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.Version 10.1.4.5 of ABINIT, released Sep 2024.
.(MPI version, prepared for a x86_64_linux_gnu13.2 computer)
.Copyright (C) 1998-2025 ABINIT group .
ABINIT comes with ABSOLUTELY NO WARRANTY.
It is free software, and you are welcome to redistribute it
under certain conditions (GNU General Public License,
see ~abinit/COPYING or http://www.gnu.org/copyleft/gpl.txt).
ABINIT is a project of the Universite Catholique de Louvain,
Corning Inc. and other collaborators, see ~abinit/doc/developers/contributors.txt .
Please read https://docs.abinit.org/theory/acknowledgments for suggested
acknowledgments of the ABINIT effort.
For more information, see https://www.abinit.org .
.Starting date : Fri 13 Sep 2024.
- ( at 19h08 )
- input file -> /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/TestBot_MPI1/v2_t05/t05.abi
- output file -> t05.abo
- root for input files -> t05i
- root for output files -> t05o
DATASET 1 : space group P1 (# 1); Bravais aP (primitive triclinic)
================================================================================
Values of the parameters that define the memory need for DATASET 1.
intxc = 0 ionmov = 0 iscf = 7 lmnmax = 2
lnmax = 2 mgfft = 16 mpssoang = 3 mqgrid = 3001
natom = 2 nloc_mem = 1 nspden = 1 nspinor = 1
nsppol = 1 nsym = 1 n1xccc = 0 ntypat = 1
occopt = 1 xclevel = 1
- mband = 4 mffmem = 1 mkmem = 2
mpw = 172 nfft = 4096 nkpt = 2
For the susceptibility and dielectric matrices, or tddft :
mgfft = 12 nbnd_in_blk= 2 nfft = 1200 npw = 83
================================================================================
P This job should need less than 1.827 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.023 Mbytes ; DEN or POT disk file : 0.033 Mbytes.
================================================================================
DATASET 2 : space group P1 (# 1); Bravais aP (primitive triclinic)
================================================================================
Values of the parameters that define the memory need for DATASET 2 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 2
nloc_mem = 1 nspden = 1 nspinor = 1 nsppol = 1
nsym = 1 n1xccc = 0 ntypat = 1 occopt = 1
xclevel = 1
- mband = 4 mffmem = 1 mkmem = 2
- mkqmem = 2 mk1mem = 2 mpw = 172
nfft = 4096 nkpt = 2
================================================================================
P This job should need less than 1.378 Mbytes of memory.
P Max. in main chain + fourwf.f
P 18 blocks of mpw integer numbers, for 0.012 Mbytes.
P 108 blocks of mpw real(dp) numbers, for 0.142 Mbytes.
P 25 blocks of nfft real(dp) numbers, for 0.781 Mbytes.
P Additional real(dp) numbers, for 0.205 Mbytes.
P With residue estimated to be 0.237 Mbytes.
P
P Comparison of the memory needs of different chains
P Main chain + fourwf.f 1.378 Mbytes.
P Main chain + nonlop.f + opernl.f 1.314 Mbytes.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.023 Mbytes ; DEN or POT disk file : 0.033 Mbytes.
================================================================================
DATASET 3 : space group P1 (# 1); Bravais aP (primitive triclinic)
================================================================================
Values of the parameters that define the memory need for DATASET 3 (RF).
intxc = 0 iscf = 7 lmnmax = 2 lnmax = 2
mgfft = 16 mpssoang = 3 mqgrid = 3001 natom = 2
nloc_mem = 1 nspden = 1 nspinor = 1 nsppol = 1
nsym = 1 n1xccc = 0 ntypat = 1 occopt = 1
xclevel = 1
- mband = 4 mffmem = 1 mkmem = 2
- mkqmem = 2 mk1mem = 2 mpw = 172
nfft = 4096 nkpt = 2
================================================================================
P This job should need less than 1.378 Mbytes of memory.
P Max. in main chain + fourwf.f
P 18 blocks of mpw integer numbers, for 0.012 Mbytes.
P 108 blocks of mpw real(dp) numbers, for 0.142 Mbytes.
P 25 blocks of nfft real(dp) numbers, for 0.781 Mbytes.
P Additional real(dp) numbers, for 0.205 Mbytes.
P With residue estimated to be 0.237 Mbytes.
P
P Comparison of the memory needs of different chains
P Main chain + fourwf.f 1.378 Mbytes.
P Main chain + nonlop.f + opernl.f 1.314 Mbytes.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 0.023 Mbytes ; DEN or POT disk file : 0.033 Mbytes.
================================================================================
--------------------------------------------------------------------------------
------------- Echo of variables that govern the present computation ------------
--------------------------------------------------------------------------------
-
- outvars: echo of selected default values
- iomode0 = 0 , fftalg0 =512 , wfoptalg0 = 0
-
- outvars: echo of global parameters not present in the input file
- max_nthreads = 0
-
-outvars: echo values of preprocessed input variables --------
acell 1.0000000000E+01 1.0000000000E+01 1.2500000000E+01 Bohr
amu 1.00000000E+00
asr 0
chneut 0
diecut 1.20000000E+00 Hartree
diegap 2.00000000E-01 Hartree
diemac1 1.00000000E+06
diemac2 1.00000000E+06
diemac3 1.00000000E+00
diemix1 1.00000000E+00
diemix2 1.00000000E+00
diemix3 7.00000000E-01
ecut 2.00000000E+00 Hartree
- fftalg 512
getddk1 0
getddk2 2
getddk3 2
getwfk1 0
getwfk2 1
getwfk3 1
iprcel 45
ixc 3
jdtset 1 2 3
kpt 0.00000000E+00 0.00000000E+00 1.25000000E-01
0.00000000E+00 0.00000000E+00 3.75000000E-01
kptopt 0
P mkmem 2
P mkqmem 2
P mk1mem 2
natom 2
nband 4
ndtset 3
ngfft 16 16 16
nkpt 2
nqpt1 0
nqpt2 1
nqpt3 1
nstep1 30
nstep2 30
nstep3 25
nsym 1
ntypat 1
occ 2.000000 2.000000 2.000000 2.000000
optdriver1 0
optdriver2 1
optdriver3 1
prtpot1 0
prtpot2 1
prtpot3 1
prtvol1 0
prtvol2 10
prtvol3 10
rfatpol1 1 2
rfatpol2 2 2
rfatpol3 2 2
rfdir1 1 1 1
rfdir2 0 0 1
rfdir3 0 0 1
rfelfd1 0
rfelfd2 2
rfelfd3 3
rfphon1 0
rfphon2 0
rfphon3 1
spgroup 1
tolwfr1 1.00000000E-22
tolwfr2 1.00000000E-22
tolwfr3 1.00000000E-15
typat 1 1
wtk 0.50000 0.50000
xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 1.3229430215E+00
xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 2.5000000000E+00
xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 2.0000000000E-01
znucl 14.00000
================================================================================
chkinp: Checking input parameters for consistency, jdtset= 1.
chkinp: Checking input parameters for consistency, jdtset= 2.
chkinp: Checking input parameters for consistency, jdtset= 3.
================================================================================
== DATASET 1 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 1, }
dimensions: {natom: 2, nkpt: 2, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 172, }
cutoff_energies: {ecut: 2.0, pawecutdg: -1.0, }
electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
meta: {optdriver: 0, ionmov: 0, optcell: 0, iscf: 7, paral_kgb: 0, }
...
Exchange-correlation functional for the present dataset will be:
LDA: old Teter (4/91) fit to Ceperley-Alder data - ixc=3
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 10.0000000 0.0000000 0.0000000 G(1)= 0.1000000 0.0000000 0.0000000
R(2)= 0.0000000 10.0000000 0.0000000 G(2)= 0.0000000 0.1000000 0.0000000
R(3)= 0.0000000 0.0000000 12.5000000 G(3)= 0.0000000 0.0000000 0.0800000
Unit cell volume ucvol= 1.2500000E+03 bohr^3
Angles (23,13,12)= 9.00000000E+01 9.00000000E+01 9.00000000E+01 degrees
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 2.000 => boxcut(ratio)= 2.01062
--- Pseudopotential description ------------------------------------------------
- pspini: atom type 1 psp file is /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/14si.Hamann_mod
- pspatm: opening atomic psp file /home/buildbot/ABINIT3/eos_gnu_13.2_mpich/trunk_merge-10.0/tests/Pspdir/14si.Hamann_mod
- Si psp produced from Hamann's atompp on 14 Feb 1990 ( !! OLD, for tests only )
- 14.00000 4.00000 900214 znucl, zion, pspdat
5 3 2 0 770 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
1.000000E-06 2.357045E-02 r1 and al (Hamman grid)
0 0.000 0.000 0 1.0529960 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
1 0.000 0.000 1 1.2715070 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
2 0.000 0.000 1 1.2715070 l,e99.0,e99.9,nproj,rcpsp
0.00000000 0.00000000 0.00000000 0.00000000 rms, ekb1, ekb2, epsatm
0.00000000000000 0.00000000000000 0.00000000000000 rchrg,fchrg,qchrg
pspatm : epsatm= 28.17357484
--- l ekb(1:nproj) -->
1 -2.083263
2 -1.959803
pspatm: atomic psp has been read and splines computed
4.50777197E+02 ecore*ucvol(ha*bohr**3)
--------------------------------------------------------------------------------
_setup2: Arith. and geom. avg. npw (full set) are 166.000 165.892
================================================================================
--- !BeginCycle
iteration_state: {dtset: 1, }
solver: {iscf: 7, nstep: 30, nline: 4, wfoptalg: 0, }
tolerances: {tolwfr: 1.00E-22, }
...
iter Etot(hartree) deltaE(h) residm vres2
ETOT 1 -6.6119032759329 -6.612E+00 2.813E-03 1.318E+01
ETOT 2 -6.6498347740658 -3.793E-02 7.790E-07 7.780E-02
ETOT 3 -6.6499679700361 -1.332E-04 1.014E-06 5.986E-03
ETOT 4 -6.6499813731127 -1.340E-05 2.794E-07 2.548E-03
ETOT 5 -6.6499917067470 -1.033E-05 6.847E-08 1.755E-04
ETOT 6 -6.6499924689013 -7.622E-07 3.987E-09 8.508E-07
ETOT 7 -6.6499924737567 -4.855E-09 2.109E-11 7.961E-09
ETOT 8 -6.6499924737995 -4.280E-11 8.178E-14 2.366E-10
ETOT 9 -6.6499924738005 -9.965E-13 1.871E-14 3.387E-11
ETOT 10 -6.6499924738006 -9.681E-14 6.017E-16 1.194E-12
ETOT 11 -6.6499924738006 -2.043E-14 1.046E-16 4.695E-14
ETOT 12 -6.6499924738006 -1.510E-14 6.202E-19 2.611E-15
ETOT 13 -6.6499924738007 -2.309E-14 8.403E-20 3.124E-16
ETOT 14 -6.6499924738006 3.109E-14 5.399E-21 4.587E-18
ETOT 15 -6.6499924738006 -6.217E-15 2.805E-22 1.714E-18
ETOT 16 -6.6499924738006 1.510E-14 8.589E-23 2.600E-19
At SCF step 16 max residual= 8.59E-23 < tolwfr= 1.00E-22 =>converged.
Cartesian components of stress tensor (hartree/bohr^3)
sigma(1 1)= 3.12986279E-04 sigma(3 2)= 0.00000000E+00
sigma(2 2)= 3.12986279E-04 sigma(3 1)= -1.77315749E-15
sigma(3 3)= -2.52556365E-03 sigma(2 1)= 3.58198459E-15
--- !ResultsGS
iteration_state: {dtset: 1, }
comment : Summary of ground state results
lattice_vectors:
- [ 10.0000000, 0.0000000, 0.0000000, ]
- [ 0.0000000, 10.0000000, 0.0000000, ]
- [ 0.0000000, 0.0000000, 12.5000000, ]
lattice_lengths: [ 10.00000, 10.00000, 12.50000, ]
lattice_angles: [ 90.000, 90.000, 90.000, ] # degrees, (23, 13, 12)
lattice_volume: 1.2500000E+03
convergence: {deltae: 1.510E-14, res2: 2.600E-19, residm: 8.589E-23, diffor: null, }
etotal : -6.64999247E+00
entropy : 0.00000000E+00
fermie : -2.16518912E-01
cartesian_stress_tensor: # hartree/bohr^3
- [ 3.12986279E-04, 3.58198459E-15, -1.77315749E-15, ]
- [ 3.58198459E-15, 3.12986279E-04, 0.00000000E+00, ]
- [ -1.77315749E-15, 0.00000000E+00, -2.52556365E-03, ]
pressure_GPa: 1.8629E+01
xred :
- [ 0.0000E+00, 0.0000E+00, 0.0000E+00, Si]
- [ 0.0000E+00, 0.0000E+00, 2.0000E-01, Si]
cartesian_forces: # hartree/bohr
- [ -1.77691326E-13, -1.62722079E-13, -1.39442274E+00, ]
- [ 1.77691326E-13, 1.62722079E-13, 1.39442274E+00, ]
force_length_stats: {min: 1.39442274E+00, max: 1.39442274E+00, mean: 1.39442274E+00, }
...
Integrated electronic density in atomic spheres:
------------------------------------------------
Atom Sphere_radius Integrated_density
1 2.00000 1.89115348
2 2.00000 2.04399159
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 63.060E-24; max= 85.889E-24
reduced coordinates (array xred) for 2 atoms
0.000000000000 0.000000000000 0.000000000000
0.000000000000 0.000000000000 0.200000000000
rms dE/dt= 1.0063E+01; max dE/dt= 1.7430E+01; dE/dt below (all hartree)
1 -0.000000000051 0.000000000048 17.430276891135
2 -0.000000000054 0.000000000044 -17.430291595222
cartesian coordinates (angstrom) at end:
1 0.00000000000000 0.00000000000000 0.00000000000000
2 0.00000000000000 0.00000000000000 1.32294302147500
cartesian forces (hartree/bohr) at end:
1 -0.00000000000018 -0.00000000000016 -1.39442273945428
2 0.00000000000018 0.00000000000016 1.39442273945428
frms,max,avg= 8.0507034E-01 1.3944227E+00 5.243E-12 -4.601E-12 5.882E-07 h/b
cartesian forces (eV/Angstrom) at end:
1 -0.00000000000914 -0.00000000000837 -71.70409422489304
2 0.00000000000914 0.00000000000837 71.70409422489304
frms,max,avg= 4.1398378E+01 7.1704094E+01 2.696E-10 -2.366E-10 3.024E-05 e/A
length scales= 10.000000000000 10.000000000000 12.500000000000 bohr
= 5.291772085900 5.291772085900 6.614715107375 angstroms
prteigrs : about to open file t05o_DS1_EIG
Fermi (or HOMO) energy (hartree) = -0.21652 Average Vxc (hartree)= -0.14741
Eigenvalues (hartree) for nkpt= 2 k points:
kpt# 1, nband= 4, wtk= 0.50000, kpt= 0.0000 0.0000 0.1250 (reduced coord)
-0.46036 -0.22810 -0.22810 -0.21652
prteigrs : prtvol=0 or 1, do not print more k-points.
--- !EnergyTerms
iteration_state : {dtset: 1, }
comment : Components of total free energy in Hartree
kinetic : 2.96063057516736E+00
hartree : 3.61408459242119E+00
xc : -2.28228607110879E+00
Ewald energy : -1.81143676288751E+00
psp_core : 3.60621757934793E-01
local_psp : -9.27524992720742E+00
non_local_psp : -2.16356638120233E-01
total_energy : -6.64999247380062E+00
total_energy_eV : -1.80955497870700E+02
band_energy : -2.27894887944559E+00
...
Cartesian components of stress tensor (hartree/bohr^3)
sigma(1 1)= 3.12986279E-04 sigma(3 2)= 0.00000000E+00
sigma(2 2)= 3.12986279E-04 sigma(3 1)= -1.77315749E-15
sigma(3 3)= -2.52556365E-03 sigma(2 1)= 3.58198459E-15
-Cartesian components of stress tensor (GPa) [Pressure= 1.8629E+01 GPa]
- sigma(1 1)= 9.20837270E+00 sigma(3 2)= 0.00000000E+00
- sigma(2 2)= 9.20837270E+00 sigma(3 1)= -5.21680857E-11
- sigma(3 3)= -7.43046354E+01 sigma(2 1)= 1.05385607E-10
================================================================================
== DATASET 2 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 2, }
dimensions: {natom: 2, nkpt: 2, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 172, }
cutoff_energies: {ecut: 2.0, pawecutdg: -1.0, }
electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
meta: {optdriver: 1, rfelfd: 2, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
mkfilename : getddk/=0, take file _1WF from output of DATASET 2.
Exchange-correlation functional for the present dataset will be:
LDA: old Teter (4/91) fit to Ceperley-Alder data - ixc=3
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 10.0000000 0.0000000 0.0000000 G(1)= 0.1000000 0.0000000 0.0000000
R(2)= 0.0000000 10.0000000 0.0000000 G(2)= 0.0000000 0.1000000 0.0000000
R(3)= 0.0000000 0.0000000 12.5000000 G(3)= 0.0000000 0.0000000 0.0800000
Unit cell volume ucvol= 1.2500000E+03 bohr^3
Angles (23,13,12)= 9.00000000E+01 9.00000000E+01 9.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 2.000 => boxcut(ratio)= 2.01062
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 3 ipert= 3
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Perturbation : derivative vs k along direction 3
dfpt_looppert : COMMENT -
In a d/dk calculation, iscf is set to -3 automatically.
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: 30, nline: 4, wfoptalg: 0, }
tolerances: {tolwfr: 1.00E-22, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 -1.8511443997815 -1.851E+00 9.945E-03 0.000E+00
ETOT 2 -1.8548471238747 -3.703E-03 3.265E-06 0.000E+00
ETOT 3 -1.8548648790560 -1.776E-05 2.622E-07 0.000E+00
ETOT 4 -1.8548649901112 -1.111E-07 1.697E-10 0.000E+00
ETOT 5 -1.8548649908854 -7.742E-10 1.432E-11 0.000E+00
ETOT 6 -1.8548649908912 -5.877E-12 1.050E-14 0.000E+00
ETOT 7 -1.8548649908913 -2.909E-14 8.653E-16 0.000E+00
ETOT 8 -1.8548649908913 -2.109E-14 7.570E-19 0.000E+00
ETOT 9 -1.8548649908913 7.105E-15 5.768E-20 0.000E+00
ETOT 10 -1.8548649908913 1.776E-15 8.365E-23 0.000E+00
At SCF step 10 max residual= 8.37E-23 < tolwfr= 1.00E-22 =>converged.
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 58.865E-24; max= 83.654E-24
0.0000 0.0000 0.1250 1 8.36543E-23 kpt; spin; max resid(k); each band:
7.53E-23 8.37E-23 8.37E-23 5.14E-23
0.0000 0.0000 0.3750 1 6.29739E-23 kpt; spin; max resid(k); each band:
4.39E-23 6.30E-23 3.50E-23 3.50E-23
dfpt_looppert : ek2= 4.0425899627E+00
f-sum rule ratio= 9.9240807077E-01
prteigrs : about to open file t05t_1WF1_EIG
Expectation of eigenvalue derivatives (hartree) for nkpt= 2 k points:
(in case of degenerate eigenvalues, averaged derivative)
kpt# 1, nband= 4, wtk= 0.50000, kpt= 0.0000 0.0000 0.1250 (reduced coord)
0.00123 0.00300 0.00300 -0.03044
kpt# 2, nband= 4, wtk= 0.50000, kpt= 0.0000 0.0000 0.3750 (reduced coord)
0.00156 -0.02106 0.00154 0.00154
Eight components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 5.56513521E+00 eigvalue= 2.98774247E+00 local= -6.31641065E+00
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
kin1= -4.01189891E+00 Hartree= 0.00000000E+00 xc= 0.00000000E+00
7,8,9: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= -3.81602042E-01 enl1= 3.02168924E-01
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -1.85486499E+00
No Ewald or frozen-wf contrib.: the relaxation energy is the total one
2DEtotal= -0.1854864991E+01 Ha. Also 2DEtotal= -0.504734432756E+02 eV
( non-var. 2DEtotal : -1.8548649909E+00 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
Total localisation tensor (bohr^2) in cartesian coordinates
WARNING : still subject to testing - especially symmetries.
direction matrix element
alpha beta real part imaginary part
1 1 0.0000000000 0.0000000000
1 2 0.0000000000 0.0000000000
1 3 0.0000000000 0.0000000000
2 1 0.0000000000 0.0000000000
2 2 0.0000000000 0.0000000000
2 3 0.0000000000 0.0000000000
3 1 0.0000000000 0.0000000000
3 2 0.0000000000 0.0000000000
3 3 3.3224058685 0.0000000000
WARNING : Localization tensor calculation (this does not apply to other properties).
Not all d/dk perturbations were computed. So the localization tensor in reciprocal space is incomplete,
and transformation to cartesian coordinates may be wrong. Check input variable rfdir.
respfn : d/dk was computed, but no 2DTE, so no DDB output.
================================================================================
== DATASET 3 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 3, }
dimensions: {natom: 2, nkpt: 2, mband: 4, nsppol: 1, nspinor: 1, nspden: 1, mpw: 172, }
cutoff_energies: {ecut: 2.0, pawecutdg: -1.0, }
electrons: {nelect: 8.00000000E+00, charge: 0.00000000E+00, occopt: 1.00000000E+00, tsmear: 1.00000000E-02, }
meta: {optdriver: 1, rfelfd: 3, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
mkfilename : getddk/=0, take file _1WF from output of DATASET 2.
Exchange-correlation functional for the present dataset will be:
LDA: old Teter (4/91) fit to Ceperley-Alder data - ixc=3
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= 10.0000000 0.0000000 0.0000000 G(1)= 0.1000000 0.0000000 0.0000000
R(2)= 0.0000000 10.0000000 0.0000000 G(2)= 0.0000000 0.1000000 0.0000000
R(3)= 0.0000000 0.0000000 12.5000000 G(3)= 0.0000000 0.0000000 0.0800000
Unit cell volume ucvol= 1.2500000E+03 bohr^3
Angles (23,13,12)= 9.00000000E+01 9.00000000E+01 9.00000000E+01 degrees
setup1 : take into account q-point for computing boxcut.
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 16 16 16
ecut(hartree)= 2.000 => boxcut(ratio)= 2.01062
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 3 ipert= 2
2) idir= 3 ipert= 4
================================================================================
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Perturbation : displacement of atom 2 along direction 3
The set of symmetries contains only one element for this perturbation.
symkpt : not enough symmetry to change the number of k points.
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 25, nline: 4, wfoptalg: 0, }
tolerances: {tolwfr: 1.00E-15, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 1010.6903354955 5.458E+02 1.232E+00 7.678E+04
ETOT 2 4462.6458532449 3.452E+03 4.244E+00 4.473E+05
ETOT 3 324.40608195777 -4.138E+03 2.216E+00 2.849E+02
ETOT 4 321.56034343667 -2.846E+00 4.079E-03 5.028E+00
ETOT 5 321.52581825341 -3.453E-02 1.341E-04 1.711E-01
ETOT 6 321.52515120848 -6.670E-04 1.391E-06 3.333E-03
ETOT 7 321.52514209867 -9.110E-06 5.176E-09 1.765E-04
ETOT 8 321.52514122926 -8.694E-07 2.935E-09 2.224E-06
ETOT 9 321.52514122334 -5.920E-09 7.201E-11 4.017E-07
ETOT 10 321.52514121998 -3.364E-09 5.370E-12 1.318E-09
ETOT 11 321.52514121997 -4.746E-12 2.726E-15 4.867E-11
ETOT 12 321.52514121997 -6.537E-13 9.459E-16 1.910E-12
At SCF step 12 max residual= 9.46E-16 < tolwfr= 1.00E-15 =>converged.
-open ddk wf file :t05o_DS2_1WF9
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 75.287E-17; max= 94.592E-17
0.0000 0.0000 0.1250 1 7.64604E-16 kpt; spin; max resid(k); each band:
7.65E-16 6.98E-16 6.98E-16 3.77E-16
0.0000 0.0000 0.3750 1 9.45921E-16 kpt; spin; max resid(k); each band:
8.18E-16 9.46E-16 8.60E-16 8.60E-16
Thirteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 1.32366786E+02 eigvalue= 4.23532597E+01 local= -7.53961307E+01
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -2.66620211E+02 Hartree= 6.73651806E+01 xc= -1.62613379E+01
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= -7.02919860E+00 enl1= -2.01769066E+01
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -1.43398558E+02
10,11,12 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 1.31953294E+02 fr.nonlo= 6.35986344E+00 Ewald= 3.26610542E+02
13,14 Frozen wf xc core corrections (1) and (2)
frxc 1 = 0.00000000E+00 frxc 2 = 0.00000000E+00
Resulting in :
2DEtotal= 0.3215251412E+03 Ha. Also 2DEtotal= 0.874914403838E+04 eV
(2DErelax= -1.4339855806E+02 Ha. 2DEnonrelax= 4.6492369928E+02 Ha)
( non-var. 2DEtotal : 3.2152514060E+02 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.000000
Perturbation : homogeneous electric field along direction 3
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
- dfpt_looppert: read the DDK wavefunctions from file: t05o_DS2_1WF9
--- !BeginCycle
iteration_state: {dtset: 3, }
solver: {iscf: 7, nstep: 25, nline: 4, wfoptalg: 0, }
tolerances: {tolwfr: 1.00E-15, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 293.11884452507 2.931E+02 6.766E-01 3.533E+04
ETOT 2 2071.8169083226 1.779E+03 2.192E+00 2.293E+05
ETOT 3 -44.105795207787 -2.116E+03 1.076E+00 5.045E+01
ETOT 4 -44.632404222893 -5.266E-01 1.111E-03 3.474E-01
ETOT 5 -44.634798990013 -2.395E-03 3.642E-05 1.083E-01
ETOT 6 -44.635521879126 -7.229E-04 2.515E-06 1.459E-02
ETOT 7 -44.635651183106 -1.293E-04 1.956E-07 2.387E-04
ETOT 8 -44.635653498284 -2.315E-06 2.202E-09 7.220E-06
ETOT 9 -44.635653558581 -6.030E-08 2.935E-11 5.554E-07
ETOT 10 -44.635653563871 -5.290E-09 4.859E-12 5.524E-09
ETOT 11 -44.635653563924 -5.387E-11 4.759E-14 7.470E-11
ETOT 12 -44.635653563924 1.350E-13 9.581E-16 3.588E-11
At SCF step 12 max residual= 9.58E-16 < tolwfr= 1.00E-15 =>converged.
-open ddk wf file :t05o_DS2_1WF9
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 66.220E-17; max= 95.806E-17
0.0000 0.0000 0.1250 1 9.58065E-16 kpt; spin; max resid(k); each band:
9.58E-16 5.46E-16 5.46E-16 4.89E-16
0.0000 0.0000 0.3750 1 9.35062E-16 kpt; spin; max resid(k); each band:
6.03E-16 9.35E-16 6.10E-16 6.10E-16
Seven components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 8.11960213E+01 eigvalue= 5.98633741E+01 local= -1.07842005E+02
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
dotwf= -8.92713011E+01 Hartree= 2.85960401E+01 xc= -1.03739423E+01
7,8,9: eventually, occupation + non-local contributions
edocc= 0.00000000E+00 enl0= -6.80384103E+00 enl1= 0.00000000E+00
1-9 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= -4.46356536E+01
No Ewald or frozen-wf contrib.: the relaxation energy is the total one
2DEtotal= -0.4463565356E+02 Ha. Also 2DEtotal= -0.121459790297E+04 eV
( non-var. 2DEtotal : -4.4635650570E+01 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
Ewald part of the dynamical matrix
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 0.0000000000 -0.0000000000
2 1 3 2 0.0000000000 0.0000000000
3 1 3 2 -326.6105421205 -0.0000000000
1 2 3 2 -0.0000000000 -0.0000000000
2 2 3 2 -0.0000000000 0.0000000000
3 2 3 2 326.6105421205 -0.0000000000
Frozen wf local part of the dynamical matrix
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 0.0000000000 0.0000000000
2 1 3 2 0.0000000000 0.0000000000
3 1 3 2 0.0000000000 0.0000000000
1 2 3 2 -0.0000000003 0.0000000000
2 2 3 2 0.0000000014 0.0000000000
3 2 3 2 131.9532937144 0.0000000000
Frozen wf non-local part of the dynamical matrix
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 0.0000000000 0.0000000000
2 1 3 2 0.0000000000 0.0000000000
3 1 3 2 0.0000000000 0.0000000000
1 2 3 2 -0.0000000001 0.0000000000
2 2 3 2 0.0000000002 0.0000000000
3 2 3 2 6.3598634414 0.0000000000
Frozen wf xc core (1) part of the dynamical matrix
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 0.0000000000 0.0000000000
2 1 3 2 0.0000000000 0.0000000000
3 1 3 2 0.0000000000 0.0000000000
1 2 3 2 0.0000000000 0.0000000000
2 2 3 2 0.0000000000 0.0000000000
3 2 3 2 0.0000000000 0.0000000000
Frozen wf xc core (2) part of the dynamical matrix
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 0.0000000000 0.0000000000
2 1 3 2 0.0000000000 0.0000000000
3 1 3 2 0.0000000000 0.0000000000
1 2 3 2 0.0000000000 0.0000000000
2 2 3 2 0.0000000000 0.0000000000
3 2 3 2 0.0000000000 0.0000000000
Non-stationary local part of the 2-order matrix
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 -0.0000000001 0.0000000000
1 1 3 4 0.0000000001 -0.0000000000
2 1 3 2 -0.0000000001 0.0000000000
2 1 3 4 0.0000000003 -0.0000000000
3 1 3 2 1.3552145615 0.0000000000
3 1 3 4 -25.6807607563 -0.0000000000
1 2 3 2 0.0000000003 0.0000000000
1 2 3 4 0.0000000004 -0.0000000000
2 2 3 2 -0.0000000013 0.0000000000
2 2 3 4 0.0000000000 -0.0000000000
3 2 3 2 -133.3101053538 0.0000000000
3 2 3 4 -25.6805889552 -0.0000000000
3 4 3 2 0.0000000000 0.0000000000
3 4 3 4 0.0000000000 0.0000000000
Non-stationary non-local part of the 2nd-order matrix
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 0.0000000000 -0.0000000000
1 1 3 4 -0.0000000000 -0.0000000000
2 1 3 2 0.0000000000 -0.0000000000
2 1 3 4 0.0000000001 -0.0000000000
3 1 3 2 3.7283284028 -0.3092623437
3 1 3 4 0.7389019039 0.2372832425
1 2 3 2 0.0000000001 -0.0000000000
1 2 3 4 0.0000000000 0.0000000000
2 2 3 2 -0.0000000002 0.0000000000
2 2 3 4 -0.0000000000 -0.0000000000
3 2 3 2 -10.0884533197 -0.0804119047
3 2 3 4 0.7389128470 -0.2372836989
3 4 3 2 -24.9416798338 5.4827524271
3 4 3 4 -44.6356505703 -0.0002493301
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 -0.0000000001 -0.0000000000
1 1 3 4 0.0000000000 0.0000000000
2 1 3 2 -0.0000000001 0.0000000000
2 1 3 4 0.0000000004 0.0000000000
3 1 3 2 -321.5269991563 -0.0000000000
3 1 3 4 -24.9418588524 0.0000000000
1 2 3 2 -0.0000000001 0.0000000000
1 2 3 4 0.0000000005 0.0000000000
2 2 3 2 0.0000000001 0.0000000000
2 2 3 4 -0.0000000000 0.0000000000
3 2 1 1 -0.0000000001 0.0000000000
3 2 2 1 -0.0000000001 -0.0000000000
3 2 3 1 -321.5269991563 0.0000000000
3 2 1 2 -0.0000000001 0.0000000000
3 2 2 2 0.0000000001 0.0000000000
3 2 3 2 321.5251406029 0.0000000000
3 2 3 4 -24.9416761082 0.0000000000
3 4 1 1 0.0000000000 0.0000000000
3 4 2 1 0.0000000004 0.0000000000
3 4 3 1 -24.9418588524 0.0000000000
3 4 1 2 0.0000000005 0.0000000000
3 4 2 2 -0.0000000000 0.0000000000
3 4 3 2 -24.9416798338 0.0000000000
3 4 3 4 -44.6356505703 0.0000000000
Dynamical matrix, in cartesian coordinates,
if specified in the inputs, asr has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 2 -0.0000000000 -0.0000000000
2 1 3 2 -0.0000000000 0.0000000000
3 1 3 2 -2.0577727946 -0.0000000000
1 2 3 2 -0.0000000000 0.0000000000
2 2 3 2 0.0000000000 0.0000000000
3 2 1 1 -0.0000000000 0.0000000000
3 2 2 1 -0.0000000000 -0.0000000000
3 2 3 1 -2.0577727946 0.0000000000
3 2 1 2 -0.0000000000 0.0000000000
3 2 2 2 0.0000000000 0.0000000000
3 2 3 2 2.0577608999 0.0000000000
Dielectric tensor, in cartesian coordinates,
j1 j2 matrix element
dir pert dir pert real part imaginary part
3 4 3 4 2.7759961066 -0.0000000000
Effective charges, in cartesian coordinates,
(from electric field response)
if specified in the inputs, charge neutrality has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 3 4 0.0000000000 0.0000000000
2 1 3 4 0.0000000001 0.0000000000
3 1 3 4 0.0303798737 0.0000000000
1 2 3 4 0.0000000001 0.0000000000
2 2 3 4 -0.0000000000 0.0000000000
3 2 3 4 0.0304089584 0.0000000000
Effective charges, in cartesian coordinates,
(from phonon response)
if specified in the inputs, charge neutrality has been imposed
j1 j2 matrix element
dir pert dir pert real part imaginary part
3 4 1 1 0.0000000000 0.0000000000
3 4 2 1 0.0000000001 0.0000000000
3 4 3 1 0.0303798737 0.0000000000
3 4 1 2 0.0000000001 0.0000000000
3 4 2 2 -0.0000000000 0.0000000000
3 4 3 2 0.0304083654 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
3.359831E-02
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00
- 7.373976E+03
chkph3 : WARNING -
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
Phonon at Gamma, with non-analyticity in the
direction (cartesian coordinates) 0.00000 0.00000 1.00000
Phonon energies in Hartree :
0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00
3.359834E-02
Phonon frequencies in cm-1 :
- 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00
- 7.373982E+03
chkph3 : WARNING -
Dynamical matrix incomplete, phonon frequencies may be wrong, see the log file for more explanations.
== END DATASET(S) ==============================================================
================================================================================
-outvars: echo values of variables after computation --------
acell 1.0000000000E+01 1.0000000000E+01 1.2500000000E+01 Bohr
amu 1.00000000E+00
asr 0
chneut 0
diecut 1.20000000E+00 Hartree
diegap 2.00000000E-01 Hartree
diemac1 1.00000000E+06
diemac2 1.00000000E+06
diemac3 1.00000000E+00
diemix1 1.00000000E+00
diemix2 1.00000000E+00
diemix3 7.00000000E-01
ecut 2.00000000E+00 Hartree
etotal1 -6.6499924738E+00
etotal2 -1.8548649909E+00
etotal3 -4.4635653564E+01
fcart1 -1.7769132557E-13 -1.6272207945E-13 -1.3944227395E+00
1.7769132557E-13 1.6272207945E-13 1.3944227395E+00
fcart2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
fcart3 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
- fftalg 512
getddk1 0
getddk2 2
getddk3 2
getwfk1 0
getwfk2 1
getwfk3 1
iprcel 45
ixc 3
jdtset 1 2 3
kpt 0.00000000E+00 0.00000000E+00 1.25000000E-01
0.00000000E+00 0.00000000E+00 3.75000000E-01
kptopt 0
P mkmem 2
P mkqmem 2
P mk1mem 2
natom 2
nband 4
ndtset 3
ngfft 16 16 16
nkpt 2
nqpt1 0
nqpt2 1
nqpt3 1
nstep1 30
nstep2 30
nstep3 25
nsym 1
ntypat 1
occ 2.000000 2.000000 2.000000 2.000000
optdriver1 0
optdriver2 1
optdriver3 1
prtpot1 0
prtpot2 1
prtpot3 1
prtvol1 0
prtvol2 10
prtvol3 10
rfatpol1 1 2
rfatpol2 2 2
rfatpol3 2 2
rfdir1 1 1 1
rfdir2 0 0 1
rfdir3 0 0 1
rfelfd1 0
rfelfd2 2
rfelfd3 3
rfphon1 0
rfphon2 0
rfphon3 1
spgroup 1
strten1 3.1298627926E-04 3.1298627924E-04 -2.5255636492E-03
0.0000000000E+00 -1.7731574900E-15 3.5819845878E-15
strten2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
strten3 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
tolwfr1 1.00000000E-22
tolwfr2 1.00000000E-22
tolwfr3 1.00000000E-15
typat 1 1
wtk 0.50000 0.50000
xangst 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 1.3229430215E+00
xcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 2.5000000000E+00
xred 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 2.0000000000E-01
znucl 14.00000
================================================================================
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] Preconditioning of self-consistent-field cycles in density functional theory: the extrapolar method
- P.-M. Anglade, X. Gonze, Phys. Rev. B 78, 045126 (2008).
- Comment: to be cited in case the extrapolar conditioner is used, i.e. non-vanishing iprcel.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#anglade2008
-
- [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] 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
-
- [4] Dynamical matrices, Born effective charges, dielectric permittivity tensors, and ,
- interatomic force constants from density-functional perturbation theory,
- X. Gonze and C. Lee, Phys. Rev. B55, 10355 (1997).
- Comment: Non-vanishing rfphon and/or rfelfd, in the norm-conserving case.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#gonze1997a
-
- [5] 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
-
- [6] 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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