mirror of https://github.com/abinit/abinit.git
787 lines
39 KiB
Plaintext
787 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 19h11 )
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- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/v6_t61/t61.abi
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- output file -> t61.abo
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- root for input files -> t61i
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- root for output files -> t61o
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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 = 45 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 = 1
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- mband = 30 mffmem = 1 mkmem = 1
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mpw = 2401 nfft = 91125 nkpt = 1
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================================================================================
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P This job should need less than 26.870 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 1.101 Mbytes ; DEN or POT disk file : 0.697 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 = 45 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 = 1
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- mband = 30 mffmem = 1 mkmem = 1
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- mkqmem = 1 mk1mem = 1 mpw = 4801
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nfft = 91125 nkpt = 1
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================================================================================
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P This job should need less than 26.571 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 2.200 Mbytes ; DEN or POT disk file : 0.697 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 1.2000000000E+01 1.2000000000E+01 Bohr
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amu 1.00794000E+00
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bdeigrf1 -1
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bdeigrf2 10
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diemac 2.00000000E+00
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ecut 1.50000000E+01 Hartree
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- fftalg 512
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getwfk1 0
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getwfk2 1
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ieig2rf1 0
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ieig2rf2 2
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istwfk1 2
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istwfk2 1
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jdtset 1 2
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kptopt1 1
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kptopt2 3
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kptrlatt 1 0 0 0 1 0 0 0 1
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kptrlen 1.20000000E+04
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P mkmem 1
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P mkqmem 1
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P mk1mem 1
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natom 2
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nband 30
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ndtset 2
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ngfft 45 45 45
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nkpt 1
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nqpt1 0
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nqpt2 1
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nstep 40
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nsym 1
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ntypat 1
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occ 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 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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optdriver1 0
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optdriver2 1
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prtpot1 0
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prtpot2 1
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rfdir 1 0 0
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rfphon1 0
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rfphon2 1
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smdelta1 0
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smdelta2 1
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spgroup 1
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tolvrs1 1.00000000E-18
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tolvrs2 1.00000000E-08
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typat 1 1
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xangst -3.8298925516E-01 0.0000000000E+00 0.0000000000E+00
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3.8298925516E-01 0.0000000000E+00 0.0000000000E+00
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xcart -7.2374480409E-01 0.0000000000E+00 0.0000000000E+00
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7.2374480409E-01 0.0000000000E+00 0.0000000000E+00
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xred -6.0312067007E-02 0.0000000000E+00 0.0000000000E+00
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6.0312067007E-02 0.0000000000E+00 0.0000000000E+00
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znucl 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: 30, nsppol: 1, nspinor: 1, nspden: 1, mpw: 2401, }
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cutoff_energies: {ecut: 15.0, pawecutdg: -1.0, }
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electrons: {nelect: 2.00000000E+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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LDA: new Teter (4/93) with spin-polarized option - ixc=1
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Citation for XC functional:
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S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
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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 12.0000000 0.0000000 G(2)= 0.0000000 0.0833333 0.0000000
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R(3)= 0.0000000 0.0000000 12.0000000 G(3)= 0.0000000 0.0000000 0.0833333
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Unit cell volume ucvol= 1.7280000E+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= 45 45 45
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ecut(hartree)= 15.000 => boxcut(ratio)= 2.10310
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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/PseudosTM_pwteter/1h.pspnc
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- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/PseudosTM_pwteter/1h.pspnc
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- Troullier-Martins psp for element H Thu Oct 27 17:28:54 EDT 1994
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- 1.00000 1.00000 940714 znucl, zion, pspdat
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1 1 0 0 2001 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
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0 7.740 11.990 0 1.5855604 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= 1.0
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pspatm : epsatm= 0.04198703
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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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1.67948119E-01 ecore*ucvol(ha*bohr**3)
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--------------------------------------------------------------------------------
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_setup2: Arith. and geom. avg. npw (full set) are 4801.000 4801.000
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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: 40, nline: 4, wfoptalg: 0, }
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tolerances: {tolvrs: 1.00E-18, }
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...
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iter Etot(hartree) deltaE(h) residm vres2
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ETOT 1 -1.1336722134623 -1.134E+00 2.668E-03 1.986E+01
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ETOT 2 -1.1365673616272 -2.895E-03 7.063E-06 2.596E+00
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ETOT 3 -1.1365908558465 -2.349E-05 4.815E-05 2.433E-01
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ETOT 4 -1.1365930140497 -2.158E-06 6.298E-06 8.046E-03
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ETOT 5 -1.1365932781439 -2.641E-07 1.228E-05 2.303E-04
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ETOT 6 -1.1365933018071 -2.366E-08 1.707E-06 8.501E-06
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ETOT 7 -1.1365933027695 -9.624E-10 3.850E-06 2.819E-07
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ETOT 8 -1.1365933028324 -6.292E-11 5.892E-07 9.060E-09
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ETOT 9 -1.1365933028338 -1.347E-12 1.311E-06 1.656E-10
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ETOT 10 -1.1365933028336 1.248E-13 2.050E-07 3.159E-12
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ETOT 11 -1.1365933028337 -2.776E-14 4.474E-07 1.415E-13
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ETOT 12 -1.1365933028337 1.221E-14 7.025E-08 3.116E-15
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ETOT 13 -1.1365933028337 -1.821E-14 1.516E-07 9.331E-18
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ETOT 14 -1.1365933028336 2.398E-14 2.376E-08 1.873E-19
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At SCF step 14 vres2 = 1.87E-19 < tolvrs= 1.00E-18 =>converged.
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Cartesian components of stress tensor (hartree/bohr^3)
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sigma(1 1)= 1.93039993E-05 sigma(3 2)= 0.00000000E+00
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sigma(2 2)= 1.08869151E-06 sigma(3 1)= 0.00000000E+00
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sigma(3 3)= 1.08869151E-06 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, 12.0000000, 0.0000000, ]
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- [ 0.0000000, 0.0000000, 12.0000000, ]
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lattice_lengths: [ 12.00000, 12.00000, 12.00000, ]
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lattice_angles: [ 90.000, 90.000, 90.000, ] # degrees, (23, 13, 12)
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lattice_volume: 1.7280000E+03
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convergence: {deltae: 2.398E-14, res2: 1.873E-19, residm: 2.376E-08, diffor: null, }
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etotal : -1.13659330E+00
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entropy : 0.00000000E+00
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fermie : -3.68287456E-01
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cartesian_stress_tensor: # hartree/bohr^3
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- [ 1.93039993E-05, 0.00000000E+00, 0.00000000E+00, ]
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- [ 0.00000000E+00, 1.08869151E-06, 0.00000000E+00, ]
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- [ 0.00000000E+00, 0.00000000E+00, 1.08869151E-06, ]
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pressure_GPa: -2.1067E-01
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xred :
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- [ -6.0312E-02, 0.0000E+00, 0.0000E+00, H]
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- [ 6.0312E-02, 0.0000E+00, 0.0000E+00, H]
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cartesian_forces: # hartree/bohr
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- [ 2.17308842E-02, 1.90097302E-15, 2.32402378E-15, ]
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- [ -2.17308842E-02, -1.90097302E-15, -2.32402378E-15, ]
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force_length_stats: {min: 2.17308842E-02, max: 2.17308842E-02, mean: 2.17308842E-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 1.45819351
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2 2.00000 1.45819351
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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= 79.209E-11; max= 23.763E-09
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reduced coordinates (array xred) for 2 atoms
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-0.060312067007 0.000000000000 0.000000000000
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0.060312067007 0.000000000000 0.000000000000
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rms dE/dt= 1.5056E-01; max dE/dt= 2.6077E-01; dE/dt below (all hartree)
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1 -0.260770610164 0.000000000001 0.000000000001
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2 0.260770610166 0.000000000001 0.000000000001
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cartesian coordinates (angstrom) at end:
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1 -0.38298925515986 0.00000000000000 0.00000000000000
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2 0.38298925515986 0.00000000000000 0.00000000000000
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cartesian forces (hartree/bohr) at end:
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1 0.02173088418040 0.00000000000000 0.00000000000000
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2 -0.02173088418040 -0.00000000000000 -0.00000000000000
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frms,max,avg= 1.2546332E-02 2.1730884E-02 -8.307E-14 -5.332E-14 -6.904E-14 h/b
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cartesian forces (eV/Angstrom) at end:
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1 1.11744689954758 0.00000000000010 0.00000000000012
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2 -1.11744689954758 -0.00000000000010 -0.00000000000012
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frms,max,avg= 6.4515827E-01 1.1174469E+00 -4.272E-12 -2.742E-12 -3.550E-12 e/A
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length scales= 12.000000000000 12.000000000000 12.000000000000 bohr
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= 6.350126503080 6.350126503080 6.350126503080 angstroms
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prteigrs : about to open file t61o_DS1_EIG
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Fermi (or HOMO) energy (hartree) = -0.36829 Average Vxc (hartree)= -0.04697
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Eigenvalues (hartree) for nkpt= 1 k points:
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kpt# 1, nband= 30, wtk= 1.00000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
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-0.36829 -0.01222 0.03792 0.07966 0.07966 0.10636 0.11027 0.15116
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0.17349 0.20714 0.20714 0.22986 0.22986 0.23414 0.24517 0.24802
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0.24802 0.24870 0.24894 0.32308 0.33978 0.36619 0.36619 0.37147
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0.37147 0.37479 0.37518 0.43668 0.44527 0.48427
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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 : 1.02169260525684E+00
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hartree : 8.16963420139678E-01
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xc : -6.41538426465240E-01
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Ewald energy : 2.20562814674697E-01
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psp_core : 9.71921987298343E-05
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local_psp : -2.55437090863835E+00
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non_local_psp : 0.00000000000000E+00
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total_energy : -1.13659330283365E+00
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total_energy_eV : -3.09282766561116E+01
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band_energy : -7.36574911837632E-01
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...
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Cartesian components of stress tensor (hartree/bohr^3)
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sigma(1 1)= 1.93039993E-05 sigma(3 2)= 0.00000000E+00
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sigma(2 2)= 1.08869151E-06 sigma(3 1)= 0.00000000E+00
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sigma(3 3)= 1.08869151E-06 sigma(2 1)= 0.00000000E+00
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-Cartesian components of stress tensor (GPa) [Pressure= -2.1067E-01 GPa]
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- sigma(1 1)= 5.67943173E-01 sigma(3 2)= 0.00000000E+00
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- sigma(2 2)= 3.20304047E-02 sigma(3 1)= 0.00000000E+00
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- sigma(3 3)= 3.20304045E-02 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: 30, nsppol: 1, nspinor: 1, nspden: 1, mpw: 4801, }
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cutoff_energies: {ecut: 15.0, pawecutdg: -1.0, }
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electrons: {nelect: 2.00000000E+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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LDA: new Teter (4/93) with spin-polarized option - ixc=1
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Citation for XC functional:
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S. Goedecker, M. Teter, J. Huetter, PRB 54, 1703 (1996)
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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 12.0000000 0.0000000 G(2)= 0.0000000 0.0833333 0.0000000
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R(3)= 0.0000000 0.0000000 12.0000000 G(3)= 0.0000000 0.0000000 0.0833333
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Unit cell volume ucvol= 1.7280000E+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= 45 45 45
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ecut(hartree)= 15.000 => boxcut(ratio)= 2.10310
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--------------------------------------------------------------------------------
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==> initialize data related to q vector <==
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The list of irreducible perturbations for this q vector is:
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1) idir= 1 ipert= 1
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2) idir= 1 ipert= 2
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================================================================================
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--------------------------------------------------------------------------------
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Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
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Perturbation : displacement of atom 1 along direction 1
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The set of symmetries contains only one element for this perturbation.
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symkpt : not enough symmetry to change the number of k points.
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--------------------------------------------------------------------------------
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--------------------------------------------------------------------------------
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Initialisation of the first-order wave-functions :
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ireadwf= 0
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--- !BeginCycle
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iteration_state: {dtset: 2, }
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solver: {iscf: 7, nstep: 40, nline: 4, wfoptalg: 0, }
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tolerances: {tolvrs: 1.00E-08, }
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...
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iter 2DEtotal(Ha) deltaE(Ha) residm vres2
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-ETOT 1 52.572168585249 -1.158E+02 7.987E-01 2.927E+04
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ETOT 2 37.240807182985 -1.533E+01 5.849E-03 2.801E+03
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ETOT 3 36.232438010883 -1.008E+00 1.493E-03 1.046E+02
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ETOT 4 36.231770529877 -6.675E-04 3.407E-05 4.206E+00
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ETOT 5 36.229786281786 -1.984E-03 9.652E-05 4.952E-01
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ETOT 6 36.229705843769 -8.044E-05 8.992E-06 4.422E-03
|
|
ETOT 7 36.229705782373 -6.140E-08 3.499E-05 5.259E-05
|
|
ETOT 8 36.229705776533 -5.840E-09 1.807E-06 4.841E-06
|
|
ETOT 9 36.229705776339 -1.943E-10 7.342E-06 2.473E-08
|
|
ETOT 10 36.229705776334 -4.547E-12 4.196E-07 1.675E-09
|
|
|
|
At SCF step 10 vres2 = 1.67E-09 < tolvrs= 1.00E-08 =>converged.
|
|
================================================================================
|
|
|
|
----iterations are completed or convergence reached----
|
|
|
|
Mean square residual over all n,k,spin= 13.988E-09; max= 41.964E-08
|
|
|
|
Thirteen components of 2nd-order total energy (hartree) are
|
|
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
|
|
kin0= 1.03702275E+02 eigvalue= 1.35503763E+01 local= -3.66855873E+01
|
|
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
|
|
loc psp = -2.64190124E+02 Hartree= 4.60844818E+01 xc= -2.18978392E+01
|
|
note that "loc psp" includes a xc core correction that could be resolved
|
|
7,8,9: eventually, occupation + non-local contributions
|
|
edocc= 2.73413552E+01 enl0= 0.00000000E+00 enl1= 0.00000000E+00
|
|
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
|
|
erelax= -1.32095062E+02
|
|
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
|
|
fr.local= 7.29689411E+01 fr.nonlo= 0.00000000E+00 Ewald= 9.53558265E+01
|
|
13,14 Frozen wf xc core corrections (1) and (2)
|
|
frxc 1 = 0.00000000E+00 frxc 2 = 0.00000000E+00
|
|
Resulting in :
|
|
2DEtotal= 0.3622970578E+02 Ha. Also 2DEtotal= 0.985860431015E+03 eV
|
|
(2DErelax= -1.3209506184E+02 Ha. 2DEnonrelax= 1.6832476761E+02 Ha)
|
|
( non-var. 2DEtotal : 3.6229705785E+01 Ha)
|
|
|
|
|
|
--------------------------------------------------------------------------------
|
|
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
|
|
Perturbation : displacement of atom 2 along direction 1
|
|
The set of symmetries contains only one element for this perturbation.
|
|
symkpt : not enough symmetry to change the number of k points.
|
|
|
|
--------------------------------------------------------------------------------
|
|
|
|
--------------------------------------------------------------------------------
|
|
|
|
Initialisation of the first-order wave-functions :
|
|
ireadwf= 0
|
|
|
|
--- !BeginCycle
|
|
iteration_state: {dtset: 2, }
|
|
solver: {iscf: 7, nstep: 40, nline: 4, wfoptalg: 0, }
|
|
tolerances: {tolvrs: 1.00E-08, }
|
|
...
|
|
|
|
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
|
|
-ETOT 1 52.572167359002 -1.158E+02 7.987E-01 2.927E+04
|
|
ETOT 2 37.240804334617 -1.533E+01 5.849E-03 2.801E+03
|
|
ETOT 3 36.232434972196 -1.008E+00 1.493E-03 1.046E+02
|
|
ETOT 4 36.231767491471 -6.675E-04 3.518E-05 4.206E+00
|
|
ETOT 5 36.229783243514 -1.984E-03 9.857E-05 4.952E-01
|
|
ETOT 6 36.229702805473 -8.044E-05 9.848E-06 4.422E-03
|
|
ETOT 7 36.229702744079 -6.139E-08 3.662E-05 5.259E-05
|
|
ETOT 8 36.229702738243 -5.836E-09 2.038E-06 4.841E-06
|
|
ETOT 9 36.229702738045 -1.984E-10 7.901E-06 2.473E-08
|
|
ETOT 10 36.229702738048 3.268E-12 4.901E-07 1.675E-09
|
|
|
|
At SCF step 10 vres2 = 1.67E-09 < tolvrs= 1.00E-08 =>converged.
|
|
================================================================================
|
|
|
|
----iterations are completed or convergence reached----
|
|
|
|
Mean square residual over all n,k,spin= 16.337E-09; max= 49.011E-08
|
|
|
|
Thirteen components of 2nd-order total energy (hartree) are
|
|
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
|
|
kin0= 1.03702237E+02 eigvalue= 1.35503657E+01 local= -3.66855664E+01
|
|
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
|
|
loc psp = -2.64190130E+02 Hartree= 4.60844844E+01 xc= -2.18978405E+01
|
|
note that "loc psp" includes a xc core correction that could be resolved
|
|
7,8,9: eventually, occupation + non-local contributions
|
|
edocc= 2.73413843E+01 enl0= 0.00000000E+00 enl1= 0.00000000E+00
|
|
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
|
|
erelax= -1.32095065E+02
|
|
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
|
|
fr.local= 7.29689411E+01 fr.nonlo= 0.00000000E+00 Ewald= 9.53558265E+01
|
|
13,14 Frozen wf xc core corrections (1) and (2)
|
|
frxc 1 = 0.00000000E+00 frxc 2 = 0.00000000E+00
|
|
Resulting in :
|
|
2DEtotal= 0.3622970274E+02 Ha. Also 2DEtotal= 0.985860348339E+03 eV
|
|
(2DErelax= -1.3209506487E+02 Ha. 2DEnonrelax= 1.6832476761E+02 Ha)
|
|
( non-var. 2DEtotal : 3.6229702747E+01 Ha)
|
|
|
|
Components of second-order derivatives of the electronic energy, EIGR2D, in Ha unit.
|
|
For automatic tests, printing the matrix for the first k-point, first band, first atom.
|
|
1 1 1 1 -6.8353388065E+00 0.0000000000E+00
|
|
1 1 2 1 0.0000000000E+00 0.0000000000E+00
|
|
1 1 3 1 0.0000000000E+00 0.0000000000E+00
|
|
2 1 1 1 0.0000000000E+00 0.0000000000E+00
|
|
2 1 2 1 0.0000000000E+00 0.0000000000E+00
|
|
2 1 3 1 0.0000000000E+00 0.0000000000E+00
|
|
3 1 1 1 0.0000000000E+00 0.0000000000E+00
|
|
3 1 2 1 0.0000000000E+00 0.0000000000E+00
|
|
3 1 3 1 0.0000000000E+00 0.0000000000E+00
|
|
|
|
Components of second-order derivatives of the electronic energy, EIGI2D.
|
|
For automatic tests, printing the matrix for the first k-point, first band, first atom.
|
|
1 1 1 1 3.2231731991E+01 0.0000000000E+00
|
|
1 1 2 1 0.0000000000E+00 0.0000000000E+00
|
|
1 1 3 1 0.0000000000E+00 0.0000000000E+00
|
|
2 1 1 1 0.0000000000E+00 0.0000000000E+00
|
|
2 1 2 1 0.0000000000E+00 0.0000000000E+00
|
|
2 1 3 1 0.0000000000E+00 0.0000000000E+00
|
|
3 1 1 1 0.0000000000E+00 0.0000000000E+00
|
|
3 1 2 1 0.0000000000E+00 0.0000000000E+00
|
|
3 1 3 1 0.0000000000E+00 0.0000000000E+00
|
|
================================================================================
|
|
|
|
---- first-order wavefunction calculations are completed ----
|
|
|
|
|
|
==> Compute Derivative Database <==
|
|
|
|
2nd-order matrix (non-cartesian coordinates, masses not included,
|
|
asr not included )
|
|
j1 j2 matrix element
|
|
dir pert dir pert real part imaginary part
|
|
|
|
1 1 1 1 36.2297057855 0.0000000000
|
|
1 1 2 1 0.0002924100 0.0000000000
|
|
1 1 3 1 -0.0001169331 0.0000000000
|
|
1 1 1 2 -36.2297064422 -0.0000000000
|
|
1 1 2 2 0.0002923917 -0.0000000000
|
|
1 1 3 2 -0.0001156081 -0.0000000000
|
|
|
|
2 1 1 1 0.0002924100 0.0000000000
|
|
2 1 1 2 -0.0004133065 -0.0000000000
|
|
|
|
3 1 1 1 -0.0001169331 0.0000000000
|
|
3 1 1 2 0.0001651081 -0.0000000000
|
|
|
|
1 2 1 1 -36.2297064423 0.0000000000
|
|
1 2 2 1 -0.0004133065 0.0000000000
|
|
1 2 3 1 0.0001651081 0.0000000000
|
|
1 2 1 2 36.2297027472 0.0000000000
|
|
1 2 2 2 -0.0004132868 0.0000000000
|
|
1 2 3 2 0.0001637443 0.0000000000
|
|
|
|
2 2 1 1 0.0002923917 0.0000000000
|
|
2 2 1 2 -0.0004132868 0.0000000000
|
|
|
|
3 2 1 1 -0.0001156081 0.0000000000
|
|
3 2 1 2 0.0001637443 0.0000000000
|
|
|
|
|
|
Dynamical matrix, in cartesian coordinates,
|
|
if specified in the inputs, asr has been imposed
|
|
j1 j2 matrix element
|
|
dir pert dir pert real part imaginary part
|
|
|
|
1 1 1 1 0.2515951836 0.0000000000
|
|
1 1 2 1 -0.0000020305 0.0000000000
|
|
1 1 3 1 0.0000008028 0.0000000000
|
|
1 1 1 2 -0.2515951836 -0.0000000000
|
|
1 1 2 2 0.0000020305 -0.0000000000
|
|
1 1 3 2 -0.0000008028 -0.0000000000
|
|
|
|
2 1 1 1 0.0000028702 0.0000000000
|
|
2 1 1 2 -0.0000028702 -0.0000000000
|
|
|
|
3 1 1 1 -0.0000011466 0.0000000000
|
|
3 1 1 2 0.0000011466 -0.0000000000
|
|
|
|
1 2 1 1 -0.2515951836 0.0000000000
|
|
1 2 2 1 -0.0000028702 0.0000000000
|
|
1 2 3 1 0.0000011466 0.0000000000
|
|
1 2 1 2 0.2515951836 -0.0000000000
|
|
1 2 2 2 0.0000028702 -0.0000000000
|
|
1 2 3 2 -0.0000011466 -0.0000000000
|
|
|
|
2 2 1 1 0.0000020305 0.0000000000
|
|
2 2 1 2 -0.0000020305 -0.0000000000
|
|
|
|
3 2 1 1 -0.0000008028 0.0000000000
|
|
3 2 1 2 0.0000008028 -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
|
|
1.654889E-02
|
|
Phonon frequencies in cm-1 :
|
|
- 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00
|
|
- 3.632061E+03
|
|
chkph3 : WARNING -
|
|
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
|
|
================================================================================
|
|
|
|
---- T=0 shift of eigenenergies due to electron-phonon interation at q ----
|
|
Warning : the total shift must be computed through anaddb,
|
|
here, only the contribution of one q point is printed.
|
|
Print first the electronic eigenvalues, then the q-dependent Fan shift of eigenvalues.
|
|
Phonons at gamma, also compute the Diagonal Debye-Waller shift of eigenvalues.
|
|
|
|
Eigenvalues (hartree) for nkpt= 1 k points:
|
|
kpt# 1, nband= 30, wtk= 1.00000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
|
|
-0.36829 -0.01222 0.03792 0.07966 0.07966 0.10636 0.11027 0.15116
|
|
0.17349 0.20714 0.20714 0.22986 0.22986 0.23414 0.24517 0.24802
|
|
0.24802 0.24870 0.24894 0.32308 0.33978 0.36619 0.36619 0.37147
|
|
0.37147 0.37479 0.37518 0.43668 0.44527 0.48427
|
|
|
|
|
|
Fan corrections to eigenvalues at T=0 (hartree) for nkpt= 1 k points:
|
|
(in case of degenerate eigenvalues, averaged derivative)
|
|
kpt# 1, nband= 30, wtk= 1.00000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
|
|
-0.00068 0.00009 -0.00120 -0.00001 -0.00001 -0.00000 -0.00000 0.00011
|
|
0.00038 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
|
|
|
|
DDW corrections to eigenvalues at T=0 (hartree) for nkpt= 1 k points:
|
|
(in case of degenerate eigenvalues, averaged derivative)
|
|
kpt# 1, nband= 30, wtk= 1.00000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
|
|
0.00088 0.00003 -0.00038 0.00002 0.00002 -0.00005 0.00000 0.00005
|
|
-0.00021 0.00001 0.00001 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
|
|
|
|
Fan+DDW corrs to eigenvalues at T=0 (hartree) for nkpt= 1 k points:
|
|
(in case of degenerate eigenvalues, averaged derivative)
|
|
kpt# 1, nband= 30, wtk= 1.00000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
|
|
0.00020 0.00012 -0.00159 0.00001 0.00001 -0.00005 0.00000 0.00015
|
|
0.00017 0.00002 0.00002 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
0.00000 0.00000 0.00000 0.00000 0.00000 0.00000
|
|
|
|
== END DATASET(S) ==============================================================
|
|
================================================================================
|
|
|
|
-outvars: echo values of variables after computation --------
|
|
acell 1.2000000000E+01 1.2000000000E+01 1.2000000000E+01 Bohr
|
|
amu 1.00794000E+00
|
|
bdeigrf1 -1
|
|
bdeigrf2 10
|
|
diemac 2.00000000E+00
|
|
ecut 1.50000000E+01 Hartree
|
|
etotal1 -1.1365933028E+00
|
|
etotal2 3.6229702738E+01
|
|
fcart1 2.1730884180E-02 1.9009730216E-15 2.3240237841E-15
|
|
-2.1730884180E-02 -1.9009730216E-15 -2.3240237841E-15
|
|
fcart2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
- fftalg 512
|
|
getwfk1 0
|
|
getwfk2 1
|
|
ieig2rf1 0
|
|
ieig2rf2 2
|
|
istwfk1 2
|
|
istwfk2 1
|
|
jdtset 1 2
|
|
kptopt1 1
|
|
kptopt2 3
|
|
kptrlatt 1 0 0 0 1 0 0 0 1
|
|
kptrlen 1.20000000E+04
|
|
P mkmem 1
|
|
P mkqmem 1
|
|
P mk1mem 1
|
|
natom 2
|
|
nband 30
|
|
ndtset 2
|
|
ngfft 45 45 45
|
|
nkpt 1
|
|
nqpt1 0
|
|
nqpt2 1
|
|
nstep 40
|
|
nsym 1
|
|
ntypat 1
|
|
occ 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 0.000000 0.000000 0.000000 0.000000
|
|
0.000000 0.000000 0.000000 0.000000 0.000000 0.000000
|
|
optdriver1 0
|
|
optdriver2 1
|
|
prtpot1 0
|
|
prtpot2 1
|
|
rfdir 1 0 0
|
|
rfphon1 0
|
|
rfphon2 1
|
|
smdelta1 0
|
|
smdelta2 1
|
|
spgroup 1
|
|
strten1 1.9303999329E-05 1.0886915096E-06 1.0886915052E-06
|
|
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
strten2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
tolvrs1 1.00000000E-18
|
|
tolvrs2 1.00000000E-08
|
|
typat 1 1
|
|
xangst -3.8298925516E-01 0.0000000000E+00 0.0000000000E+00
|
|
3.8298925516E-01 0.0000000000E+00 0.0000000000E+00
|
|
xcart -7.2374480409E-01 0.0000000000E+00 0.0000000000E+00
|
|
7.2374480409E-01 0.0000000000E+00 0.0000000000E+00
|
|
xred -6.0312067007E-02 0.0000000000E+00 0.0000000000E+00
|
|
6.0312067007E-02 0.0000000000E+00 0.0000000000E+00
|
|
znucl 1.00000
|
|
|
|
================================================================================
|
|
|
|
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] Verification of first-principles codes: Comparison of total energies, phonon frequencies,
|
|
- electron--phonon coupling and zero-point motion correction to the gap between ABINIT and QE/Yambo
|
|
- S. Ponce, G. Antonius, P. Boulanger, E. Cannuccia, A. Marini, M. Cote and X. Gonze. Computational Material Science 83, 341 (2014)
|
|
- Comment: the temperature-dependence of the electronic structure is computed (or the zero-point renormalisation).
|
|
- Strong suggestion to cite this paper in your publications.
|
|
- DOI and bibtex : see https://docs.abinit.org/theory/bibliography/#ponce2014
|
|
-
|
|
- [2] Temperature dependence of the electronic structure of semiconductors and insulators
|
|
- S. Ponce, Y. Gillet, J. Laflamme Janssen, A. Marini, M. Verstraete and X. Gonze. J. Chem. Phys. 143, 102813 (2015)
|
|
- Comment: the temperature-dependence of the electronic structure is computed (or the zero-point renormalisation).
|
|
- Strong suggestion to cite this paper in your publications.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#ponce2015
|
|
-
|
|
- [3] The Abinit project: Impact, environment and recent developments.
|
|
- Computer Phys. Comm. 248, 107042 (2020).
|
|
- X.Gonze, B. Amadon, G. Antonius, F.Arnardi, L.Baguet, J.-M.Beuken,
|
|
- J.Bieder, F.Bottin, J.Bouchet, E.Bousquet, N.Brouwer, F.Bruneval,
|
|
- G.Brunin, T.Cavignac, J.-B. Charraud, Wei Chen, M.Cote, S.Cottenier,
|
|
- J.Denier, G.Geneste, Ph.Ghosez, M.Giantomassi, Y.Gillet, O.Gingras,
|
|
- D.R.Hamann, G.Hautier, Xu He, N.Helbig, N.Holzwarth, Y.Jia, F.Jollet,
|
|
- W.Lafargue-Dit-Hauret, K.Lejaeghere, M.A.L.Marques, A.Martin, C.Martins,
|
|
- H.P.C. Miranda, F.Naccarato, K. Persson, G.Petretto, V.Planes, Y.Pouillon,
|
|
- S.Prokhorenko, F.Ricci, G.-M.Rignanese, A.H.Romero, M.M.Schmitt, M.Torrent,
|
|
- M.J.van Setten, B.Van Troeye, M.J.Verstraete, G.Zerah and J.W.Zwanzig
|
|
- Comment: the fifth generic paper describing the ABINIT project.
|
|
- Note that a version of this paper, that is not formatted for Computer Phys. Comm.
|
|
- is available at https://www.abinit.org/sites/default/files/ABINIT20.pdf .
|
|
- The licence allows the authors to put it on the Web.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze2020
|
|
-
|
|
- [4] First-principles responses of solids to atomic displacements and homogeneous electric fields:,
|
|
- implementation of a conjugate-gradient algorithm. X. Gonze, Phys. Rev. B55, 10337 (1997).
|
|
- Comment: Non-vanishing rfphon and/or rfelfd, in the norm-conserving case.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze1997
|
|
-
|
|
- [5] Dynamical matrices, Born effective charges, dielectric permittivity tensors, and ,
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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.
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- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze1997a
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-
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- [6] ABINIT: Overview, and focus on selected capabilities
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- 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,
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- D.R.Hamann, G.Hautier, F.Jollet, G. Jomard,
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- A.Martin,
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- H.P.C. Miranda, F.Naccarato, G.Petretto, N.A. Pike, V.Planes,
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- S.Prokhorenko, T. Rangel, F.Ricci, G.-M.Rignanese, M.Royo, M.Stengel, M.Torrent,
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- M.J.van Setten, B.Van Troeye, M.J.Verstraete, J.Wiktor, J.W.Zwanziger, and X.Gonze.
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- 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 .
|
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- The licence allows the authors to put it on the Web.
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- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#romero2020
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|
-
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- [7] 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= 7.1 wall= 7.1
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================================================================================
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Calculation completed.
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.Delivered 1 WARNINGs and 13 COMMENTs to log file.
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+Overall time at end (sec) : cpu= 7.1 wall= 7.1
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