319E+01 -1.23659E+00 4.6170E-03 1.39E-02 0.00E+00 0.00E+00
|
|
1-> 18 1.24281E+00 3.38186E+01 -1.22605E+00 6.7316E-03 0.00E+00 1.64E-03 1.86E-02
|
|
1-> 19 1.24281E+00 3.38186E+01 -1.22605E+00 6.7316E-03 0.00E+00 1.86E-02 1.64E-03
|
|
1-> 20 1.25141E+00 3.40526E+01 -1.21745E+00 2.5412E-03 7.62E-03 0.00E+00 0.00E+00
|
|
Sum of osc. strength : 1.343376E+00
|
|
|
|
TDDFT singlet excitation energies (at most 20 of them are printed),
|
|
and corresponding total energies.
|
|
Excit# (Ha) and (eV) total energy (Ha) major contributions
|
|
1 6.96115E-01 1.89423E+01 -1.772749E+00 0.99( 1-> 2) 0.01( 1-> 7)
|
|
2 8.94269E-01 2.43343E+01 -1.574595E+00 1.00( 1-> 3) 0.00( 1-> 9)
|
|
3 9.44448E-01 2.56997E+01 -1.524417E+00 0.62( 1-> 4) 0.38( 1-> 5)
|
|
4 9.44448E-01 2.56997E+01 -1.524416E+00 0.62( 1-> 5) 0.38( 1-> 4)
|
|
5 1.02004E+00 2.77567E+01 -1.448825E+00 0.99( 1-> 6) 0.01( 1-> 7)
|
|
6 1.05074E+00 2.85921E+01 -1.418125E+00 1.00( 1-> 8) 0.00( 1-> 16)
|
|
7 1.05495E+00 2.87065E+01 -1.413919E+00 0.97( 1-> 7) 0.01( 1-> 6)
|
|
8 1.13054E+00 3.07635E+01 -1.338326E+00 0.99( 1-> 9) 0.00( 1-> 3)
|
|
9 1.15430E+00 3.14101E+01 -1.314563E+00 0.62( 1-> 10) 0.35( 1-> 11)
|
|
10 1.15430E+00 3.14102E+01 -1.314562E+00 0.62( 1-> 11) 0.35( 1-> 10)
|
|
11 1.18070E+00 3.21284E+01 -1.288168E+00 0.70( 1-> 13) 0.27( 1-> 12)
|
|
12 1.18070E+00 3.21284E+01 -1.288168E+00 0.70( 1-> 12) 0.27( 1-> 13)
|
|
13 1.20864E+00 3.28887E+01 -1.260227E+00 1.00( 1-> 14) 0.00( 1-> 17)
|
|
14 1.21191E+00 3.29777E+01 -1.256955E+00 1.00( 1-> 15) 0.00( 1-> 16)
|
|
15 1.23022E+00 3.34760E+01 -1.238643E+00 1.00( 1-> 16) 0.00( 1-> 15)
|
|
16 1.23865E+00 3.37054E+01 -1.230213E+00 0.95( 1-> 17) 0.05( 1-> 20)
|
|
17 1.24418E+00 3.38559E+01 -1.224682E+00 0.50( 1-> 19) 0.49( 1-> 18)
|
|
18 1.24418E+00 3.38559E+01 -1.224682E+00 0.50( 1-> 18) 0.49( 1-> 19)
|
|
19 1.26429E+00 3.44030E+01 -1.204579E+00 0.94( 1-> 20) 0.05( 1-> 17)
|
|
|
|
Oscillator strengths : (elements smaller than 1.e-6 are set to zero)
|
|
Excit# (Ha) Average XX YY ZZ XY XZ YZ
|
|
1 6.96115E-01 4.081E-01 1.224E+00 0.000E+00 0.000E+00 -1.50E-06 0.00E+00 0.00E+00
|
|
2 8.94269E-01 2.849E-02 8.547E-02 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
3 9.44448E-01 3.223E-01 0.000E+00 7.350E-01 2.321E-01 1.93E-06 1.08E-06 4.13E-01
|
|
4 9.44448E-01 3.223E-01 0.000E+00 2.321E-01 7.350E-01 -1.25E-06 2.22E-06 -4.13E-01
|
|
5 1.02004E+00 7.984E-03 2.395E-02 0.000E+00 0.000E+00 0.00E+00 -1.16E-06 0.00E+00
|
|
6 1.05074E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
7 1.05495E+00 3.838E-03 1.151E-02 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
8 1.13054E+00 3.993E-02 1.198E-01 0.000E+00 0.000E+00 -3.71E-06 2.21E-06 0.00E+00
|
|
9 1.15430E+00 1.493E-02 0.000E+00 3.156E-03 4.163E-02 0.00E+00 -1.43E-06 -1.15E-02
|
|
10 1.15430E+00 1.493E-02 0.000E+00 4.163E-02 3.156E-03 1.49E-06 0.00E+00 1.15E-02
|
|
11 1.18070E+00 7.417E-02 0.000E+00 2.095E-01 1.303E-02 1.39E-05 -3.46E-06 -5.22E-02
|
|
12 1.18070E+00 7.417E-02 0.000E+00 1.303E-02 2.095E-01 -1.32E-06 -5.28E-06 5.22E-02
|
|
13 1.20864E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
14 1.21191E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
15 1.23022E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
16 1.23865E+00 9.100E-03 2.730E-02 0.000E+00 0.000E+00 4.24E-06 -1.05E-06 0.00E+00
|
|
17 1.24418E+00 1.143E-02 0.000E+00 2.665E-02 7.625E-03 -5.65E-06 -3.02E-06 1.43E-02
|
|
18 1.24418E+00 1.143E-02 0.000E+00 7.625E-03 2.665E-02 -4.01E-06 7.51E-06 -1.43E-02
|
|
19 1.26429E+00 2.323E-04 6.969E-04 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
Sum of osc. strength : 1.343377E+00
|
|
Cauchy coeffs (au) : ( -2)-> 1.793E+00, ( -4)-> 2.734E+00, ( -6)-> 4.655E+00
|
|
(-8)-> 8.568E+00, (-10)-> 1.656E+01, (-12)-> 3.295E+01, (-14)-> 6.665E+01
|
|
|
|
TDDFT triplet excitation energies (at most 20 of them are printed),
|
|
and corresponding total energies.
|
|
Excit# (Ha) and (eV) total energy (Ha) major contributions
|
|
1 4.96899E-01 1.35213E+01 -1.971966E+00 0.99( 1-> 2) 0.00( 1-> 7)
|
|
2 8.67102E-01 2.35950E+01 -1.601762E+00 0.99( 1-> 3) 0.00( 1-> 9)
|
|
3 8.84458E-01 2.40673E+01 -1.584406E+00 0.66( 1-> 5) 0.33( 1-> 4)
|
|
4 8.84459E-01 2.40673E+01 -1.584406E+00 0.66( 1-> 4) 0.33( 1-> 5)
|
|
5 1.01343E+00 2.75769E+01 -1.455430E+00 0.95( 1-> 6) 0.05( 1-> 7)
|
|
6 1.02808E+00 2.79754E+01 -1.440787E+00 0.94( 1-> 7) 0.05( 1-> 6)
|
|
7 1.04883E+00 2.85400E+01 -1.420037E+00 1.00( 1-> 8) 0.00( 1-> 16)
|
|
8 1.10119E+00 2.99649E+01 -1.367676E+00 0.99( 1-> 9) 0.01( 1-> 7)
|
|
9 1.14296E+00 3.11014E+01 -1.325909E+00 0.62( 1-> 11) 0.36( 1-> 10)
|
|
10 1.14296E+00 3.11014E+01 -1.325908E+00 0.62( 1-> 10) 0.36( 1-> 11)
|
|
11 1.16537E+00 3.17112E+01 -1.303499E+00 0.71( 1-> 12) 0.26( 1-> 13)
|
|
12 1.16537E+00 3.17112E+01 -1.303498E+00 0.71( 1-> 13) 0.26( 1-> 12)
|
|
13 1.20390E+00 3.27597E+01 -1.264966E+00 1.00( 1-> 14) 0.00( 1-> 17)
|
|
14 1.21151E+00 3.29670E+01 -1.257350E+00 1.00( 1-> 15) 0.00( 1-> 16)
|
|
15 1.22525E+00 3.33408E+01 -1.243613E+00 0.95( 1-> 17) 0.05( 1-> 20)
|
|
16 1.22947E+00 3.34556E+01 -1.239392E+00 1.00( 1-> 16) 0.00( 1-> 15)
|
|
17 1.24185E+00 3.37924E+01 -1.227016E+00 0.77( 1-> 19) 0.23( 1-> 18)
|
|
18 1.24185E+00 3.37924E+01 -1.227016E+00 0.77( 1-> 18) 0.23( 1-> 19)
|
|
19 1.24320E+00 3.38292E+01 -1.225665E+00 0.95( 1-> 20) 0.05( 1-> 17)
|
|
|
|
Oscillator strengths : (elements smaller than 1.e-6 are set to zero)
|
|
Excit# (Ha) Average XX YY ZZ XY XZ YZ
|
|
1 4.96899E-01 4.225E-01 1.267E+00 0.000E+00 0.000E+00 2.30E-06 0.00E+00 0.00E+00
|
|
2 8.67102E-01 3.478E-02 1.044E-01 0.000E+00 0.000E+00 1.14E-06 0.00E+00 0.00E+00
|
|
3 8.84458E-01 3.676E-01 0.000E+00 2.225E-01 8.804E-01 0.00E+00 0.00E+00 -4.43E-01
|
|
4 8.84459E-01 3.676E-01 0.000E+00 8.804E-01 2.225E-01 0.00E+00 0.00E+00 4.43E-01
|
|
5 1.01343E+00 3.122E-03 9.365E-03 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
6 1.02808E+00 3.496E-03 1.049E-02 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
7 1.04883E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
8 1.10119E+00 2.737E-02 8.211E-02 0.000E+00 0.000E+00 0.00E+00 -1.19E-06 0.00E+00
|
|
9 1.14296E+00 2.254E-02 0.000E+00 6.295E-02 4.665E-03 0.00E+00 0.00E+00 1.71E-02
|
|
10 1.14296E+00 2.254E-02 0.000E+00 4.665E-03 6.295E-02 0.00E+00 0.00E+00 -1.71E-02
|
|
11 1.16537E+00 2.847E-02 0.000E+00 5.364E-03 8.004E-02 0.00E+00 -1.33E-06 2.07E-02
|
|
12 1.16537E+00 2.847E-02 0.000E+00 8.004E-02 5.363E-03 3.07E-06 0.00E+00 -2.07E-02
|
|
13 1.20390E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
14 1.21151E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
15 1.22525E+00 1.399E-03 4.196E-03 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
16 1.22947E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.00E+00 0.00E+00 0.00E+00
|
|
17 1.24185E+00 4.249E-03 0.000E+00 6.362E-03 6.384E-03 -5.02E-06 5.03E-06 -6.37E-03
|
|
18 1.24185E+00 4.248E-03 0.000E+00 6.384E-03 6.362E-03 0.00E+00 0.00E+00 6.37E-03
|
|
19 1.24320E+00 4.987E-03 1.496E-02 0.000E+00 0.000E+00 1.69E-06 -2.71E-06 0.00E+00
|
|
Sum of osc. strength : 1.343377E+00
|
|
|
|
--- !ResultsGS
|
|
iteration_state: {dtset: 2, }
|
|
comment : Summary of ground state results
|
|
lattice_vectors:
|
|
- [ 12.0000000, 0.0000000, 0.0000000, ]
|
|
- [ 0.0000000, 10.0000000, 0.0000000, ]
|
|
- [ 0.0000000, 0.0000000, 10.0000000, ]
|
|
lattice_lengths: [ 12.00000, 10.00000, 10.00000, ]
|
|
lattice_angles: [ 90.000, 90.000, 90.000, ] # degrees, (23, 13, 12)
|
|
lattice_volume: 1.2000000E+03
|
|
convergence: {deltae: 0.000E+00, res2: 0.000E+00, residm: 9.431E-10, diffor: 0.000E+00, }
|
|
etotal : -2.46886422E+00
|
|
entropy : 0.00000000E+00
|
|
fermie : -8.41187493E-01
|
|
cartesian_stress_tensor: null
|
|
pressure_GPa: null
|
|
xred :
|
|
- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, He]
|
|
- [ 1.6667E-01, 0.0000E+00, 0.0000E+00, H]
|
|
cartesian_forces: null
|
|
force_length_stats: {min: null, max: null, mean: null, }
|
|
...
|
|
|
|
Integrated electronic density in atomic spheres:
|
|
------------------------------------------------
|
|
Atom Sphere_radius Integrated_density
|
|
1 2.00000 1.80406349
|
|
2 2.00000 0.93296351
|
|
================================================================================
|
|
|
|
----iterations are completed or convergence reached----
|
|
|
|
Mean square residual over all n,k,spin= 43.834E-11; max= 94.310E-11
|
|
reduced coordinates (array xred) for 2 atoms
|
|
0.000000000000 0.000000000000 0.000000000000
|
|
0.166666666667 0.000000000000 0.000000000000
|
|
|
|
cartesian coordinates (angstrom) at end:
|
|
1 0.00000000000000 0.00000000000000 0.00000000000000
|
|
2 1.05835441718000 0.00000000000000 0.00000000000000
|
|
length scales= 12.000000000000 10.000000000000 10.000000000000 bohr
|
|
= 6.350126503080 5.291772085900 5.291772085900 angstroms
|
|
prteigrs : about to open file t54o_DS2_EIG
|
|
Eigenvalues (hartree) for nkpt= 1 k points:
|
|
kpt# 1, nband= 20, wtk= 1.00000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
|
|
-0.84119 -0.23131 0.04090 0.07517 0.07517 0.17601 0.19930 0.20860
|
|
0.27392 0.30779 0.30779 0.33066 0.33066 0.36508 0.37052 0.38866
|
|
0.39109 0.40162 0.40162 0.41022
|
|
|
|
== END DATASET(S) ==============================================================
|
|
================================================================================
|
|
|
|
-outvars: echo values of variables after computation --------
|
|
acell 1.2000000000E+01 1.0000000000E+01 1.0000000000E+01 Bohr
|
|
amu 4.00260200E+00 1.00794000E+00
|
|
boxcenter 0.00000000E+00 0.00000000E+00 0.00000000E+00
|
|
cellcharge 1.00000000E+00
|
|
diecut1 2.20000000E+00 Hartree
|
|
diecut2 3.60000000E+01 Hartree
|
|
diemac 1.00000000E+00
|
|
diemix 5.00000000E-01
|
|
ecut 9.00000000E+00 Hartree
|
|
etotal1 -2.4688642225E+00
|
|
fcart1 3.7830754134E-02 -0.0000000000E+00 -0.0000000000E+00
|
|
-3.7830754134E-02 -0.0000000000E+00 -0.0000000000E+00
|
|
- fftalg 512
|
|
getden1 0
|
|
getden2 1
|
|
getwfk1 0
|
|
getwfk2 1
|
|
iscf1 7
|
|
iscf2 -1
|
|
istwfk 2
|
|
ixc 20
|
|
jdtset 1 2
|
|
kptnrm 4.00000000E+00
|
|
kptopt 0
|
|
P mkmem 1
|
|
natom 2
|
|
nband1 1
|
|
nband2 20
|
|
ndtset 2
|
|
ngfft 36 30 30
|
|
nkpt 1
|
|
nstep 25
|
|
nsym 8
|
|
ntypat 2
|
|
occ1 2.000000
|
|
occ2 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 0.000000 0.000000 0.000000
|
|
0.000000 0.000000
|
|
spgroup 99
|
|
strten1 5.3563297661E-04 4.8987647530E-04 4.8987647530E-04
|
|
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
symrel 1 0 0 0 1 0 0 0 1 1 0 0 0 1 0 0 0 -1
|
|
1 0 0 0 -1 0 0 0 -1 1 0 0 0 -1 0 0 0 1
|
|
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
|
|
tolwfr1 1.00000000E-22
|
|
tolwfr2 1.00000000E-09
|
|
typat 1 2
|
|
xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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1.0583544172E+00 0.0000000000E+00 0.0000000000E+00
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xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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2.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
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1.6666666667E-01 0.0000000000E+00 0.0000000000E+00
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znucl 2.00000 1.00000
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================================================================================
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- Timing analysis has been suppressed with timopt=0
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================================================================================
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Suggested references for the acknowledgment of ABINIT usage.
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The users of ABINIT have little formal obligations with respect to the ABINIT group
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(those specified in the GNU General Public License, http://www.gnu.org/copyleft/gpl.txt).
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However, it is common practice in the scientific literature,
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to acknowledge the efforts of people that have made the research possible.
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In this spirit, please find below suggested citations of work written by ABINIT developers,
|
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corresponding to implementations inside of ABINIT that you have used in the present run.
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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
|
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of the ABINIT implementation.
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For information on why they are suggested, see also https://docs.abinit.org/theory/acknowledgments.
|
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-
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|
- [1] The Abinit project: Impact, environment and recent developments.
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- Computer Phys. Comm. 248, 107042 (2020).
|
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- 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,
|
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- 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] 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
|
|
-
|
|
- [3] 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:
|
|
-
|
|
- [4] 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
|
|
-
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- Proc. 0 individual time (sec): cpu= 0.7 wall= 0.8
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================================================================================
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Calculation completed.
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.Delivered 17 WARNINGs and 13 COMMENTs to log file.
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+Overall time at end (sec) : cpu= 0.7 wall= 0.8
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