mirror of https://github.com/abinit/abinit.git
514 lines
27 KiB
Plaintext
514 lines
27 KiB
Plaintext
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.Version 10.1.4.5 of ABINIT, released Sep 2024.
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.(MPI version, prepared for a x86_64_linux_gnu13.2 computer)
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.Copyright (C) 1998-2025 ABINIT group .
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ABINIT comes with ABSOLUTELY NO WARRANTY.
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It is free software, and you are welcome to redistribute it
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under certain conditions (GNU General Public License,
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see ~abinit/COPYING or http://www.gnu.org/copyleft/gpl.txt).
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ABINIT is a project of the Universite Catholique de Louvain,
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Corning Inc. and other collaborators, see ~abinit/doc/developers/contributors.txt .
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Please read https://docs.abinit.org/theory/acknowledgments for suggested
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acknowledgments of the ABINIT effort.
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For more information, see https://www.abinit.org .
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.Starting date : Fri 13 Sep 2024.
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- ( at 19h10 )
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- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/v4_t94/t94.abi
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- output file -> t94.abo
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- root for input files -> t94i
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- root for output files -> t94o
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Symmetries : 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 of the present run
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intxc = 0 ionmov = 0 iscf = 17 lmnmax = 13
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lnmax = 5 mgfft = 10 mpssoang = 3 mqgrid = 3001
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natom = 1 nloc_mem = 2 nspden = 1 nspinor = 1
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nsppol = 1 nsym = 1 n1xccc = 1 ntypat = 1
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occopt = 7 xclevel = 1
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- mband = 6 mffmem = 1 mkmem = 2
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mpw = 28 nfft = 640 nkpt = 2
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PAW method is used; the additional fine FFT grid is defined by:
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mgfftf= 20 nfftf = 5760
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================================================================================
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P This job should need less than 3.167 Mbytes of memory.
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Rough estimation (10% accuracy) of disk space for files :
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_ WF disk file : 0.007 Mbytes ; DEN or POT disk file : 0.046 Mbytes.
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================================================================================
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--------------------------------------------------------------------------------
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------------- Echo of variables that govern the present computation ------------
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--------------------------------------------------------------------------------
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-
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- outvars: echo of selected default values
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- iomode0 = 0 , fftalg0 =512 , wfoptalg0 = 10
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-
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- outvars: echo of global parameters not present in the input file
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- max_nthreads = 0
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-
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-outvars: echo values of preprocessed input variables --------
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acell 3.0000000000E+00 3.5000000000E+00 4.0000000000E+00 Bohr
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amu 4.00780000E+01
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densfor_pred 0
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ecut 3.00000000E+00 Hartree
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enunit 2
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- fftalg 400
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istwfk 2 0
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ixc 7
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kpt 0.00000000E+00 0.00000000E+00 0.00000000E+00
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3.00000000E-01 3.00000000E-01 3.00000000E-01
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kptopt 0
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P mkmem 2
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natom 1
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nband 6
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nbdblock 2
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ngfft 8 8 10
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ngfftdg 16 18 20
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nkpt 2
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nline 10
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nblock_lobpcg 6
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nnsclo 1
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nstep 25
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nsym 1
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ntime 5
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ntypat 1
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occ 2.000000 2.000000 2.000000 2.000000 2.000000 0.000000
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2.000000 2.000000 2.000000 2.000000 2.000000 0.000000
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occopt 7
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ortalg 1
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pawecutdg 1.50000000E+01 Hartree
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pawmixdg 1
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prtwf 0
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rprim 1.4000000000E+00 0.0000000000E+00 0.0000000000E+00
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0.0000000000E+00 1.4000000000E+00 0.0000000000E+00
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0.0000000000E+00 0.0000000000E+00 1.4000000000E+00
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spgroup 1
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toldfe 1.00000000E-08 Hartree
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tsmear 2.00000000E-02 Hartree
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typat 1
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useylm 1
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wfoptalg 4
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wtk 0.50000 0.50000
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znucl 20.00000
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================================================================================
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chkinp: Checking input parameters for consistency.
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================================================================================
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== DATASET 1 ==================================================================
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- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
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--- !DatasetInfo
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iteration_state: {dtset: 1, }
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dimensions: {natom: 1, nkpt: 2, mband: 6, nsppol: 1, nspinor: 1, nspden: 1, mpw: 28, }
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cutoff_energies: {ecut: 3.0, pawecutdg: 15.0, }
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electrons: {nelect: 1.00000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 2.00000000E-02, }
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meta: {optdriver: 0, ionmov: 0, optcell: 0, iscf: 17, paral_kgb: 0, }
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...
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Exchange-correlation functional for the present dataset will be:
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LDA: Perdew-Wang 92 LSD fit to Ceperley-Alder data - ixc=7
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Citation for XC functional:
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J.P.Perdew and Y.Wang, PRB 45, 13244 (1992)
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Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
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R(1)= 4.2000000 0.0000000 0.0000000 G(1)= 0.2380952 0.0000000 0.0000000
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R(2)= 0.0000000 4.9000000 0.0000000 G(2)= 0.0000000 0.2040816 0.0000000
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R(3)= 0.0000000 0.0000000 5.6000000 G(3)= 0.0000000 0.0000000 0.1785714
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Unit cell volume ucvol= 1.1524800E+02 bohr^3
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Angles (23,13,12)= 9.00000000E+01 9.00000000E+01 9.00000000E+01 degrees
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Coarse grid specifications (used for wave-functions):
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getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 8 8 10
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ecut(hartree)= 3.000 => boxcut(ratio)= 2.09396
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Fine grid specifications (used for densities):
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getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 18 20
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ecut(hartree)= 15.000 => boxcut(ratio)= 2.04848
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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/20ca.paw
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- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/20ca.paw
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- Paw atomic data for element Ca - Generated by AtomPAW (N. Holzwarth)
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- 20.00000 10.00000 20040423 znucl, zion, pspdat
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7 7 2 0 350 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
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Pseudopotential format is: paw2
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basis_size (lnmax)= 5 (lmn_size= 13), orbitals= 0 0 1 1 2
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Spheres core radius: rc_sph= 1.91000000
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2 radial meshes are used:
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- mesh 1: r(i)=AA*exp(BB*(i-2)), size= 350 , AA= 0.98023E-05 BB= 0.35000E-01
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- mesh 2: r(i)=step*(i-1), size= 766 , step= 0.25000E-02
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Shapefunction is SIN type: shapef(r)=[sin(pi*r/rshp)/(pi*r/rshp)]**2
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Radius for shape functions = sphere core radius
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Radial grid used for partial waves is grid 1
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Radial grid used for projectors is grid 2
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Radial grid used for (t)core density is grid 1
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Radial grid used for Vloc is grid 1
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Compensation charge density is taken into account in XC energy/potential
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pspatm: atomic psp has been read and splines computed
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2.49056342E+02 ecore*ucvol(ha*bohr**3)
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--------------------------------------------------------------------------------
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_setup2: Arith. and geom. avg. npw (full set) are 28.500 28.496
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================================================================================
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--- !BeginCycle
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iteration_state: {dtset: 1, }
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solver: {iscf: 17, nstep: 25, nline: 10, wfoptalg: 4, }
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tolerances: {toldfe: 1.00E-08, }
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...
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iter Etot(hartree) deltaE(h) residm nres2
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ETOT 1 -33.277612404323 -3.328E+01 2.950E-04 6.032E+00
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ETOT 2 -33.272392409270 5.220E-03 6.709E-07 1.031E+00
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ETOT 3 -33.254673977625 1.772E-02 3.978E-05 4.878E-02
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ETOT 4 -33.254304699135 3.693E-04 7.005E-09 1.490E-02
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ETOT 5 -33.254164024586 1.407E-04 3.273E-09 1.327E-03
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ETOT 6 -33.254151371823 1.265E-05 4.130E-11 2.156E-05
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ETOT 7 -33.254151305506 6.632E-08 3.372E-13 2.874E-06
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ETOT 8 -33.254151300149 5.357E-09 4.300E-15 4.214E-08
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ETOT 9 -33.254151300731 -5.819E-10 3.308E-16 5.202E-09
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At SCF step 9, etot is converged :
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for the second time, diff in etot= 5.819E-10 < toldfe= 1.000E-08
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Cartesian components of stress tensor (hartree/bohr^3)
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sigma(1 1)= 2.69450250E-02 sigma(3 2)= -6.15460434E-04
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sigma(2 2)= 3.30137604E-02 sigma(3 1)= 2.80919398E-04
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sigma(3 3)= 3.62581461E-02 sigma(2 1)= 9.84965337E-04
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--- !ResultsGS
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iteration_state: {dtset: 1, }
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comment : Summary of ground state results
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lattice_vectors:
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- [ 4.2000000, 0.0000000, 0.0000000, ]
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- [ 0.0000000, 4.9000000, 0.0000000, ]
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- [ 0.0000000, 0.0000000, 5.6000000, ]
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lattice_lengths: [ 4.20000, 4.90000, 5.60000, ]
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lattice_angles: [ 90.000, 90.000, 90.000, ] # degrees, (23, 13, 12)
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lattice_volume: 1.1524800E+02
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convergence: {deltae: -5.819E-10, res2: 5.202E-09, residm: 3.308E-16, diffor: null, }
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etotal : -3.32541513E+01
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entropy : 0.00000000E+00
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fermie : 4.11572518E-01
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cartesian_stress_tensor: # hartree/bohr^3
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- [ 2.69450250E-02, 9.84965337E-04, 2.80919398E-04, ]
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- [ 9.84965337E-04, 3.30137604E-02, -6.15460434E-04, ]
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- [ 2.80919398E-04, -6.15460434E-04, 3.62581461E-02, ]
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pressure_GPa: -9.4360E+02
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xred :
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- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Ca]
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cartesian_forces: # hartree/bohr
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- [ 0.00000000E+00, 0.00000000E+00, 0.00000000E+00, ]
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force_length_stats: {min: 0.00000000E+00, max: 0.00000000E+00, mean: 0.00000000E+00, }
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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 1.91000 6.53706986
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PAW TEST:
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==== Compensation charge inside spheres ============
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The following values must be close to each other ...
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Compensation charge over spherical meshes = -0.490044234234298
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Compensation charge over fine fft grid = -0.490076675971514
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==== Results concerning PAW augmentation regions ====
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Total pseudopotential strength Dij (hartree):
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0.75450 -0.02910 -0.00000 -0.00000 -0.00000 0.00000 0.00000 0.00000 0.00002 0.00001 0.00043 0.00002 ...
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-0.02910 0.02908 0.00000 0.00000 0.00000 0.00000 -0.00000 0.00000 -0.00000 0.00001 0.00003 0.00000 ...
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-0.00000 0.00000 -0.73512 0.00004 -0.00001 -0.00194 -0.00003 0.00004 0.00000 0.00000 -0.00000 0.00000 ...
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-0.00000 0.00000 0.00004 -0.73444 0.00002 -0.00003 -0.00095 0.00003 0.00000 0.00000 0.00000 0.00000 ...
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-0.00000 0.00000 -0.00001 0.00002 -0.73462 0.00004 0.00003 -0.00162 0.00000 0.00000 -0.00000 0.00000 ...
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0.00000 0.00000 -0.00194 -0.00003 0.00004 -0.74728 0.00002 0.00002 0.00000 0.00000 -0.00000 0.00000 ...
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0.00000 -0.00000 -0.00003 -0.00095 0.00003 0.00002 -0.74622 0.00003 0.00000 0.00000 0.00000 0.00000 ...
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0.00000 0.00000 0.00004 0.00003 -0.00162 0.00002 0.00003 -0.74670 0.00000 0.00000 -0.00000 0.00000 ...
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0.00002 -0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 -0.41311 0.00002 -0.00003 -0.00001 ...
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0.00001 0.00001 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00002 -0.41250 -0.00001 0.00003 ...
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0.00043 0.00003 -0.00000 0.00000 -0.00000 -0.00000 0.00000 -0.00000 -0.00003 -0.00001 -0.41212 0.00001 ...
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0.00002 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 -0.00001 0.00003 0.00001 -0.41222 ...
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... only 12 components have been written...
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Total pseudopotential strength Dij (eV):
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20.53089 -0.79194 -0.00000 -0.00000 -0.00000 0.00000 0.00000 0.00000 0.00062 0.00037 0.01171 0.00066 ...
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-0.79194 0.79118 0.00000 0.00000 0.00000 0.00000 -0.00000 0.00000 -0.00001 0.00014 0.00073 0.00008 ...
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-0.00000 0.00000 -20.00366 0.00119 -0.00018 -0.05277 -0.00070 0.00108 0.00000 0.00000 -0.00000 0.00000 ...
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-0.00000 0.00000 0.00119 -19.98504 0.00042 -0.00070 -0.02591 0.00069 0.00000 0.00000 0.00000 0.00000 ...
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-0.00000 0.00000 -0.00018 0.00042 -19.98999 0.00108 0.00069 -0.04406 0.00000 0.00000 -0.00000 0.00000 ...
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0.00000 0.00000 -0.05277 -0.00070 0.00108 -20.33458 0.00066 0.00057 0.00000 0.00000 -0.00000 0.00000 ...
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0.00000 -0.00000 -0.00070 -0.02591 0.00069 0.00066 -20.30559 0.00080 0.00000 0.00000 0.00000 0.00000 ...
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0.00000 0.00000 0.00108 0.00069 -0.04406 0.00057 0.00080 -20.31873 0.00000 0.00000 -0.00000 0.00000 ...
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0.00062 -0.00001 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 -11.24118 0.00067 -0.00092 -0.00017 ...
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0.00037 0.00014 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 0.00067 -11.22459 -0.00023 0.00086 ...
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0.01171 0.00073 -0.00000 0.00000 -0.00000 -0.00000 0.00000 -0.00000 -0.00092 -0.00023 -11.21424 0.00032 ...
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0.00066 0.00008 0.00000 0.00000 0.00000 0.00000 0.00000 0.00000 -0.00017 0.00086 0.00032 -11.21716 ...
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... only 12 components have been written...
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Augmentation waves occupancies Rhoij:
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1.55020 0.55439 -0.00000 -0.00000 0.00000 -0.00000 0.00000 0.00000 0.01590 -0.00784 0.06498 0.00508 ...
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0.55439 0.34042 -0.00000 -0.00000 -0.00000 0.00000 -0.00000 -0.00000 0.00289 -0.00365 -0.04145 0.00186 ...
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-0.00000 -0.00000 0.74749 0.01233 -0.01852 0.23496 0.00114 -0.00361 -0.00000 -0.00000 0.00000 0.00000 ...
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-0.00000 -0.00000 0.01233 0.70740 -0.00690 0.00126 0.22595 -0.00165 0.00000 -0.00000 -0.00000 -0.00000 ...
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0.00000 -0.00000 -0.01852 -0.00690 0.84897 -0.00401 -0.00249 0.25157 -0.00000 0.00000 0.00000 -0.00000 ...
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-0.00000 0.00000 0.23496 0.00126 -0.00401 0.07398 -0.00037 -0.00052 -0.00000 -0.00000 0.00000 0.00000 ...
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0.00000 -0.00000 0.00114 0.22595 -0.00249 -0.00037 0.07230 -0.00061 0.00000 -0.00000 -0.00000 -0.00000 ...
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0.00000 -0.00000 -0.00361 -0.00165 0.25157 -0.00052 -0.00061 0.07543 -0.00000 0.00000 0.00000 -0.00000 ...
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0.01590 0.00289 -0.00000 0.00000 -0.00000 -0.00000 0.00000 -0.00000 0.00919 0.00448 0.00075 0.00794 ...
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-0.00784 -0.00365 -0.00000 -0.00000 0.00000 -0.00000 -0.00000 0.00000 0.00448 0.00696 0.00276 0.00473 ...
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0.06498 -0.04145 0.00000 -0.00000 0.00000 0.00000 -0.00000 0.00000 0.00075 0.00276 0.14531 0.00408 ...
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0.00508 0.00186 0.00000 -0.00000 -0.00000 0.00000 -0.00000 -0.00000 0.00794 0.00473 0.00408 0.00924 ...
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... only 12 components have been written...
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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= 28.740E-18; max= 33.083E-17
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reduced coordinates (array xred) for 1 atoms
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0.000000000000 0.000000000000 0.000000000000
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rms dE/dt= 1.7359E-06; max dE/dt= 2.5353E-06; dE/dt below (all hartree)
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1 0.000001424020 0.000000764069 0.000002535337
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cartesian coordinates (angstrom) at end:
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1 0.00000000000000 0.00000000000000 0.00000000000000
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cartesian forces (hartree/bohr) at end:
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1 0.00000000000000 0.00000000000000 0.00000000000000
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frms,max,avg= 0.0000000E+00 0.0000000E+00 -3.391E-07 -1.559E-07 -4.527E-07 h/b
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cartesian forces (eV/Angstrom) at end:
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1 0.00000000000000 0.00000000000000 0.00000000000000
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frms,max,avg= 0.0000000E+00 0.0000000E+00 -1.743E-05 -8.018E-06 -2.328E-05 e/A
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length scales= 3.000000000000 3.500000000000 4.000000000000 bohr
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= 1.587531625770 1.852120230065 2.116708834360 angstroms
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prteigrs : about to open file t94o_EIG
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Fermi (or HOMO) energy (hartree) = 0.41157 Average Vxc (hartree)= -0.44494
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Eigenvalues (hartree) for nkpt= 2 k points:
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kpt# 1, nband= 6, wtk= 0.50000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
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-1.55527 -0.37623 -0.36794 -0.33598 0.20462 0.40006
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occupation numbers for kpt# 1
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2.00000 2.00000 2.00000 2.00000 2.00000 1.58426
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prteigrs : prtvol=0 or 1, do not print more k-points.
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Fermi (or HOMO) energy (eV) = 11.19946 Average Vxc (eV)= -12.10742
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Eigenvalues ( eV ) for nkpt= 2 k points:
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kpt# 1, nband= 6, wtk= 0.50000, kpt= 0.0000 0.0000 0.0000 (reduced coord)
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-42.32109 -10.23775 -10.01210 -9.14258 5.56789 10.88627
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prteigrs : prtvol=0 or 1, do not print more k-points.
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--- !EnergyTerms
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iteration_state : {dtset: 1, }
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comment : Components of total free energy in Hartree
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kinetic : 1.06069714067113E+01
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hartree : 3.63129200504840E+00
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xc : -4.54807366711236E+00
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Ewald energy : -2.85262776194305E+01
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psp_core : 2.16104697573995E+00
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local_psp : -1.45196812008668E+01
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spherical_terms : -2.05130611360355E+00
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internal : -3.32460282135136E+01
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'-kT*entropy' : -8.10280238900790E-03
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total_energy : -3.32541310159026E+01
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total_energy_eV : -9.04890924004457E+02
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...
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--- !EnergyTermsDC
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iteration_state : {dtset: 1, }
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comment : '"Double-counting" decomposition of free energy'
|
|
band_energy : -4.77728500973845E+00
|
|
Ewald energy : -2.85262776194305E+01
|
|
psp_core : 2.16104697573995E+00
|
|
xc_dc : -2.22852717346934E+00
|
|
spherical_terms : 1.24994328556784E-01
|
|
internal : -3.32460484983416E+01
|
|
'-kT*entropy' : -8.10280238900790E-03
|
|
total_energy_dc : -3.32541513007306E+01
|
|
total_energy_dc_eV : -9.04891475982698E+02
|
|
...
|
|
|
|
|
|
Cartesian components of stress tensor (hartree/bohr^3)
|
|
sigma(1 1)= 2.69450250E-02 sigma(3 2)= -6.15460434E-04
|
|
sigma(2 2)= 3.30137604E-02 sigma(3 1)= 2.80919398E-04
|
|
sigma(3 3)= 3.62581461E-02 sigma(2 1)= 9.84965337E-04
|
|
|
|
-Cartesian components of stress tensor (GPa) [Pressure= -9.4360E+02 GPa]
|
|
- sigma(1 1)= 7.92749873E+02 sigma(3 2)= -1.81074681E+01
|
|
- sigma(2 2)= 9.71298202E+02 sigma(3 1)= 8.26493263E+00
|
|
- sigma(3 3)= 1.06675131E+03 sigma(2 1)= 2.89786758E+01
|
|
|
|
== END DATASET(S) ==============================================================
|
|
================================================================================
|
|
|
|
-outvars: echo values of variables after computation --------
|
|
acell 3.0000000000E+00 3.5000000000E+00 4.0000000000E+00 Bohr
|
|
amu 4.00780000E+01
|
|
densfor_pred 0
|
|
ecut 3.00000000E+00 Hartree
|
|
enunit 2
|
|
etotal -3.3254151301E+01
|
|
fcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
- fftalg 400
|
|
istwfk 2 0
|
|
ixc 7
|
|
kpt 0.00000000E+00 0.00000000E+00 0.00000000E+00
|
|
3.00000000E-01 3.00000000E-01 3.00000000E-01
|
|
kptopt 0
|
|
P mkmem 2
|
|
natom 1
|
|
nband 6
|
|
nbdblock 2
|
|
ngfft 8 8 10
|
|
ngfftdg 16 18 20
|
|
nkpt 2
|
|
nline 10
|
|
nblock_lobpcg 6
|
|
nnsclo 1
|
|
nstep 25
|
|
nsym 1
|
|
ntime 5
|
|
ntypat 1
|
|
occ 2.000000 2.000000 2.000000 2.000000 2.000000 1.584257
|
|
2.000000 2.000000 2.000000 2.000000 0.415743 0.000000
|
|
occopt 7
|
|
ortalg 1
|
|
pawecutdg 1.50000000E+01 Hartree
|
|
pawmixdg 1
|
|
prtwf 0
|
|
rprim 1.4000000000E+00 0.0000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 1.4000000000E+00 0.0000000000E+00
|
|
0.0000000000E+00 0.0000000000E+00 1.4000000000E+00
|
|
spgroup 1
|
|
strten 2.6945025046E-02 3.3013760430E-02 3.6258146065E-02
|
|
-6.1546043441E-04 2.8091939758E-04 9.8496533690E-04
|
|
toldfe 1.00000000E-08 Hartree
|
|
tsmear 2.00000000E-02 Hartree
|
|
typat 1
|
|
useylm 1
|
|
wfoptalg 4
|
|
wtk 0.50000 0.50000
|
|
znucl 20.00000
|
|
|
|
================================================================================
|
|
|
|
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] Implementation of the Projector Augmented-Wave Method in the ABINIT code.
|
|
- M. Torrent, F. Jollet, F. Bottin, G. Zerah, and X. Gonze Comput. Mat. Science 42, 337, (2008).
|
|
- Comment: PAW calculations. Strong suggestion to cite this paper.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#torrent2008
|
|
-
|
|
- [2] The Abinit project: Impact, environment and recent developments.
|
|
- Computer Phys. Comm. 248, 107042 (2020).
|
|
- X.Gonze, B. Amadon, G. Antonius, F.Arnardi, L.Baguet, J.-M.Beuken,
|
|
- J.Bieder, F.Bottin, J.Bouchet, E.Bousquet, N.Brouwer, F.Bruneval,
|
|
- G.Brunin, T.Cavignac, J.-B. Charraud, Wei Chen, M.Cote, S.Cottenier,
|
|
- J.Denier, G.Geneste, Ph.Ghosez, M.Giantomassi, Y.Gillet, O.Gingras,
|
|
- D.R.Hamann, G.Hautier, Xu He, N.Helbig, N.Holzwarth, Y.Jia, F.Jollet,
|
|
- W.Lafargue-Dit-Hauret, K.Lejaeghere, M.A.L.Marques, A.Martin, C.Martins,
|
|
- H.P.C. Miranda, F.Naccarato, K. Persson, G.Petretto, V.Planes, Y.Pouillon,
|
|
- S.Prokhorenko, F.Ricci, G.-M.Rignanese, A.H.Romero, M.M.Schmitt, M.Torrent,
|
|
- M.J.van Setten, B.Van Troeye, M.J.Verstraete, G.Zerah and J.W.Zwanzig
|
|
- Comment: the fifth generic paper describing the ABINIT project.
|
|
- Note that a version of this paper, that is not formatted for Computer Phys. Comm.
|
|
- is available at https://www.abinit.org/sites/default/files/ABINIT20.pdf .
|
|
- The licence allows the authors to put it on the Web.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze2020
|
|
-
|
|
- [3] ABINIT: Overview, and focus on selected capabilities
|
|
- J. Chem. Phys. 152, 124102 (2020).
|
|
- A. Romero, D.C. Allan, B. Amadon, G. Antonius, T. Applencourt, L.Baguet,
|
|
- J.Bieder, F.Bottin, J.Bouchet, E.Bousquet, F.Bruneval,
|
|
- G.Brunin, D.Caliste, M.Cote,
|
|
- J.Denier, C. Dreyer, Ph.Ghosez, M.Giantomassi, Y.Gillet, O.Gingras,
|
|
- D.R.Hamann, G.Hautier, F.Jollet, G. Jomard,
|
|
- A.Martin,
|
|
- H.P.C. Miranda, F.Naccarato, G.Petretto, N.A. Pike, V.Planes,
|
|
- S.Prokhorenko, T. Rangel, F.Ricci, G.-M.Rignanese, M.Royo, M.Stengel, M.Torrent,
|
|
- M.J.van Setten, B.Van Troeye, M.J.Verstraete, J.Wiktor, J.W.Zwanziger, and X.Gonze.
|
|
- Comment: a global overview of ABINIT, with focus on selected capabilities .
|
|
- Note that a version of this paper, that is not formatted for J. Chem. Phys
|
|
- is available at https://www.abinit.org/sites/default/files/ABINIT20_JPC.pdf .
|
|
- The licence allows the authors to put it on the Web.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#romero2020
|
|
-
|
|
- [4] Recent developments in the ABINIT software package.
|
|
- Computer Phys. Comm. 205, 106 (2016).
|
|
- X.Gonze, F.Jollet, F.Abreu Araujo, D.Adams, B.Amadon, T.Applencourt,
|
|
- C.Audouze, J.-M.Beuken, J.Bieder, A.Bokhanchuk, E.Bousquet, F.Bruneval
|
|
- D.Caliste, M.Cote, F.Dahm, F.Da Pieve, M.Delaveau, M.Di Gennaro,
|
|
- B.Dorado, C.Espejo, G.Geneste, L.Genovese, A.Gerossier, M.Giantomassi,
|
|
- Y.Gillet, D.R.Hamann, L.He, G.Jomard, J.Laflamme Janssen, S.Le Roux,
|
|
- A.Levitt, A.Lherbier, F.Liu, I.Lukacevic, A.Martin, C.Martins,
|
|
- M.J.T.Oliveira, S.Ponce, Y.Pouillon, T.Rangel, G.-M.Rignanese,
|
|
- A.H.Romero, B.Rousseau, O.Rubel, A.A.Shukri, M.Stankovski, M.Torrent,
|
|
- M.J.Van Setten, B.Van Troeye, M.J.Verstraete, D.Waroquier, J.Wiktor,
|
|
- B.Xu, A.Zhou, J.W.Zwanziger.
|
|
- Comment: the fourth generic paper describing the ABINIT project.
|
|
- Note that a version of this paper, that is not formatted for Computer Phys. Comm.
|
|
- is available at https://www.abinit.org/sites/default/files/ABINIT16.pdf .
|
|
- The licence allows the authors to put it on the Web.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze2016
|
|
-
|
|
- And optionally:
|
|
-
|
|
- [5] ABINIT: First-principles approach of materials and nanosystem properties.
|
|
- Computer Phys. Comm. 180, 2582-2615 (2009).
|
|
- X. Gonze, B. Amadon, P.-M. Anglade, J.-M. Beuken, F. Bottin, P. Boulanger, F. Bruneval,
|
|
- D. Caliste, R. Caracas, M. Cote, T. Deutsch, L. Genovese, Ph. Ghosez, M. Giantomassi
|
|
- S. Goedecker, D.R. Hamann, P. Hermet, F. Jollet, G. Jomard, S. Leroux, M. Mancini, S. Mazevet,
|
|
- M.J.T. Oliveira, G. Onida, Y. Pouillon, T. Rangel, G.-M. Rignanese, D. Sangalli, R. Shaltaf,
|
|
- M. Torrent, M.J. Verstraete, G. Zerah, J.W. Zwanziger
|
|
- Comment: the third generic paper describing the ABINIT project.
|
|
- Note that a version of this paper, that is not formatted for Computer Phys. Comm.
|
|
- is available at https://www.abinit.org/sites/default/files/ABINIT_CPC_v10.pdf .
|
|
- The licence allows the authors to put it on the Web.
|
|
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze2009
|
|
-
|
|
- Proc. 0 individual time (sec): cpu= 0.6 wall= 0.6
|
|
|
|
================================================================================
|
|
|
|
Calculation completed.
|
|
.Delivered 9 WARNINGs and 3 COMMENTs to log file.
|
|
+Overall time at end (sec) : cpu= 0.6 wall= 0.6
|