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.Version 9.11.2 of ABINIT
.(MPI version, prepared for a x86_64_linux_gnu9.3 computer)
.Copyright (C) 1998-2022 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 : Sat 15 Jul 2023.
- ( at 12h10 )
- input file -> /home/marc/work/abinit/abinit-git/tests/Test_suite/gpu_omp_t06-t07-t24/t24.abi
- output file -> t24.abo
- root for input files -> t24i
- root for output files -> t24o
DATASET 2 : space group Im -3 m (#229); Bravais cI (body-center cubic)
================================================================================
Values of the parameters that define the memory need for DATASET 2 (RF).
intxc = 0 iscf = 7 lmnmax = 18 lnmax = 6
mgfft = 15 mpssoang = 3 mqgrid = 3001 natom = 1
nloc_mem = 2 nspden = 2 nspinor = 1 nsppol = 2
nsym = 48 n1xccc = 1 ntypat = 1 occopt = 7
xclevel = 2
- mband = 12 mffmem = 1 mkmem = 64
- mkqmem = 64 mk1mem = 64 mpw = 92
nfft = 3375 nkpt = 64
================================================================================
P This job should need less than 10.167 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
_ WF disk file : 2.158 Mbytes ; DEN or POT disk file : 0.053 Mbytes.
================================================================================
--------------------------------------------------------------------------------
------------- Echo of variables that govern the present computation ------------
--------------------------------------------------------------------------------
-
- outvars: echo of selected default values
- iomode0 = 0 , fftalg0 =312 , wfoptalg0 = 10
-
- outvars: echo of global parameters not present in the input file
- max_nthreads = 0
-
-outvars: echo values of preprocessed input variables --------
acell 4.8000000000E+00 4.8000000000E+00 4.8000000000E+00 Bohr
amu 5.58470000E+01
bandpp 6
ecut 1.00000000E+01 Hartree
- fftalg 312
getwfk 1
- gpu_option 2
-invovl_blksliced 0
iscf 7
ixc 11
jdtset 2
kpt 1.25000000E-01 1.25000000E-01 1.25000000E-01
3.75000000E-01 1.25000000E-01 1.25000000E-01
-3.75000000E-01 1.25000000E-01 1.25000000E-01
-1.25000000E-01 1.25000000E-01 1.25000000E-01
1.25000000E-01 3.75000000E-01 1.25000000E-01
3.75000000E-01 3.75000000E-01 1.25000000E-01
-3.75000000E-01 3.75000000E-01 1.25000000E-01
-1.25000000E-01 3.75000000E-01 1.25000000E-01
1.25000000E-01 -3.75000000E-01 1.25000000E-01
3.75000000E-01 -3.75000000E-01 1.25000000E-01
-3.75000000E-01 -3.75000000E-01 1.25000000E-01
-1.25000000E-01 -3.75000000E-01 1.25000000E-01
1.25000000E-01 -1.25000000E-01 1.25000000E-01
3.75000000E-01 -1.25000000E-01 1.25000000E-01
-3.75000000E-01 -1.25000000E-01 1.25000000E-01
-1.25000000E-01 -1.25000000E-01 1.25000000E-01
1.25000000E-01 1.25000000E-01 3.75000000E-01
3.75000000E-01 1.25000000E-01 3.75000000E-01
-3.75000000E-01 1.25000000E-01 3.75000000E-01
-1.25000000E-01 1.25000000E-01 3.75000000E-01
1.25000000E-01 3.75000000E-01 3.75000000E-01
3.75000000E-01 3.75000000E-01 3.75000000E-01
-3.75000000E-01 3.75000000E-01 3.75000000E-01
-1.25000000E-01 3.75000000E-01 3.75000000E-01
1.25000000E-01 -3.75000000E-01 3.75000000E-01
3.75000000E-01 -3.75000000E-01 3.75000000E-01
-3.75000000E-01 -3.75000000E-01 3.75000000E-01
-1.25000000E-01 -3.75000000E-01 3.75000000E-01
1.25000000E-01 -1.25000000E-01 3.75000000E-01
3.75000000E-01 -1.25000000E-01 3.75000000E-01
-3.75000000E-01 -1.25000000E-01 3.75000000E-01
-1.25000000E-01 -1.25000000E-01 3.75000000E-01
1.25000000E-01 1.25000000E-01 -3.75000000E-01
3.75000000E-01 1.25000000E-01 -3.75000000E-01
-3.75000000E-01 1.25000000E-01 -3.75000000E-01
-1.25000000E-01 1.25000000E-01 -3.75000000E-01
1.25000000E-01 3.75000000E-01 -3.75000000E-01
3.75000000E-01 3.75000000E-01 -3.75000000E-01
-3.75000000E-01 3.75000000E-01 -3.75000000E-01
-1.25000000E-01 3.75000000E-01 -3.75000000E-01
1.25000000E-01 -3.75000000E-01 -3.75000000E-01
3.75000000E-01 -3.75000000E-01 -3.75000000E-01
-3.75000000E-01 -3.75000000E-01 -3.75000000E-01
-1.25000000E-01 -3.75000000E-01 -3.75000000E-01
1.25000000E-01 -1.25000000E-01 -3.75000000E-01
3.75000000E-01 -1.25000000E-01 -3.75000000E-01
-3.75000000E-01 -1.25000000E-01 -3.75000000E-01
-1.25000000E-01 -1.25000000E-01 -3.75000000E-01
1.25000000E-01 1.25000000E-01 -1.25000000E-01
3.75000000E-01 1.25000000E-01 -1.25000000E-01
outvar_i_n : Printing only first 50 k-points.
kptopt 3
kptrlatt 4 0 0 0 4 0 0 0 4
kptrlen 1.66276878E+01
P mkmem 64
P mkqmem 64
P mk1mem 64
natom 1
nband 12
nbdbuf 2
ndtset 1
ngfft 15 15 15
ngfftdg 18 18 18
nkpt 64
nline 6
nqpt 1
nspden 2
nsppol 2
nstep 3
nsym 48
ntypat 1
occ 1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
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1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
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1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
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1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
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1.000000 1.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.000000 0.000000 0.000000 0.000000
prtocc : prtvol=0, do not print more k-points.
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
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1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.000000 0.000000 0.000000 0.000000
prtocc : prtvol=0, do not print more k-points.
occopt 7
optdriver 1
pawecutdg 2.00000000E+01 Hartree
pawnphi 8
pawntheta 5
pawxcdev 0
prtpot 1
qpt 0.00000000E+00 0.00000000E+00 5.00000000E-01
rfphon 1
rprim -5.0000000000E-01 5.0000000000E-01 5.0000000000E-01
5.0000000000E-01 -5.0000000000E-01 5.0000000000E-01
5.0000000000E-01 5.0000000000E-01 -5.0000000000E-01
shiftk 5.00000000E-01 5.00000000E-01 5.00000000E-01
spgroup 229
spinat 0.0000000000E+00 0.0000000000E+00 4.0000000000E+00
symrel 1 0 0 0 1 0 0 0 1 -1 0 0 0 -1 0 0 0 -1
-1 -1 -1 0 0 1 0 1 0 1 1 1 0 0 -1 0 -1 0
0 1 0 1 0 0 -1 -1 -1 0 -1 0 -1 0 0 1 1 1
0 0 1 -1 -1 -1 1 0 0 0 0 -1 1 1 1 -1 0 0
0 1 0 1 0 0 0 0 1 0 -1 0 -1 0 0 0 0 -1
-1 -1 -1 0 0 1 1 0 0 1 1 1 0 0 -1 -1 0 0
1 0 0 0 1 0 -1 -1 -1 -1 0 0 0 -1 0 1 1 1
0 0 1 -1 -1 -1 0 1 0 0 0 -1 1 1 1 0 -1 0
-1 -1 -1 1 0 0 0 0 1 1 1 1 -1 0 0 0 0 -1
0 1 0 0 0 1 1 0 0 0 -1 0 0 0 -1 -1 0 0
1 0 0 -1 -1 -1 0 1 0 -1 0 0 1 1 1 0 -1 0
0 0 1 0 1 0 -1 -1 -1 0 0 -1 0 -1 0 1 1 1
1 0 0 -1 -1 -1 0 0 1 -1 0 0 1 1 1 0 0 -1
0 1 0 0 0 1 -1 -1 -1 0 -1 0 0 0 -1 1 1 1
-1 -1 -1 1 0 0 0 1 0 1 1 1 -1 0 0 0 -1 0
0 0 1 0 1 0 1 0 0 0 0 -1 0 -1 0 -1 0 0
0 1 0 -1 -1 -1 0 0 1 0 -1 0 1 1 1 0 0 -1
1 0 0 0 0 1 -1 -1 -1 -1 0 0 0 0 -1 1 1 1
-1 -1 -1 0 1 0 1 0 0 1 1 1 0 -1 0 -1 0 0
0 0 1 1 0 0 0 1 0 0 0 -1 -1 0 0 0 -1 0
-1 -1 -1 0 1 0 0 0 1 1 1 1 0 -1 0 0 0 -1
1 0 0 0 0 1 0 1 0 -1 0 0 0 0 -1 0 -1 0
0 1 0 -1 -1 -1 1 0 0 0 -1 0 1 1 1 -1 0 0
0 0 1 1 0 0 -1 -1 -1 0 0 -1 -1 0 0 1 1 1
tolrde 1.00000000E-03
tolwfr 1.00000000E-12
typat 1
- useylm 1
wtk 0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563
outvars : Printing only first 50 k-points.
znucl 26.00000
================================================================================
chkinp: Checking input parameters for consistency, jdtset= 2.
================================================================================
== DATASET 2 ==================================================================
- mpi_nproc: 1, omp_nthreads: -1 (-1 if OMP is not activated)
--- !DatasetInfo
iteration_state: {dtset: 2, }
dimensions: {natom: 1, nkpt: 64, mband: 12, nsppol: 2, nspinor: 1, nspden: 2, mpw: 92, }
cutoff_energies: {ecut: 10.0, pawecutdg: 20.0, }
electrons: {nelect: 1.60000000E+01, charge: 0.00000000E+00, occopt: 7.00000000E+00, tsmear: 1.00000000E-02, }
meta: {optdriver: 1, rfphon: 1, }
...
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
Exchange-correlation functional for the present dataset will be:
GGA: Perdew-Burke-Ernzerhof functional - ixc=11
Citation for XC functional:
J.P.Perdew, K.Burke, M.Ernzerhof, PRL 77, 3865 (1996)
Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
R(1)= -2.4000000 2.4000000 2.4000000 G(1)= 0.0000000 0.2083333 0.2083333
R(2)= 2.4000000 -2.4000000 2.4000000 G(2)= 0.2083333 0.0000000 0.2083333
R(3)= 2.4000000 2.4000000 -2.4000000 G(3)= 0.2083333 0.2083333 0.0000000
Unit cell volume ucvol= 5.5296000E+01 bohr^3
Angles (23,13,12)= 1.09471221E+02 1.09471221E+02 1.09471221E+02 degrees
setup1 : take into account q-point for computing boxcut.
Coarse grid specifications (used for wave-functions):
getcut: wavevector= 0.0000 0.0000 0.5000 ngfft= 15 15 15
ecut(hartree)= 10.000 => boxcut(ratio)= 2.20013
getcut : COMMENT -
Note that boxcut > 2.2 ; recall that boxcut=Gcut(box)/Gcut(sphere) = 2
is sufficient for exact treatment of convolution.
Such a large boxcut is a waste : you could raise ecut
e.g. ecut= 12.101403 Hartrees makes boxcut=2
Fine grid specifications (used for densities):
getcut: wavevector= 0.0000 0.0000 0.5000 ngfft= 18 18 18
ecut(hartree)= 20.000 => boxcut(ratio)= 2.03316
--- Pseudopotential description ------------------------------------------------
- pspini: atom type 1 psp file is /home/marc/work/abinit/abinit-git/tests/Pspdir/26fe.paw
- pspatm: opening atomic psp file /home/marc/work/abinit/abinit-git/tests/Pspdir/26fe.paw
- iron - PAW data extracted from US-psp (D.Vanderbilt) - generated by USpp2Abinit v2.2.1
- 26.00000 16.00000 20070813 znucl, zion, pspdat
7 11 2 0 594 0.00000 pspcod,pspxc,lmax,lloc,mmax,r2well
Pseudopotential format is: paw3
basis_size (lnmax)= 6 (lmn_size= 18), orbitals= 0 0 1 1 2 2
Spheres core radius: rc_sph= 2.02984247
3 radial meshes are used:
- mesh 1: r(i)=AA*[exp(BB*(i-1))-1], size= 594 , AA= 0.95337E-04 BB= 0.16949E-01
- mesh 2: r(i)=AA*[exp(BB*(i-1))-1], size= 590 , AA= 0.95337E-04 BB= 0.16949E-01
- mesh 3: r(i)=AA*[exp(BB*(i-1))-1], size= 683 , AA= 0.95337E-04 BB= 0.16949E-01
Shapefunction is BESSEL type: shapef(r,l)=aa(1,l)*jl(q(1,l)*r)+aa(2,l)*jl(q(2,l)*r)
Radius for shape functions = sphere core radius
Radial grid used for partial waves is grid 1
Radial grid used for projectors is grid 2
Radial grid used for (t)core density is grid 1
Radial grid used for Vloc is grid 3
Compensation charge density is taken into account in XC energy/potential
pspatm: atomic psp has been read and splines computed
5.80402498E+02 ecore*ucvol(ha*bohr**3)
--------------------------------------------------------------------------------
==> initialize data related to q vector <==
The list of irreducible perturbations for this q vector is:
1) idir= 1 ipert= 1
2) idir= 3 ipert= 1
================================================================================
The perturbation idir= 2 ipert= 1 is
symmetric of a previously calculated perturbation.
So, its SCF calculation is not needed.
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.500000
Perturbation : displacement of atom 1 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.
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.600000E+01 and 1.600000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 2, }
solver: {iscf: 7, nstep: 3, nline: 6, wfoptalg: 10, }
tolerances: {tolwfr: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 289.50892186824 7.136E+02 2.866E-01 8.223E+05
ETOT 2 20.335412316667 -2.692E+02 3.064E-02 6.520E+04
ETOT 3 18.492305945759 -1.843E+00 7.798E-03 3.514E+04
scprqt: WARNING -
nstep= 3 was not enough SCF cycles to converge;
maximum residual= 7.798E-03 exceeds tolwfr= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 10.725E-04; max= 77.982E-04
Fourteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.20940897E+02 eigvalue= 2.46170249E+01 local= -4.72284632E+01
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -3.48127596E+02 Hartree= 8.60266512E+02 xc= -1.30162566E+02
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 1.48728414E+02 enl0= -7.67463431E+00 enl1= -2.81938145E+02
10: eventually, PAW "on-site" Hxc contribution: epaw1= 3.19204353E+00
1-10 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= 4.42613488E+02
11,12,13 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 1.01437000E+03 fr.nonlo= -1.49038180E+03 Ewald= 5.18906191E+01
14,15 Frozen wf xc core corrections (1) and (2)
frxc 1 = 0.00000000E+00 frxc 2 = 0.00000000E+00
16 Contribution from 1st-order change of wavefunctions overlap
eovl1 = 7.32597485E+02
Resulting in :
2DEtotal= 0.1849230595E+02 Ha. Also 2DEtotal= 0.503201235547E+03 eV
(2DErelax= 4.4261348809E+02 Ha. 2DEnonrelax= -4.2412118214E+02 Ha)
( non-var. 2DEtotal : -6.5565675555E+00 Ha)
--------------------------------------------------------------------------------
Perturbation wavevector (in red.coord.) 0.000000 0.000000 0.500000
Perturbation : displacement of atom 1 along direction 3
Found 2 symmetries that leave the perturbation invariant.
symkpt : the number of k-points, thanks to the symmetries,
is reduced to 40 .
--------------------------------------------------------------------------------
--------------------------------------------------------------------------------
dfpt_looppert : total number of electrons, from k and k+q
fully or partially occupied states are 1.600000E+01 and 1.600000E+01.
Initialisation of the first-order wave-functions :
ireadwf= 0
--- !BeginCycle
iteration_state: {dtset: 2, }
solver: {iscf: 7, nstep: 3, nline: 6, wfoptalg: 10, }
tolerances: {tolwfr: 1.00E-12, }
...
iter 2DEtotal(Ha) deltaE(Ha) residm vres2
-ETOT 1 3213.8895400691 3.727E+03 8.382E-01 1.417E+07
ETOT 2 64.046791075685 -3.150E+03 3.191E-01 2.454E+05
ETOT 3 18.570337790615 -4.548E+01 9.028E-03 2.345E+04
scprqt: WARNING -
nstep= 3 was not enough SCF cycles to converge;
maximum residual= 9.028E-03 exceeds tolwfr= 1.000E-12
================================================================================
----iterations are completed or convergence reached----
Mean square residual over all n,k,spin= 14.622E-04; max= 90.279E-04
Fourteen components of 2nd-order total energy (hartree) are
1,2,3: 0th-order hamiltonian combined with 1st-order wavefunctions
kin0= 2.43055460E+02 eigvalue= 2.09299320E+01 local= -5.21645500E+01
4,5,6: 1st-order hamiltonian combined with 1st and 0th-order wfs
loc psp = -7.87419558E+02 Hartree= 1.38879151E+03 xc= -1.38408663E+02
note that "loc psp" includes a xc core correction that could be resolved
7,8,9: eventually, occupation + non-local contributions
edocc= 1.55710200E+02 enl0= -5.29772995E+00 enl1= -2.95508214E+02
10: eventually, PAW "on-site" Hxc contribution: epaw1= 1.93703586E+00
1-10 gives the relaxation energy (to be shifted if some occ is /=2.0)
erelax= 5.31625425E+02
11,12,13 Non-relaxation contributions : frozen-wavefunctions and Ewald
fr.local= 1.01437000E+03 fr.nonlo= -2.14574090E+03 Ewald= 6.18315814E+02
14,15 Frozen wf xc core corrections (1) and (2)
frxc 1 = 0.00000000E+00 frxc 2 = 0.00000000E+00
16 Contribution from 1st-order change of wavefunctions overlap
eovl1 = 1.05053394E+03
Resulting in :
2DEtotal= 0.1857033779E+02 Ha. Also 2DEtotal= 0.505324590030E+03 eV
(2DErelax= 5.3162542534E+02 Ha. 2DEnonrelax= -5.1305508755E+02 Ha)
( non-var. 2DEtotal : -3.9850367561E+00 Ha)
================================================================================
---- first-order wavefunction calculations are completed ----
==> Compute Derivative Database <==
2nd-order matrix (non-cartesian coordinates, masses not included,
asr not included )
j1 j2 matrix element
dir pert dir pert real part imaginary part
1 1 1 1 -6.5565675555 0.0000000000
1 1 2 1 6.3673537405 0.0000000000
1 1 3 1 0.0946069075 0.0000000000
2 1 1 1 6.3673537405 0.0000000000
2 1 2 1 -6.5565675555 0.0000000000
2 1 3 1 0.0946069075 0.0000000000
3 1 1 1 0.0946069075 -0.0000000000
3 1 2 1 0.0946069075 0.0000000000
3 1 3 1 12.7832256584 0.0013528360
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 0.2784666631 0.0000587168
1 1 2 1 0.8394007471 0.0000587168
1 1 3 1 0.0000000000 -0.0000000000
2 1 1 1 0.8394007471 0.0000587168
2 1 2 1 0.2784666631 0.0000587168
2 1 3 1 0.0000000000 -0.0000000000
3 1 1 1 0.0000000000 0.0000000000
3 1 2 1 0.0000000000 0.0000000000
3 1 3 1 -0.0164248103 0.0000000000
Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.50000
Phonon energies in Hartree :
-2.347340E-03 -4.016707E-04 3.313715E-03
Phonon frequencies in cm-1 :
- -5.151815E+02 -8.815654E+01 7.272764E+02
== END DATASET(S) ==============================================================
================================================================================
-outvars: echo values of variables after computation --------
acell 4.8000000000E+00 4.8000000000E+00 4.8000000000E+00 Bohr
amu 5.58470000E+01
bandpp 6
ecut 1.00000000E+01 Hartree
etotal2 1.8570337791E+01
fcart2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
- fftalg 312
getwfk 1
- gpu_option 2
-invovl_blksliced 0
iscf 7
ixc 11
jdtset 2
kpt 1.25000000E-01 1.25000000E-01 1.25000000E-01
3.75000000E-01 1.25000000E-01 1.25000000E-01
-3.75000000E-01 1.25000000E-01 1.25000000E-01
-1.25000000E-01 1.25000000E-01 1.25000000E-01
1.25000000E-01 3.75000000E-01 1.25000000E-01
3.75000000E-01 3.75000000E-01 1.25000000E-01
-3.75000000E-01 3.75000000E-01 1.25000000E-01
-1.25000000E-01 3.75000000E-01 1.25000000E-01
1.25000000E-01 -3.75000000E-01 1.25000000E-01
3.75000000E-01 -3.75000000E-01 1.25000000E-01
-3.75000000E-01 -3.75000000E-01 1.25000000E-01
-1.25000000E-01 -3.75000000E-01 1.25000000E-01
1.25000000E-01 -1.25000000E-01 1.25000000E-01
3.75000000E-01 -1.25000000E-01 1.25000000E-01
-3.75000000E-01 -1.25000000E-01 1.25000000E-01
-1.25000000E-01 -1.25000000E-01 1.25000000E-01
1.25000000E-01 1.25000000E-01 3.75000000E-01
3.75000000E-01 1.25000000E-01 3.75000000E-01
-3.75000000E-01 1.25000000E-01 3.75000000E-01
-1.25000000E-01 1.25000000E-01 3.75000000E-01
1.25000000E-01 3.75000000E-01 3.75000000E-01
3.75000000E-01 3.75000000E-01 3.75000000E-01
-3.75000000E-01 3.75000000E-01 3.75000000E-01
-1.25000000E-01 3.75000000E-01 3.75000000E-01
1.25000000E-01 -3.75000000E-01 3.75000000E-01
3.75000000E-01 -3.75000000E-01 3.75000000E-01
-3.75000000E-01 -3.75000000E-01 3.75000000E-01
-1.25000000E-01 -3.75000000E-01 3.75000000E-01
1.25000000E-01 -1.25000000E-01 3.75000000E-01
3.75000000E-01 -1.25000000E-01 3.75000000E-01
-3.75000000E-01 -1.25000000E-01 3.75000000E-01
-1.25000000E-01 -1.25000000E-01 3.75000000E-01
1.25000000E-01 1.25000000E-01 -3.75000000E-01
3.75000000E-01 1.25000000E-01 -3.75000000E-01
-3.75000000E-01 1.25000000E-01 -3.75000000E-01
-1.25000000E-01 1.25000000E-01 -3.75000000E-01
1.25000000E-01 3.75000000E-01 -3.75000000E-01
3.75000000E-01 3.75000000E-01 -3.75000000E-01
-3.75000000E-01 3.75000000E-01 -3.75000000E-01
-1.25000000E-01 3.75000000E-01 -3.75000000E-01
1.25000000E-01 -3.75000000E-01 -3.75000000E-01
3.75000000E-01 -3.75000000E-01 -3.75000000E-01
-3.75000000E-01 -3.75000000E-01 -3.75000000E-01
-1.25000000E-01 -3.75000000E-01 -3.75000000E-01
1.25000000E-01 -1.25000000E-01 -3.75000000E-01
3.75000000E-01 -1.25000000E-01 -3.75000000E-01
-3.75000000E-01 -1.25000000E-01 -3.75000000E-01
-1.25000000E-01 -1.25000000E-01 -3.75000000E-01
1.25000000E-01 1.25000000E-01 -1.25000000E-01
3.75000000E-01 1.25000000E-01 -1.25000000E-01
outvar_i_n : Printing only first 50 k-points.
kptopt 3
kptrlatt 4 0 0 0 4 0 0 0 4
kptrlen 1.66276878E+01
P mkmem 64
P mkqmem 64
P mk1mem 64
natom 1
nband 12
nbdbuf 2
ndtset 1
ngfft 15 15 15
ngfftdg 18 18 18
nkpt 64
nline 6
nqpt 1
nspden 2
nsppol 2
nstep 3
nsym 48
ntypat 1
occ 1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.000356 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.000356 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.999528 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
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1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
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1.000000 1.000000 1.000000 0.999528 0.000000 0.000000
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1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.999528 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.941748 0.941748 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.999753 0.999753 0.198925 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.941748 0.941748 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.999753 0.999753 0.198925 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.999753 0.999753 0.198925 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.941748 0.941748 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.000356 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.000356 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.941748 0.941748 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.999753 0.999753 0.198925 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.999753 0.999753 0.198925 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.941748 0.941748 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.999753 0.999753 0.198925 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.941748 0.941748 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.999528 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
prtocc : prtvol=0, do not print more k-points.
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.999528 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.941748 0.941748 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.000356 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.019421 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.999528 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.000356 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.999947 0.999186 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 1.000000 0.000356 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000128 0.000128 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000001 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000128 0.000128 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.990609 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000001 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000001 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000128 0.000128 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.990609 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 1.000000 0.990609 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000001 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000001 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000001 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.013122 0.013122 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.013122 0.013122 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
0.013122 0.013122 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000128 0.000128 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000128 0.000128 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.000000 0.000000 0.000000 0.000000 0.000000
1.000000 1.000000 1.000000 1.000000 1.000000 1.000000
1.000000 0.715940 0.000000 0.000000 0.000000 0.000000
prtocc : prtvol=0, do not print more k-points.
occopt 7
optdriver 1
pawecutdg 2.00000000E+01 Hartree
pawnphi 8
pawntheta 5
pawxcdev 0
prtpot 1
qpt 0.00000000E+00 0.00000000E+00 5.00000000E-01
rfphon 1
rprim -5.0000000000E-01 5.0000000000E-01 5.0000000000E-01
5.0000000000E-01 -5.0000000000E-01 5.0000000000E-01
5.0000000000E-01 5.0000000000E-01 -5.0000000000E-01
shiftk 5.00000000E-01 5.00000000E-01 5.00000000E-01
spgroup 229
spinat 0.0000000000E+00 0.0000000000E+00 4.0000000000E+00
strten2 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
symrel 1 0 0 0 1 0 0 0 1 -1 0 0 0 -1 0 0 0 -1
-1 -1 -1 0 0 1 0 1 0 1 1 1 0 0 -1 0 -1 0
0 1 0 1 0 0 -1 -1 -1 0 -1 0 -1 0 0 1 1 1
0 0 1 -1 -1 -1 1 0 0 0 0 -1 1 1 1 -1 0 0
0 1 0 1 0 0 0 0 1 0 -1 0 -1 0 0 0 0 -1
-1 -1 -1 0 0 1 1 0 0 1 1 1 0 0 -1 -1 0 0
1 0 0 0 1 0 -1 -1 -1 -1 0 0 0 -1 0 1 1 1
0 0 1 -1 -1 -1 0 1 0 0 0 -1 1 1 1 0 -1 0
-1 -1 -1 1 0 0 0 0 1 1 1 1 -1 0 0 0 0 -1
0 1 0 0 0 1 1 0 0 0 -1 0 0 0 -1 -1 0 0
1 0 0 -1 -1 -1 0 1 0 -1 0 0 1 1 1 0 -1 0
0 0 1 0 1 0 -1 -1 -1 0 0 -1 0 -1 0 1 1 1
1 0 0 -1 -1 -1 0 0 1 -1 0 0 1 1 1 0 0 -1
0 1 0 0 0 1 -1 -1 -1 0 -1 0 0 0 -1 1 1 1
-1 -1 -1 1 0 0 0 1 0 1 1 1 -1 0 0 0 -1 0
0 0 1 0 1 0 1 0 0 0 0 -1 0 -1 0 -1 0 0
0 1 0 -1 -1 -1 0 0 1 0 -1 0 1 1 1 0 0 -1
1 0 0 0 0 1 -1 -1 -1 -1 0 0 0 0 -1 1 1 1
-1 -1 -1 0 1 0 1 0 0 1 1 1 0 -1 0 -1 0 0
0 0 1 1 0 0 0 1 0 0 0 -1 -1 0 0 0 -1 0
-1 -1 -1 0 1 0 0 0 1 1 1 1 0 -1 0 0 0 -1
1 0 0 0 0 1 0 1 0 -1 0 0 0 0 -1 0 -1 0
0 1 0 -1 -1 -1 1 0 0 0 -1 0 1 1 1 -1 0 0
0 0 1 1 0 0 -1 -1 -1 0 0 -1 -1 0 0 1 1 1
tolrde 1.00000000E-03
tolwfr 1.00000000E-12
typat 1
- useylm 1
wtk 0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563 0.01563 0.01563 0.01563 0.01563
0.01563 0.01563
outvars : Printing only first 50 k-points.
znucl 26.00000
================================================================================
- 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] Projector augmented-wave approach to density-functional perturbation theory.
- C. Audouze, F. Jollet, M. Torrent and X. Gonze, Phys. Rev. B 73, 235101 (2006).
- Comparison between projector augmented-wave and ultrasoft pseudopotential formalisms
- at the density-functional perturbation theory level.
- C. Audouze, F. Jollet, M. Torrent and X. Gonze, Phys. Rev. B 78, 035105 (2008).
- Comment: to be cited in case the computation of response function with PAW, i.e. (rfphon=1 or rfelfd=1) and usepaw=1.
- Strong suggestion to cite these papers.
- DOI and bibtex: see https://docs.abinit.org/theory/bibliography/#audouze2006,
- and https://docs.abinit.org/theory/bibliography/#audouze2008
-
- [2] 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
-
- [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 ,
- 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
-
- [6] 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
-
- [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
-
- Proc. 0 individual time (sec): cpu= 19.9 wall= 20.0
================================================================================
Calculation completed.
.Delivered 7 WARNINGs and 4 COMMENTs to log file.
+Overall time at end (sec) : cpu= 19.9 wall= 20.0
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